CN111708322A - Three-coordinate positioner posture adjusting operation and control method and system, posture adjusting controller and storage medium - Google Patents

Three-coordinate positioner posture adjusting operation and control method and system, posture adjusting controller and storage medium Download PDF

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CN111708322A
CN111708322A CN202010534922.6A CN202010534922A CN111708322A CN 111708322 A CN111708322 A CN 111708322A CN 202010534922 A CN202010534922 A CN 202010534922A CN 111708322 A CN111708322 A CN 111708322A
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rigid body
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acceleration
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CN111708322B (en
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鄢继红
周玉龙
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Guangzhou Numerical Control Equipment Co Ltd
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    • GPHYSICS
    • G05CONTROLLING; REGULATING
    • G05BCONTROL OR REGULATING SYSTEMS IN GENERAL; FUNCTIONAL ELEMENTS OF SUCH SYSTEMS; MONITORING OR TESTING ARRANGEMENTS FOR SUCH SYSTEMS OR ELEMENTS
    • G05B19/00Programme-control systems
    • G05B19/02Programme-control systems electric
    • G05B19/18Numerical control [NC], i.e. automatically operating machines, in particular machine tools, e.g. in a manufacturing environment, so as to execute positioning, movement or co-ordinated operations by means of programme data in numerical form
    • G05B19/404Numerical control [NC], i.e. automatically operating machines, in particular machine tools, e.g. in a manufacturing environment, so as to execute positioning, movement or co-ordinated operations by means of programme data in numerical form characterised by control arrangements for compensation, e.g. for backlash, overshoot, tool offset, tool wear, temperature, machine construction errors, load, inertia
    • GPHYSICS
    • G05CONTROLLING; REGULATING
    • G05BCONTROL OR REGULATING SYSTEMS IN GENERAL; FUNCTIONAL ELEMENTS OF SUCH SYSTEMS; MONITORING OR TESTING ARRANGEMENTS FOR SUCH SYSTEMS OR ELEMENTS
    • G05B2219/00Program-control systems
    • G05B2219/30Nc systems
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    • G05B2219/32063Adapt speed of tool as function of deviation from target rate of workpieces

Abstract

The invention discloses a three-coordinate positioner posture adjusting operation and control method, a three-coordinate positioner posture adjusting operation and control system, a posture adjusting controller and a storage medium, wherein the method comprises the following steps: resolving the translational movement amount and translational direction vector of the rigid body, and the rotation angle and rotation axis vector of the rigid body fixed axis rotation; resolving the circle center and radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, and resolving a circular arc angular velocity range and a rigid body angular velocity range; planning and finishing the rigid body composite motion speed; adjusting the speed and the acceleration of the rigid body composite motion according to the speed range and the acceleration range allowed by each positioner driving shaft, and planning and finishing the rigid body composite motion speed again; carrying out interpolation calculation according to a time division method, and outputting a three-axis instruction coordinate position of each locator; and carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each positioner, and outputting the actual position of each axis driver. The invention can meet the acceleration requirement, has redundant driving shafts, and has stable and impact-free posture adjusting process.

Description

Three-coordinate positioner posture adjusting operation and control method and system, posture adjusting controller and storage medium
Technical Field
The invention relates to a three-coordinate positioner posture adjusting operation and control method, a three-coordinate positioner posture adjusting operation and control system, a posture adjusting controller and a storage medium, and belongs to the research field of airplane digital assembly.
Background
Aircraft assembly is one of the most important and complex links in aircraft manufacturing. The problem of spatial positioning of aircraft parts or assemblies is a common key problem in aircraft assembly, and the positioning accuracy directly influences the aerodynamic appearance, fatigue life, reliability and the like of aircraft products. In order to improve the quality and efficiency of the attitude adjustment of the aircraft components, the advanced attitude adjustment technology is developing towards digitization, automation and flexibility.
The automatic attitude adjusting mechanism for the airplane parts mainly comprises a plurality of three-coordinate numerical control positioners and a process interface. One end of the process joint is fixedly connected with the airplane component, and the other end of the process joint and the positioner form a spherical pair or a ball-and-socket pair. The positioner is movable in three mutually perpendicular directions (X, Y, Z) to change the position of its support point (the process connection center of sphere). The 3 points in space can define a plane, with the aircraft components supported by 3 or more than 3 locators. The multiple positioners can move along the respective X, Y, Z axes, and the airplane component can realize the pose adjustment with six degrees of freedom in three-dimensional space. 3 numerical control locator units can receive 9 control shaft motion instruction inputs and have redundant drive shafts. The large-part posture adjusting device is provided with 4 or 6 or 8 positioners, and a total of 12 or 18 or 24 driving shafts. The attitude adjusting device consisting of a plurality of positioners and airplane components is a redundant drive parallel structure. The axes move in concert so that the large part rests on the locators, can translate and rotate in space, and ensure that the large part or workpiece does not deform during movement. The parallel structure has the advantages of high rigidity, high precision, stable structure and uniform bearing capacity distribution. In the posture adjusting process, a key problem is how to ensure that all the support points of the numerical control positioner cooperatively move according to the rigid body motion rule.
The positioner drive placement direction is preferably parallel to the global coordinate system, and the X, Y, Z axes of the plurality of positioners are generally parallel and in the same direction. But the measurement precision of the positioner in the installation process is insufficient, and if the positioner is not adjusted in place, the installation angle error still exists.
The large part of the airplane is a rigid body, and rigid body motion comprises rigid body translation and rigid body dead axle rotation. The posture adjusting instruction data comprise X, Y, Z axis translation movement amount and A, B, C rotation angle increment. The attitude adjusting operation and control comprises attitude adjusting instruction decomposition, interpolation processing, speed planning and error compensation, and finally the actual position is output to the servo drive of each positioner.
The whole process of airplane posture adjustment and assembly is as follows.
(1) Positioning a component: hoisting the aircraft component to the positioner;
(2) initial measurement: measuring the position of a component measuring point by a laser tracker to obtain an initial position;
(3) initial adjustment: calculating deviation and sending a pose adjusting instruction, and adjusting the components through a positioner;
(4) and (3) accurate measurement: measuring the position of the measuring point of the component again by the laser tracker;
(5) and (3) precise adjustment: if the deviation exists, sending out an instruction again to adjust the pose;
(6) detecting whether the posture adjusting target is finished or not, and taking off the shelf or withdrawing the shelf when the assembly is finished; otherwise, repeating the step (4) and the step (5) to adjust the position.
At present, the operation and control method for adjusting the attitude of the domestic airplane has the following conditions:
(1) positioner posture adjustment without redundant shaft
A floating shaft or a follow-up shaft exists in a non-redundant driving shaft, the floating shaft can freely slide along with the change of the posture position of a large component in the posture adjusting process, the floating shaft can directly move from the starting point of the support point of the positioner to the final position of the posture adjusting, and the support point is not needed to be used as a particle on a rigid body for optimal path analysis. Six active control axes of three positioners can be adopted for the attitude adjustment of the six-degree-of-freedom airplane. For example, the wing attitude adjusting device is provided with 3 numerical control positioners, the first positioner is provided with X, Y, Z driving shafts, the 2 nd positioner is provided with only Y, Z driving shafts (X-axis floating), and the 3 rd positioner is provided with only Z driving shafts (XY-axis floating).
A. The number of active control shafts of the positioner is reduced, a part of shafts of the positioner adopt floating shafts, the positioner posture adjusting device with the floating shafts adjusts the posture of the airplane component by the active control shafts in the posture adjusting process, and the airplane component can drag the floating shafts to slide.
B. In the attitude adjusting mechanism force-position hybrid control system, one part of a positioner is an active control shaft, other redundant driving shafts are used as driven shafts, the active control shaft adjusts the attitude of an airplane component in the attitude adjusting process, and the driven shafts move along the direction of tension according to the feedback force of a force sensor on a process joint.
(2) Positioner attitude adjustment with redundant axes
The six-degree-of-freedom airplane attitude adjustment of the positioner with the redundant driving shafts needs to consider airplane components as rigid bodies for calculation, follows the principle that the distance between any two mass points in the rigid bodies is always kept unchanged, and has more complex interpolation algorithm processing. Pose adjustment is generally divided into a pose adjustment stage and a position adjustment stage, and generally does not overlap in time. The posture adjustment and the position adjustment are solved by adopting an algorithm of stepwise rotation and translation respectively according to time. The motion planning of each stage adopts a position-time mode, and generally adopts an integral cubic or cubic polynomial which is not segmented to carry out speed planning. And solving discrete points of each locator supporting point on a space moving curve, and directly outputting position coordinates to a driver of the locator.
The process of adjusting the posture with the redundant driving shaft 6 degrees of freedom generally comprises the following 4 stages:
A. the pitch angle, the deflection angle and the position are kept unchanged, the rotation is carried out around the coordinate axis of the device, and the roll angle is adjusted to a target angle.
B. And the roll angle, the deflection angle and the position are kept unchanged, the roll angle, the deflection angle and the position rotate around the coordinate axis of the roll angle, and the pitch angle is adjusted to a target angle.
C. The roll angle, the pitch angle and the position are kept unchanged, the device rotates around the coordinate axis of the device, and the deflection angle is adjusted to a target angle.
D. The attitude remains unchanged and the position is translated from the initial position to the target position.
In summary, the current situation analysis of the current posture adjusting operation and control method is as follows:
1) the positioner without the redundant active driving shaft mode has the advantages of less active driving shafts, simple control and low cost. The six-freedom-degree airplane posture adjusting device can adopt six active control shafts of three positioners and a positioner posture adjusting device with a floating shaft. The floating shaft mode needs large parts of the airplane to provide pulling force for dragging, and the large parts of the airplane have large internal stress. The follow-up mode follows the stress change and controls the driven shaft, can reduce the aircraft part stress of accent appearance process, but the driven shaft can not provide enough holding power voluntarily, and the accent appearance process can not be to the part shape keeping. The main defects of the mode without a redundant active driving shaft are that the number of the positioners is small, the supporting rigidity is insufficient, and the local deformation of the airplane is easily caused due to large local supporting force. This approach does not provide for the retention or support of aircraft components during attitude adjustment. Because the large airplane is large in size and heavy in weight, more positioners are needed for bearing, enough supporting points are provided to form a flexible support for shape keeping, and the positioner posture adjusting mode without a redundant active driving shaft is not suitable for large airplane posture adjustment;
2) the six-degree-of-freedom airplane attitude adjustment of the existing redundant driving shaft three-coordinate positioner generally comprises the steps of executing attitude adjustment step by step and then executing position adjustment, and the attitude adjustment time is longer;
3) acceleration is not accurately calculated in the motion planning process, the speed/acceleration allowable range of a driving motor of a three-coordinate numerical control positioner or the speed/acceleration allowable range of rotation or translation of a large part of an airplane is possibly exceeded in the airplane attitude adjusting process, the attitude adjusting operation is unstable or the attitude adjusting action is slow, and particularly the motor is easy to have impact when the attitude adjusting is started and finished;
4) the position error and the contour error of the supporting point are not accurately analyzed in the attitude adjusting process, and if the contour error is large or the mechanical positioning precision and the installation precision of a positioner are not high enough, a large part of the airplane may deform a small amount in the attitude adjusting process of the airplane, so that the airplane is subjected to overlarge stress and even is damaged.
Disclosure of Invention
In view of the above, the invention provides a three-coordinate positioner attitude adjusting operation and control method, a three-coordinate positioner attitude adjusting operation and control system, an attitude adjusting controller and a storage medium, which are applied to airplane digital assembly, can meet the acceleration requirement, have redundant driving shafts, do not need to rotate and translate step by step, do not need to limit the number of the shafts of drivers, have stable attitude adjusting process and no impact, and can overcome the defects of the three-coordinate positioner attitude adjusting operation and control processing in the existing airplane assembly.
The invention aims to provide a three-coordinate positioner posture adjusting operation and control method.
The invention also provides a three-coordinate positioner posture adjusting operation control system.
The third purpose of the invention is to provide a posture adjusting controller.
It is a fourth object of the present invention to provide a storage medium.
The first purpose of the invention can be achieved by adopting the following technical scheme:
a three-coordinate positioner posture adjusting operation and control method is applied to airplane digital assembly, and comprises the following steps:
establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, and resolving a translational movement amount and a translational direction vector of the rigid body, and a rotation angle and a rotation axis vector of the rigid body fixed axis rotation according to an attitude adjusting instruction;
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, and calculating a corresponding circular arc angular velocity range and a rigid body angular velocity range according to the allowable error of each circular arc track;
planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and a rotation angular speed range, an angular acceleration range, a translation speed range and a translation acceleration range which are allowed by attitude adjustment of a large part of the airplane;
according to the velocity planning of the rigid body compound motion, taking each locator supporting point as a mass point on the rigid body, calculating the maximum velocity and the maximum acceleration on each locator driving shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
after the speed and the acceleration of the rigid body compound motion are adjusted, the rigid body compound motion speed is planned and maintained again;
according to the new speed plan of the rigid body compound motion, carrying out interpolation calculation according to a time segmentation method, and outputting a three-axis instruction coordinate position of each locator;
and carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each positioner, and outputting the actual position of each axis driver.
Further, the establishing of the rigid body local coordinate system and the locator local coordinate system of the large aircraft component specifically includes:
establishing a global coordinate system Oxyz for a relative ground reference system;
establishing a rigid local coordinate system O for a large aircraft partlxyz, the X, Y, Z axial direction of the local rigid body coordinate system is parallel to the X, Y, Z axial direction of the global coordinate system, the rotation center of the local rigid body coordinate system is set as the origin of the global coordinate system, and the coordinate in the global coordinate system before the origin of the local coordinate system is adjusted to the attitude is Ol(px,py,pz)T
Establishing a locator local coordinate system O for the ith locatorixyz, the X, Y, Z axial direction of the local coordinate system of the positioner is the driving moving direction of the supporting point of the positioner along the X, Y, Z axis of the positioner, the origin of the local coordinate system of the positioner is the supporting point position after the X, Y, Z axis of the positioner returns to zero, and the coordinate of the origin of the local coordinate system of the ith positioner in the global coordinate system is Oi(oix,oiy,oiz)TThe coordinate of the ith locator supporting point in the global coordinate system is Pi(pix,piy,piz)T
Further, the resolving of the translational movement amount and the translational direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body fixed axis rotation according to the attitude adjusting instruction specifically includes:
resolving the translational motion quantity of the rigid body as follows:
Figure BDA0002536674330000051
resolving the translation direction vector of the rigid body as follows:
Figure BDA0002536674330000052
in the formula,
Figure BDA0002536674330000053
Firstly, rotating the rigid body around the Z axis by an angle A, then rotating the rigid body around the Y axis by an angle B, and finally rotating the rigid body around the X axis by an angle C, wherein the angle A is as follows:
Figure BDA0002536674330000054
wherein s1 ═ sin (a), c1 ═ cos (a), s2 ═ sin (b), c2 ═ cos (b), s3 ═ sin (c), c3 ═ cos (c);
resolving the rotation angle of the rigid body fixed shaft rotation, as follows:
Figure BDA0002536674330000055
solving a rotating shaft vector of the rigid body fixed shaft rotation, and adopting the following formula:
Figure BDA0002536674330000056
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000057
Figure BDA0002536674330000058
further, the method specifically includes, according to the rotating axis vector of the rigid body fixed axis rotation, the rigid body rotation center position and the current position of each locator support point, using each locator support point as a mass point on the rigid body, calculating the circle center and the radius of the spatial circular arc track of each locator in the rigid body fixed axis rotation process, and calculating the corresponding circular arc angular velocity range and the rigid body angular velocity range according to the allowable error of each circular arc track:
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, and calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, wherein the following formula is as follows:
Figure BDA0002536674330000059
Figure BDA00025366743300000510
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000061
is the circle center position of the spatial circular arc track of the ith positioner in the rotating process of the rigid body fixed shaft,
Figure BDA0002536674330000062
in the local rigid body coordinate system O before the orientation adjustment for the ith support point of the positionerlThe position in the xyz is determined by the position,
Figure BDA0002536674330000063
rotation axis vector for rigid body fixed axis rotation, riRadius of the spatial circular arc track of the ith positioner in the rigid body dead axle rotation process:
let TinpTo interpolate the cycle time, HerrFor error in height of bow, LcTo interpolate the cycle output chord length, the following equation is used:
Lc 2=8Herrri+4Herr 2
calculating the height error HerrThe chord length of (c) is as follows:
Figure BDA0002536674330000064
in the formula, Lc=VTinpo=ωiriTinpThen, then
Figure BDA0002536674330000065
If the ith locator adjusts the posture processBy allowable bow height error HerrThen, the rotational angular velocity ω of the rigid body is requirediMaximum, and bow height error HerrRadius r when constantiGreater allowable rigid body rotational angular velocity ωiThe smaller;
and solving the maximum radius in the space circular arc track radii of all the positioners as follows:
rmax=max(r1,r2,r3,…,ri,…,rN)
during interpolation, the interpolation period time TinpThe same angular speeds are the same when the rigid body fixed shaft rotates a plurality of circular arcs;
calculating the bow height error HerrRigid body winding meeting the requirements
Figure BDA0002536674330000066
Maximum rotational angular velocity, as follows:
Figure BDA0002536674330000067
further, the planning and trimming of the rigid body composite motion speed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range allowed by the attitude adjustment of the large airplane component specifically includes:
according to the maximum value of the angular velocity of the rigid body, the maximum angular velocity omega required by the strength of the rigid body fixed-axis rotating structure is adjustedmax=min(ωmax1max2);
Maximum angular acceleration α allowed by airplane large component attitude adjustmentmaxMaximum translational velocity vmaxMaximum translational acceleration amaxMaximum angular velocity omega required by strength of rigid body fixed-axis rotating structuremax=min(ωmax1max2) Velocity v at the beginning and end of the set of posturess=ve0, acceleration a at the beginning and end of posture adjustments=aeRotation angle theta of rigid body fixed axis rotationeAnd the translational movement quantity S of the rigid body, respectively carrying out bell-shaped acceleration/decelerationPlanning and calculating the rigid body composite motion speed, and calculating the actual maximum acceleration a of the time and the translation of each stagenowmaxActual maximum translational velocity vnowmaxActual maximum angular acceleration of rotation αnowmaxAnd the actual maximum angular velocity ωnowmaxAnd then carrying out rigid body composite motion speed planning time trimming.
Further, the calculation of the bell-shaped acceleration/deceleration rigid body composite motion speed plan specifically includes:
according to the translational movement quantity s and the maximum translational speed v of the rigid bodymaxMaximum translational acceleration amaxAnd translation plus acceleration jlThe method comprises the following steps of performing speed planning calculation in seven stages including an acceleration stage, a uniform acceleration stage, a deceleration stage, a uniform speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration stage; wherein:
the acceleration is calculated as follows:
Figure BDA0002536674330000071
wherein J is Jl
The acceleration is calculated as follows:
Figure BDA0002536674330000072
the velocity is calculated as follows:
Figure BDA0002536674330000073
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The translation movement amount is calculated as follows:
Figure BDA0002536674330000081
the translation speed is planned to be s ═ fs1(t),v=fv1(t),a=fa1(t),js=J(t);
According to bell type increasing/decreasing time T1s=T3s,T5s=T7sVelocity v at the beginning and end of the set of posturess=veAcceleration a at the beginning and end of the set-ups=ae0, and the acceleration and deceleration stages are mirror symmetric, resulting in T1s=T7s=T5s=T3s,T2s=T6s
The maximum speed and the maximum acceleration are limited as v in the safety range3≤vmax,Jt1≤amaxCalculating the acceleration stage time T1sTime T of uniform acceleration stage2sDecreasing acceleration stage time T3sTime T at uniform speed stage4sAcceleration and deceleration stage time T5sTime T of uniform deceleration stage6sTime T of deceleration stage7s
Calculating the actual maximum acceleration anowmax=jlT1sActual maximum velocity vnowmax=v3And total translational time Ts=T1s+T2s+T3s+T4s+T5s+T6s+T7s
Rotation angle theta according to rigid body fixed axis rotationeMaximum angular velocity ωmaxMaximum angular acceleration αmaxAnd angle of rotation plus acceleration jθThe method comprises the following steps of calculating speed planning in seven stages including an acceleration stage, a uniform acceleration stage, an acceleration reduction stage, a constant speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration reduction stage; wherein:
the angular acceleration is calculated as follows:
Figure BDA0002536674330000082
wherein J is Jθ
The angular acceleration is calculated as follows:
Figure BDA0002536674330000091
the angular velocity is calculated as follows:
Figure BDA0002536674330000092
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The rotation angle is calculated as follows:
Figure BDA0002536674330000093
the speed of rotation is programmed as jθ=J(t),θ=fθ1(t),ω=fω1(t),α=fα1(t);
According to bell type increasing/decreasing time T=T,T=TEstablishing a piecewise function of the rotation angle and adding an acceleration J ═ J according to the angleθAngle of rotation and attitude increment thetaeAngular velocity ω of starting and ending of posture adjustments=ωe0, angular acceleration α of starting and ending of pose adjustments=αe0, and the acceleration and deceleration stages are mirror symmetric, resulting in T=T=T=T,T=T;T=T=T=T,T=T
The maximum speed and the maximum acceleration are limited to be omega in a safety range3≤ωmax,Jt1≤αmaxCalculating the acceleration stage time TTime T of uniform acceleration stageDecreasing acceleration stage time TTime T at uniform speed stageAcceleration and deceleration stage time TTime T of uniform deceleration stageTime T of deceleration stage
Calculating the actual maximum angular acceleration αnowmaxActual maximum angular velocity ωnowmaxAnd total time of rotation Tθ=T+T+T+T+T+T+T
Further, the time adjustment for planning the rigid body compound motion speed specifically includes:
two motion time trimming to interpolation period time T for bell-type acceleration/deceleration speed planning of rigid body fixed axis rotation and rigid body translation respectivelyinpIntegral multiple, the translation time and the rotation time are adjusted to be equal, and the time of each stage after the time axis is adjusted and the actual maximum acceleration a of rigid translation after the time axis is adjusted are calculatednow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2max
Further, the calculation of the time of each stage after the time axis is adjusted and the actual maximum acceleration a of the rigid translationnow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2maxThe method specifically comprises the following steps:
total translational time TsOr total time of rotation TθRounded up to an interpolation period time TinpInteger multiple of (d) is as follows:
Figure BDA0002536674330000101
the rigid body translation and the rigid body dead axle rotation are synchronously carried out, and when the requirement is simultaneously started and finished, the translation time and the dead axle rotation time are adjusted to be the same time, as the following formula:
Tnow=Tnows=Tnowθ=max(Tnows,Tnowθ)
the time of each stage is adjusted proportionally as follows:
rigid body translation time adjustment proportion:
Figure BDA0002536674330000102
rigid body dead axle rotation time adjustment proportion:
Figure BDA0002536674330000103
T1s=T7s=T5s=T3s=T1sKnows,T2s=T6s=T2sKnows,T4s=T4sKnows
T=T=T=T=TKnowθ,T=T=TKnowθ,T=TKnowθ
translation distance S and rotation angle thetaeRemains unchanged, TnowsAnd TnowθThe time is prolonged, the time of each stage is prolonged, and the actual speed, the actual acceleration and the actual jerk are adjusted as follows:
adjusting the actual maximum speed of rigid translation and the actual maximum angular speed of rigid fixed shaft rotation:
Figure BDA0002536674330000104
Figure BDA0002536674330000105
actual maximum acceleration and rigidity of rigid translationAdjusting the actual maximum angular acceleration of the body fixed shaft rotation:
Figure BDA0002536674330000106
Figure BDA0002536674330000107
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure BDA0002536674330000111
Figure BDA0002536674330000112
after the time, speed, acceleration and jerk of each stage are adjusted in proportion, the rigid translation movement amount and the rigid fixed axis rotation angle of each stage are kept unchanged with the speed before adjustment, and the adjusted speed is planned as follows:
rigid translation: s ═ fs(t);v=fv(t);a=fa(T) where T ∈ [0, Tnow];s∈[0,S]
Rigid body dead axle rotates: theta ═ fθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe]。
Further, the planning according to the velocity of the rigid body compound motion, using each locator support point as a mass point on the rigid body, calculating a maximum velocity and a maximum acceleration on each locator drive shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to a velocity range and an acceleration range allowed by each locator drive shaft specifically includes:
and taking each locator support point as a mass point on the rigid body, carrying out synchronous superposition motion of fixed axis rotation and translation on the rigid body, solving a space circular arc motion track, a speed and an acceleration of each locator drive shaft by utilizing inverse kinematics position inverse solution, calculating the maximum speed and the maximum acceleration on each locator drive shaft in a locator local coordinate system, and adjusting the speed and the acceleration of rigid body composite motion according to the speed range and the acceleration range allowed by each locator drive shaft.
Further, the method includes that each locator support point is used as a mass point on a rigid body, the rigid body performs synchronous superposition motion of fixed axis rotation and translation, inverse solution is performed by using a reverse kinematics position, a space circular arc motion track, a speed and an acceleration of each locator drive shaft are solved, the maximum speed and the maximum acceleration of each locator drive shaft are calculated in a local coordinate system of the locator, and the speed and the acceleration of rigid body composite motion are adjusted according to the speed range and the acceleration range allowed by each locator drive shaft, and specifically includes the following steps:
with the ith locator supporting point space arc CiEstablishing a new local coordinate system C with the center of the circle as the origin of coordinatesixyz, local coordinate system CiThe X, Y, Z axis of xyz is parallel to the localizer local coordinate system OiX, Y, Z axis of xyz;
the central angle in the space circular arc motion track is the angle theta of rigid rotation ═ fθ(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiTranslation distance s ═ f in xyzs(t);
Rigid translation direction vector
Figure BDA0002536674330000113
Wherein
Figure BDA0002536674330000114
Corresponding to a local coordinate system CiThe origin of xyz is in the localizer local coordinate system OiVector in xyz direction
Figure BDA0002536674330000115
Figure BDA0002536674330000116
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational position component in xyz is in the form ofThe following:
fis(t)=[xis(t) yis(t) zis(t)]T
in the formula, xis(t)=uixfs(t),yis(t)=uiyfs(t),zis(t)=uizfs(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational velocity component in xyz is of the form:
fiv(t)=[xiv(t) yiv(t) ziv(t)]T
in the formula, xiv(t)=uixfv(t),yiv(t)=uiyfv(t),ziv(t)=uizfv(t);
Local coordinate system O of positioneriThe maximum speed of X, Y, Z shaft translation process in xyz is as follows:
viSxmax=max(|xiv(t)|)=|uix|max(fv(t))=|uix|vnow2max
viSymax=max(|yiv(t)|)=|uiy|max(fv(t))=|uiy|vnow2max
viSzmax=max(|ziv(t)|)=|uiz|max(fv(t))=|uiz|vnow2max
local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational acceleration component in xyz is of the form:
fia(t)=[xia(t) yia(t) zia(t)]T
in the formula, xia(t)=uixfa(t),yia(t)=uiyfa(t),zia(t)=uizfa(t);
Local coordinate system O of positioneriX, Y, Z axis in xyzThe maximum acceleration of the translation process is as follows:
aiSxmax=max(|xia(t)|)=|uix|max(fa(t))=|uix|anow2max
aiSymax=max(|yia(t)|)=|uiy|max(fa(t))=|uiy|anow2max
aiSzmax=max(|zia(t)|)=|uiz|max(fa(t))=|uiz|anow2max
further, the adjusting the speed and the acceleration of the rigid body composite motion according to the speed range and the acceleration range allowed by the driving shaft of each positioner specifically includes:
rigid body local coordinate system O in rigid body fixed axis rotationlAxis of rotation of xyz
Figure BDA0002536674330000121
Rotation angle theta f of rigid body fixed axis rotationθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe];
Before adjusting the posture, the support point of the ith positioner is in the local rigid coordinate system OlPosition vector in xyz
Figure BDA0002536674330000122
I-th locator in rigid local coordinate system OlRadius of rotation in xyz
Figure BDA0002536674330000123
Circle center coordinate
Figure BDA0002536674330000124
Rigid body fixed axis rotation angle theta ═ fθ(t) rigid body rotation Rw,θThe following formula:
Figure BDA0002536674330000131
in the formula, sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ(t),t∈[0,Tnow],θ∈[0,θe](ii) a In the posture adjusting process, the support point of the ith positioner is in a rigid body local coordinate system OlThe position vector in xyz is
Figure BDA0002536674330000132
Rigid body rotation axis in local coordinate system CiIn xyz are
Figure BDA0002536674330000133
The support point of the ith positioner in the local coordinate system CiPosition C in xyzi(θ) is a function of the rotation angle θ, as follows:
Figure BDA0002536674330000134
Figure BDA0002536674330000135
the support point of the ith positioner in the local coordinate system CiPosition C in xyziThe component form of (θ) is as follows:
Ci(θ)=[xi(θ) yi(θ) zi(θ)]T,xi(θ),yi(θ),zi(θ)
Cithe normal direction vector for any θ position is given by:
Figure BDA0002536674330000136
Figure BDA0002536674330000137
Cithe normal direction vector component for any θ position is of the form:
Figure BDA0002536674330000138
xin(θ),yin(θ),zin(θ);
Figure BDA0002536674330000139
xint(fθ(t)),yint(fθ(t)),zint(fθ(t));
Cithe maximum absolute value of the axis component of the normal direction vector X, Y, Z at any θ position is given by:
xintmax=max(|xint(fθ(t))|)=max(|xin(θ)|)
yintmax=max(|yint(fθ(t))|)=max(|yin(θ)|)
zintmax=max(|zint(fθ(t))|)=max(|zin(θ)|)
Cithe tangential direction vector at any θ position is given by:
Figure BDA00025366743300001310
wherein
Figure BDA00025366743300001311
Figure BDA00025366743300001312
CiThe tangential direction vector component at any θ position is of the form:
Figure BDA0002536674330000141
x(θ),y(θ),z(θ);
Figure BDA0002536674330000142
xiτt(fθ(t)),yiτt(fθ(t)),ziτt(fθ(t));
Cithe maximum absolute value of the axial component of the tangential direction vector X, Y, Z at any θ position is given by:
xiτtmax=max(|xiτt(fθ(t))|)=max(|x(θ)|)
yiτtmax=max(|yiτt(fθ(t))|)=max(|y(θ)|)
ziτtmax=max(|ziτt(fθ(t))|)=max(|z(θ)|)
the support point of the ith positioner in the local coordinate system CiLinear velocity v in xyz(t)=rifω(t);
The support point of the ith positioner in the local coordinate system CiMaximum linear velocity max (v) in xyz(t))=riωnow2max
The support point of the ith positioner in the local coordinate system CiSpeed of circular arc motion in xyz
Figure BDA0002536674330000143
The support point of the ith positioner in the local coordinate system CiThe circular arc motion velocity component in xyz is of the form:
fivτ(t)=[xivτ(t) yivτ(t) zivτ(t)]T
in the formula, xivτ(t)=v(t)xiτt(fθ(t)),yivτ(t)=v(t)yiτt(fθ(t)),zivτ(t)=v(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiThe maximum linear velocity of the circular arc motion in xyz multiplied by the maximum value of each axial component of the direction vector is not less than the circular arc motion fivτ(t) maximum speed of each axis, as follows:
max(|xivτ(t)|)=max(v(t)|xiτt(fθ(t))|)≤max(v(t))max(|xiτt(fθ(t))|)
max(|yivτ(t)|)=max(v(t)|yiτt(fθ(t))|)≤max(v(t))max(|yiτt(fθ(t))|)
max(|zivτ(t)|)=max(v(t)|ziτt(fθ(t))|)≤max(v(t))max(|ziτt(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion speed fivτ(t) and translational velocity fiv(t) the sum of the synchronous superposition speed, the maximum speed of the shaft component of the translational speed X, Y, Z and the maximum speed of the shaft component of the circular motion speed X, Y, Z is greater than the actual maximum speed of the positioner X, Y, Z, if the sum is less than the allowable speed range of each driving shaft, the safety is ensured, otherwise, the speed of the rigid body compound motion is reduced, and the method comprises the following steps:
vixtest≥max(v(t)|xiτt(fθ(t))|)+max(|xiv(t)|)≥max(|xivτ(t)+xiv(t)|)
viytest≥max(v(t)|yiτt(fθ(t))|)+max(|yiv(t)|)≥max(|yivτ(t)+yiv(t)|)
viztest≥max(v(t)|ziτt(fθ(t))|)+max(|ziv(t)|)≥max(|zivτ(t)+ziv(t)|)
in the formula, xivτ(t)+xiv(t) is the X-axis actual speed, yivτ(t)+yiv(t) is the actual speed of the Y-axis, zivτ(t)+ziv(t) is the Z-axis actual speed;
vixtest=max(v(t))max(|xiτt(fθ(t))|)+max(|xiv(t)|)=riωnow2maxxiτtmax+|uix|vnow2max
viytest=max(v(t))max(|yiτt(fθ(t))|)+max(|yiv(t)|)=riωnow2maxyiτtmax+|uiy|vnow2max
viztest=max(v(t))max(|ziτt(fθ(t))|)+max(|ziv(t)|)=riωnow2maxziτtmax+|uiz|vnow2max
if v isixtest≤vixmaxIs provided with
Figure BDA0002536674330000151
Otherwise
Figure BDA0002536674330000152
If v isiytest≤viymaxIs provided with
Figure BDA0002536674330000153
Otherwise
Figure BDA0002536674330000154
If v isiztest≤vizmaxIs provided with
Figure BDA0002536674330000155
Otherwise
Figure BDA0002536674330000156
Ith positioner velocity adjustment factor
Figure BDA0002536674330000157
The support point of the ith positioner in the local coordinate system CiTangential acceleration f in xyziaτ(t)=rifα(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of tangential acceleration max (f) in xyziaτ(t))=riαnow2max
The support point of the ith positioner in the local coordinate system CiCircular arc tangential acceleration vector in xyz
Figure BDA0002536674330000158
Figure BDA0002536674330000159
The support point of the ith positioner in the local coordinate system CiThe circular arc tangential acceleration component in xyz is of the form:
a(t)=[xiaτ(t) yiaτ(t) ziaτ(t)]T
in the formula, xiaτ(t)=fiaτ(t)xiτt(fθ(t)),yiaτ(t)=fiaτ(t)yiτt(fθ(t)),ziaτ(t)=fiaτ(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiCentripetal acceleration f in xyzian(t)=rifω 2(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of centripetal acceleration max (f) in xyzian(t))=riωnow2max 2
The support point of the ith positioner in the local coordinate system CiCircular arc normal acceleration vector in xyz
Figure BDA00025366743300001510
Figure BDA00025366743300001511
The support point of the ith positioner in the local coordinate system CiThe circular arc normal acceleration component in xyz is of the form:
ain(t)=[xian(t) yian(t) zian(t)]T
in the formula, xiaθ(t)=fiaτ(t)xiτt(fθ(t))+fian(t)xint(fθ(t));yiaθ(t)=fiaτ(t)yiτt(fθ(t))+fian(t)yint(fθ(t));ziaθ(t)=fiaτ(t)ziτt(fθ(t))+fian(t)zint(fθ(t));
The support point of the ith positioner in the local coordinate system CiCircular arc motion acceleration a in xyz(t) X, Y, Z axis component maximum value is not more than maximum value of angular acceleration and angular velocity and each axis normal component and tangential component maximum value are calculated as follows:
max(|xiaθ(t)|)≤max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)
max(|yiaθ(t)|)≤max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)
max(|ziaθ(t)|)≤max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion acceleration a(t) and translational acceleration fia(t) the sum of the synchronous superimposed acceleration, the maximum value of the shaft component of the translational acceleration X, Y, Z and the maximum value of the shaft component of the circular arc motion acceleration X, Y, Z is greater than the actual maximum acceleration of the positioner X, Y, Z, if the sum is smaller than the allowable acceleration range of each driving shaft, the safety is ensured, otherwise, the acceleration and the angular speed of the rigid body composite motion are reduced, and the method comprises the following steps:
aixtest≥max(|xiaθ(t)|)+max(|xia(t)|)≥max(|xiaθ(t)+xia(t)|)
aiytest≥max(|yiaθ(t)|)+max(|yia(t)|)≥max(|yiaθ(t)+yia(t)|)
aiztest≥max(|ziaθ(t)|)+max(|zia(t)|)≥max(|ziaθ(t)+zia(t)|)
in the formula, xiaθ(t)+xia(t) is the actual acceleration of the X-axis, yiaθ(t)+yia(t) is the actual acceleration of the Y-axis, ziaθ(t)+zia(t) is the Z-axis actual acceleration;
aixtest=max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)+max(|xia(t)|)
=riαnow2maxxiτtmax+riωnow2max 2xintmax+|uix|anow2max
aiytest=max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)+max(|yia(t)|)
=riαnow2maxyiτtmax+riωnow2max 2yintmax+|uiy|anow2max
aiztest=max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)+max(|zia(t)|)
=riαnow2maxziτtmax+riωnow2max 2zintmax+|uiz|anow2max
if aixtest≤aixmaxIs provided with
Figure BDA0002536674330000161
Otherwise
Figure BDA0002536674330000162
If aiytest≤aiymaxIs provided with
Figure BDA0002536674330000163
Otherwise
Figure BDA0002536674330000164
If aiztest≤aizmaxIs provided with
Figure BDA0002536674330000165
Otherwise
Figure BDA0002536674330000166
Acceleration adjustment coefficient of ith positioner
Figure BDA0002536674330000167
If it is
Figure BDA0002536674330000168
And is
Figure BDA0002536674330000169
The rotational angular velocity of the rigid body is reduced, the centripetal acceleration is reduced, and the adjustment is performed
Figure BDA0002536674330000171
Determining the maximum value of the speed regulating coefficient in the attitude regulating process of the airplane
Figure BDA0002536674330000172
Solving the maximum value of the acceleration regulating coefficient in the process of adjusting the attitude of the airplane
Figure BDA0002536674330000173
And adjusting the speed and the acceleration of rigid translation and fixed shaft rotation according to the speed and the acceleration adjusting coefficient in the attitude adjusting process of the airplane, as follows:
maximum speed of rigid translation and maximum angular speed of rigid fixed shaft rotation:
Figure BDA0002536674330000174
Figure BDA0002536674330000175
maximum acceleration of rigid translation and maximum angular acceleration of rigid fixed axis rotation:
Figure BDA0002536674330000176
Figure BDA0002536674330000177
the jerk of rigid translation and the jerk of rigid fixed axis rotation: j is a function ofl=jl2,jθ=jθ2
Further, the planning and modifying of the rigid body compound motion speed again specifically includes:
and (3) re-planning the speed of the rigid body translation as follows:
according to the maximum velocity v of rigid translationmaxMaximum acceleration amaxJerk jl, initial and final velocity of posture adjustment vs=veAcceleration a at the beginning and end of the set-ups=aeWhen the rigid translation movement quantity S is equal to 0, the ring-type acceleration/deceleration rigid translation speed planning calculation is carried out, and the actual maximum speed v of the rigid translation is calculatednewmaxAnd the actual maximum acceleration anewmax
Recalculating translation run time TsEach stage time T1s,T2s,T3s,T4s,T5s,T6s,T7s(ii) a Wherein T is1s=T7s=T5s=T3s,T2s=T6s
The speed planning time is rounded as follows:
Figure BDA0002536674330000178
and (3) re-planning the speed of the rigid body dead axle rotation, as follows:
maximum angular velocity omega based on rigid body dead axle rotationmaxMaximum angular acceleration αmaxAngular jerk jθSpeed omega of starting and ending of posture adjustments=ωe0, acceleration α for start and end of stance turns=αeAngle increment theta of rigid body fixed axis rotationePerforming bell-shaped acceleration/deceleration planning calculation on the rotation speed of the rigid body fixed shaft to calculate the actual maximum angular speed omega of the rigid body fixed shaft rotationnewmaxAnd maximum angular acceleration αnewmax
Recalculating rigid body dead axle rotation time TθEach stage having a time T,T,T,T,T,T,T(ii) a Wherein T is=T=T=T,T=T
The speed planning time is rounded as follows:
Figure BDA0002536674330000181
the rigid body translation and the rigid body fixed shaft rotation are synchronously carried out, and the translation time and the fixed shaft rotation time are adjusted to be the same time as follows:
Tnew=Tnews=Tnewθ=max(Tnews,Tnewθ)
wherein the time of each stage is proportionally adjusted as follows:
T1s=T7s=T5s=T3s=T1sKnews,T2s=T6s=T2sKnews,T4s=T4sKnews
T=T=T=T=TKnewθ,T=T=TKnewθ,T=TKnewθ
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000182
adjusting the proportion of rigid translation time;
Figure BDA0002536674330000183
rigid body fixed axis rotation time adjustment proportion;
adjusting the actual speed, the actual acceleration and the actual jerk as follows:
adjusting the actual maximum speed of rigid translation and the actual angular speed of rigid fixed shaft rotation:
Figure BDA0002536674330000184
Figure BDA0002536674330000185
adjusting the actual maximum acceleration of rigid translation and the actual angular acceleration of rigid fixed shaft rotation:
Figure BDA0002536674330000186
Figure BDA0002536674330000187
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure BDA0002536674330000188
Figure BDA0002536674330000189
obtaining an adjusted speed plan:
rigid translation: s ═ fs3(t);v=fv3(t);a=fa3(T) where T ∈ [0, Tnew];s∈[0,S];
Rigid body dead axle rotates: theta ═ fθ3(t);ω=fω3(t);α=fα3(T) where T ∈ [0, Tnew];θ∈[0,θe]。
Further, the interpolating calculation is performed according to a time division method according to the new velocity plan of the rigid body compound motion, and the three-axis instruction coordinate position of each locator is output, which specifically includes:
according to the new speed plan of rigid body composite motion, rigid body fixed axis rotation interpolation and rigid body translation interpolation are respectively carried out according to a time division method, the position of each locator supporting point in a global coordinate system is calculated after synchronous superposition, then the locator supporting point is converted into a local coordinate system of each locator, and the three-axis instruction coordinate position of each locator is output.
Further, the planning according to the new velocity of the rigid body compound motion, respectively performing rigid body fixed axis rotation interpolation and rigid body translation interpolation according to a time division method, calculating the position of each locator supporting point in a global coordinate system after synchronous superposition, then converting to a local coordinate system of each locator, and outputting a three-axis instruction coordinate position of each locator specifically comprises:
rigid body local coordinate system OlPosition in global coordinate system before origin attitude adjustment of xyz
Figure BDA0002536674330000191
Local coordinate system O of positioneriLocation of origin of xyz in global coordinates
Figure BDA0002536674330000192
The position of the ith locator support point before attitude adjustment, including the position in the global coordinate system
Figure BDA0002536674330000193
In a rigid body local coordinate system OlPosition in xyz
Figure BDA0002536674330000194
And in the localizer local coordinate system OiPosition in xyz
Figure BDA0002536674330000195
The position of the ith locator support point after attitude adjustment is included in the rigid body local coordinate system OlPosition in xyz
Figure BDA0002536674330000196
Position in global coordinates
Figure BDA0002536674330000197
And in the localizer local coordinate system OiPosition in xyz
Figure BDA0002536674330000198
Calculating the interpolation position of the ith positioner supporting point attitude adjusting process as follows:
the rotation angle function of the rigid body fixed axis rotation is as follows:
θ=fθ3(t);ω=fω3(t);α=fα3(t);t∈[0,Tnew];θ∈[0,θe];
rigid body rotation axis in rigid body local coordinate system OlVector of xyz
Figure BDA0002536674330000199
The function of the amount of movement of the rigid translation is:
s=fs3(t);v=fv3(t);a=fa3(t);t∈[0,Tnew];s∈[0,S];
rigid translation direction vector
Figure BDA00025366743300001910
Solving the i-th locator supporting point in the local coordinate system O of the locatorixyz location function
Figure BDA00025366743300001911
The following formula:
Figure BDA00025366743300001912
in the formula (I), the compound is shown in the specification,
Figure BDA00025366743300001913
for the position vector of the ith localizer support point in the global coordinate system, the following equation is used:
Figure BDA00025366743300001914
in the formula (I), the compound is shown in the specification,
Figure BDA00025366743300001915
is the position of the origin of the rigid body local coordinate system in the global coordinate system in the pose adjusting process,
Figure BDA00025366743300001916
when the rotation and translation of the rigid body fixed shaft are synchronously superposed, the support point of the ith positioner is in the local coordinate system O of the positioneriThe position calculation formula for xyz is as follows:
Figure BDA0002536674330000201
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000202
sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ3(t),t∈[0,Tnew],θ∈[0,θe];
the attitude adjusting process of the ith positioner supporting point is carried out in a local coordinate system O of the positioneriThe position component of xyz is of the form:
Figure BDA0002536674330000203
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000204
for interpolationThe output X-axis instruction coordinate position,
Figure BDA0002536674330000205
in order to interpolate the output Y-axis command coordinate position,
Figure BDA0002536674330000206
the Z-axis command coordinate position is output for interpolation.
Further, the performing spatial compensation according to the three-axis instruction coordinate position of each locator and the spatial error data, and outputting the actual position of each axis driver specifically includes:
and performing reverse clearance compensation and pitch error compensation of each axis according to the three-axis instruction coordinate position of each positioner, performing three-axis compensation processing according to the spatial error data, and outputting the actual position of each axis driver.
Further, according to the three-axis instruction coordinate position of each positioner, reverse clearance compensation and pitch error compensation of each axis are performed, and then three-axis compensation processing is performed according to spatial error data, and the actual position of each axis driver is output, which specifically includes:
reading X, Y, Z shaft instruction coordinate position of each locator, performing reverse clearance compensation and pitch error compensation of each shaft, if the locator is at a single-shaft measuring point, directly reading reverse clearance compensation data and pitch error compensation data, if the locator is not at the single-shaft measuring point, performing linear interpolation according to error values of two end points of the single-shaft measuring interval, compensating the single-shaft pitch error of the single-shaft measuring interval, and adding a reverse clearance value;
reading X, Y, Z axis instruction coordinate position of each locator, performing spatial error compensation, directly reading data for compensation if the position is on the grid vertex of the spatial error measurement, reading eight vertex error data of a grid for spatial linear interpolation if the position is not on the grid vertex of the spatial error measurement in a certain grid, and solving the spatial error fitted by the eight vertices of the grid;
and after the reverse clearance compensation, the pitch error compensation and the space error compensation of each shaft are carried out, the actual position of each shaft driver is output.
The second purpose of the invention can be achieved by adopting the following technical scheme:
a three-coordinate locator posture-adjusting operation and control system is applied to airplane digital assembly, and comprises:
the first resolving module is used for establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, resolving the translational movement amount and the translational direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body in fixed-axis rotation according to the attitude adjusting instruction;
the second resolving module is used for resolving the circle center and the radius of a space circular arc track of each locator in the rigid body fixed axis rotation process according to the rotating shaft vector of the rigid body fixed axis rotation, the rigid body rotating center position and the current position of each locator supporting point as the mass point on the rigid body, and resolving the corresponding circular arc angular speed range and the rigid body angular speed range according to the allowable error of each circular arc track;
the first planning and finishing module is used for planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range which are allowed by the attitude adjustment of the large airplane component;
the adjusting module is used for calculating the maximum speed and the maximum acceleration of each locator driving shaft by taking each locator supporting point as a mass point on the rigid body according to the velocity plan of the rigid body composite motion, and adjusting the velocity and the acceleration of the rigid body composite motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
the second planning and trimming module is used for re-planning and trimming the rigid body composite motion speed after adjusting the speed and the acceleration of the rigid body composite motion;
the interpolation calculation module is used for carrying out interpolation calculation according to a time division method according to a new speed plan of rigid body compound motion and outputting a three-axis instruction coordinate position of each locator;
and the compensation module is used for carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each locator and outputting the actual position of each axis driver.
The third purpose of the invention can be achieved by adopting the following technical scheme:
a posture adjusting controller comprises a processor and a memory for storing an executable program of the processor, and when the processor executes the program stored in the memory, the posture adjusting operation and control method of the three-coordinate positioner is realized.
The fourth purpose of the invention can be achieved by adopting the following technical scheme:
a storage medium stores a program, and when the program is executed by a processor, the three-coordinate locator posture adjusting operation and control method is realized.
Compared with the prior art, the invention has the following beneficial effects:
1. the six-degree-of-freedom attitude adjusting process of the large part of the airplane is a rigid body compound motion of simultaneously executing rigid body translation and rigid body dead axle rotation, and the attitude adjusting time can be shortened; the attitude adjusting interpolation calculation has no limit on the number of redundant drive shafts, and each locator support point is calculated as a mass point on the rigid body, so that the requirement that the distance between any two points on the rigid body is kept unchanged in the attitude adjusting process is met, and the internal stress of airplane components is reduced. The device can be used for adjusting the attitude of a multi-positioner airplane with a redundant driving shaft, and meets the requirement of shape maintenance in the attitude adjusting process of a large airplane.
2. According to the invention, a user only needs to input an attitude adjusting instruction of an airplane component with six degrees of freedom, according to set attitude adjusting parameters, an attitude adjusting interpolation algorithm automatically calculates the maximum translational speed, the maximum translational acceleration, the maximum rotational angular speed and the maximum angular acceleration which meet the requirements of the airplane large component according to the current position of the airplane component and the attitude adjusting instruction, and performs speed planning according to the maximum speed and the maximum acceleration which meet the requirements of each locator driving shaft, and the finishing treatment is added aiming at the condition that the speed planning time is not integral multiple of the interpolation period time, so that the speed of the airplane in the whole attitude adjusting process is stable without impact, and the operation of the airplane large component in the attitude adjusting process is stable. Satisfactory results can be obtained without repeated attempts.
3. The invention limits and compensates the error of the positioner support point in the process of adjusting the attitude and interpolating the large part of the airplane, reduces the internal stress and the deformation of the large part of the airplane in the process of adjusting the attitude, improves the assembly quality, mainly analyzes the arc contour error in the rigid body rotation process, performs coordinate rotation processing on the condition that the axial direction of the positioner X, Y, Z is not parallel to the axial direction of the global coordinate system X, Y, Z, and performs space compensation on the positioning error of the positioner.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to the structures shown in the drawings without creative efforts.
Fig. 1 is a flowchart of a three-coordinate positioner pose adjusting operation and control method in embodiment 1 of the present invention.
Fig. 2 is a block diagram of a three-coordinate positioner pose adjusting operation and control system according to embodiment 2 of the present invention.
Fig. 3 is a block diagram of a posture adjustment controller according to embodiment 3 of the present invention.
Detailed Description
In order to make the objects, technical solutions and advantages of the embodiments of the present invention clearer and more complete, the technical solutions in the embodiments of the present invention will be described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are some embodiments of the present invention, but not all embodiments, and all other embodiments obtained by a person of ordinary skill in the art without creative efforts based on the embodiments of the present invention belong to the protection scope of the present invention.
Before discussing exemplary embodiments in more detail, it should be noted that some exemplary embodiments are described as processes or methods depicted as flowcharts. Although a flowchart may describe the steps as a sequential process, many of the steps in the equation can be performed in parallel, concurrently, or simultaneously. In addition, the order of the steps may be rearranged. The process may be terminated when its operations are completed, but may have additional steps not included in the figure. The processes may correspond to methods, functions, procedures, subroutines, and the like.
Example 1:
as shown in fig. 1, the present embodiment provides a three-coordinate positioner pose adjusting operation and control method, which is applied to a pose adjusting controller for butt joint of large components in airplane digital assembly, can meet acceleration requirements, has redundant driving shafts, and can support the large components of an airplane to perform pose adjusting control with six degrees of freedom, and includes the following steps:
s101, establishing a local rigid body coordinate system and a local positioner coordinate system of the large airplane component, and resolving the translation movement amount and the translation direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body fixed axis rotation according to the attitude adjusting instruction.
A. And establishing a rigid body local coordinate system and a locator local coordinate system of the large part of the airplane.
Describing the current aircraft large part and each locator position before attitude adjustment, establishing the following coordinates:
establishing a global coordinate system Oxyz for a relative ground reference system;
establishing a rigid local coordinate system O for a large aircraft partlxyz, the X, Y, Z axial direction of the local rigid body coordinate system is parallel to the X, Y, Z axial direction of the global coordinate system, the rotation center of the local rigid body coordinate system is set as the origin of the global coordinate system, and the coordinate in the global coordinate system before the origin of the local coordinate system is adjusted to the attitude is Ol(px,py,pz)T
Establishing a locator local coordinate system O for the ith locatorixyz, the X, Y, Z axis of the positioner local coordinate system is the direction of the positioner support point along the X, Y, Z axis of the positioner (i.e. the direction of the X, Y, Z axis servo drive motor drive motion), which may be non-parallel to the X, Y, Z axis of the global coordinate system, and the attitude of the positioner local coordinate system that is not parallel to the X, Y, Z axis of the global coordinate system is known to adjust the euler angle or rotation matrix RiOrigin of local coordinate system of positionerThe point is the position of the X, Y, Z axis zero-reset supporting point of the positioner, and the coordinate of the origin of the i-th positioner local coordinate system in the global coordinate system is Oi(oix,oiy,oiz)TThe coordinate of the ith locator supporting point in the global coordinate system is Pi(pix,piy,piz)T
B. And resolving the translational movement amount and the translational direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body fixed axis rotation according to the attitude adjusting instruction.
Specifically, the compound motion of the six-degree-of-freedom pose adjustment of the airplane is decomposed into rigid translation and fixed-axis rotation synchronous superposition, the translation direction vector and the movement amount of the translation path of the position adjustment are calculated, the attitude adjustment instruction is converted into a rotation process which is completed by rotating around a rigid Euler axis (namely a rotating axis) once, and the rotation angle and the rotating axis vector of the rigid fixed-axis rotation (rotating around a rigid rotating center) are calculated.
The attitude adjusting instruction is an airplane six-degree-of-freedom attitude adjusting (pose adjusting) instruction, and is generally similar to a P _ Alignment (x, y, z, A, B and C), wherein x, y, z, A, B and C are generally a translational increment and a rotation angle increment relative to the position before attitude adjustment, x, y and z are rigid body translational movement increments of a large part of an airplane along the axial direction of a global coordinate system X, Y, Z, and A, B and C are rotation angle increments of the large part of the airplane along rigid body coordinate axes respectively.
Resolving the translational motion quantity of the rigid body as follows:
Figure BDA0002536674330000231
resolving the translation direction vector of the rigid body as follows:
Figure BDA0002536674330000232
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000233
translation endRear rigid body local coordinate system OlThe origin of xyz is represented by the coordinate O in the global coordinate system Oxyzle(px+x,py+y,pz+z)T
The rotation around the rotation center from the current posture can be described by the common conditions that the rotation is performed by an angle A around the Z axis of the rigid body, then the rotation is performed by an angle B around the Y axis of the rigid body, and finally the rotation is performed by an angle C around the X axis of the rigid body, or the rotation can be performed in other modes. The different euler angular rotations can be converted into corresponding rotation matrices R, as follows:
R=RA·RB·RC
Figure BDA0002536674330000241
firstly, rotating the rigid body around the Z axis by an angle A, then rotating the rigid body around the Y axis by an angle B, and finally rotating the rigid body around the X axis by an angle C, wherein the angle A is as follows:
Figure BDA0002536674330000242
wherein s1 ═ sin (a), c1 ═ cos (a), s2 ═ sin (b), c2 ═ cos (b), s3 ═ sin (c), c3 ═ cos (c);
can convert rigid body fixed axis rotation into rotation
Figure BDA0002536674330000243
The shaft rotates:
resolving the rotation angle of the rigid body fixed shaft rotation, as follows:
Figure BDA0002536674330000244
solving a rotating shaft vector of the rigid body fixed shaft rotation, and adopting the following formula:
Figure BDA0002536674330000245
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000246
Figure BDA0002536674330000247
s102, according to a rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, each locator supporting point is used as a mass point on the rigid body, the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process are calculated, and a corresponding circular arc angular speed range and a rigid body angular speed range are calculated according to the allowable error of each circular arc track.
Rigid body local coordinate system OlPosition in global coordinate system before origin attitude adjustment of xyz
Figure BDA0002536674330000248
I-th locator local coordinate system OiPlacement of xyz origin in position in global coordinate system
Figure BDA0002536674330000249
Position of ith locator support point in global coordinate system before attitude adjustment
Figure BDA0002536674330000251
Before the support point of the ith positioner is adjusted to the posture, the local rigid coordinate system O is positionedlPosition in xyz
Figure BDA0002536674330000252
Figure BDA0002536674330000253
The support point of the ith positioner is in the local coordinate system O of the positioneriPosition in xyz
Figure BDA0002536674330000254
Figure BDA0002536674330000255
According to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, and calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, wherein the following formula is as follows:
Figure BDA0002536674330000256
Figure BDA0002536674330000257
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000258
is the circle center position of the spatial circular arc track of the ith positioner in the rotating process of the rigid body fixed shaft,
Figure BDA0002536674330000259
rotation axis vector for rigid body fixed axis rotation, riThe radius of the space circular arc track of the ith positioner in the rigid body dead axle rotation process.
Similar calculation is carried out to obtain the space circular arc radius r of all the locators1,r2,r3,…,ri,…,rN
A time division method is adopted to output a position coordinate on the circular arc each time through circular arc interpolation, the actual track replaces the arc with a string, and a bow height error (namely a circular arc track error) exists. The height of the bow can be considered as the deformation of the airplane during the posture adjustment process of the large parts. If the height error of the bow is not large, the posture adjusting process is safe because a small amount of gaps exist in the posture adjusting device; otherwise, too large a bow height error may cause deformation of the aircraft components, which is to be avoided.
Let TinpTo interpolate the cycle time, HerrFor error in height of bow, LcTo interpolate the cycle output chord length, the following equation is used:
Lc 2=8Herrri+4Herr 2
calculating the height error HerrThe chord length of (c) is as follows:
Figure BDA00025366743300002510
in the formula, Lc=VTinpo=ωiriTinpThen, then
Figure BDA00025366743300002511
If the ith positioner adjusts the attitude according to the allowable height error HerrThen, the rotational angular velocity ω of the rigid body is requirediMaximum, and bow height error HerrRadius r when constantiGreater allowable rigid body rotational angular velocity ωiThe smaller;
and solving the maximum radius in the space circular arc track radii of all the positioners as follows:
rmax=max(r1,r2,r3,…,ri,…,rN)
during interpolation, the interpolation period time TinpThe same angular speeds are the same when the rigid body fixed shaft rotates a plurality of circular arcs;
calculating the bow height error HerrRigid body winding meeting the requirements
Figure BDA0002536674330000262
Maximum rotational angular velocity, as follows:
Figure BDA0002536674330000263
s103, planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range which are allowed by the attitude adjustment of the large airplane component.
S1031, adjusting the maximum angular velocity omega required by the rigid body fixed shaft rotation structure strength according to the maximum value of the rigid body angular velocitymax=min(ωmax1max2)。
S1032, adjusting the maximum angular acceleration α allowed according to the airplane large componentmaxMaximum translational velocity vmaxMaximum translational acceleration amaxThen, considering omega of the bow height error requirementmax1Maximum angular velocity omega for adjusting rigid body fixed axis rotation structure strength requirementmax=min(ωmax1max2) Velocity v at the beginning and end of the set of posturess=ve0, acceleration a at the beginning and end of posture adjustments=aeRotation angle theta of rigid body fixed axis rotationeAnd the translational movement quantity S of the rigid body, respectively carrying out bell-shaped acceleration/deceleration rigid body composite motion speed planning calculation, and calculating the actual maximum acceleration a of each stage time and translational movementnowmaxActual maximum translational velocity vnowmaxActual maximum angular acceleration of rotation αnowmaxAnd the actual maximum angular velocity ωnowmaxAnd then carrying out rigid body composite motion speed planning time trimming.
A. And performing bell-shaped acceleration/deceleration rigid body composite motion speed planning calculation.
Rotation angle of rigid body around fixed axis: theta ═ fθ1(t);t∈[0,Tθ];θ∈[0,θe];
Rigid body translation distance: s ═ fs1(t);t∈[0,Ts];s∈[0,S];
And (3) according to bell-type acceleration/deceleration speed planning, respectively calculating the speed planning of translation increment and angle increment bell-type acceleration/deceleration as follows:
according to the translational movement quantity S and the maximum translational speed v of the rigid bodymaxMaximum translational acceleration amaxAnd translation plus acceleration jlThe method comprises the following steps of performing speed planning calculation in seven stages including an acceleration stage, a uniform acceleration stage, a deceleration stage, a uniform speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration stage; wherein:
the acceleration is calculated as follows:
Figure BDA0002536674330000261
wherein J is Jl
The acceleration is calculated as follows:
Figure BDA0002536674330000271
the velocity is calculated as follows:
Figure BDA0002536674330000272
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The translation movement amount is calculated as follows:
Figure BDA0002536674330000273
the translation speed is planned to be s ═ fs1(t),v=fv1(t),a=fa1(t),js=J(t);
According to bell type increasing/decreasing time T1s=T3s,T5s=T7sVelocity v at the beginning and end of the set of posturess=veAcceleration a at the beginning and end of the set-ups=ae0, and the acceleration and deceleration stages are mirror symmetric, resulting in T1s=T7s=T5s=T3s,T2s=T6s
The maximum speed and the maximum acceleration are limited as v in the safety range3≤vmax,Jt1≤amaxCalculating the acceleration stage time T1sTime T of uniform acceleration stage2sDecreasing acceleration stage time T3sTime T at uniform speed stage4sAcceleration and deceleration stage time T5sTime T of uniform deceleration stage6sTime T of deceleration stage7s
Calculated according to the speed planning formula, if general conditions exist
Figure BDA0002536674330000283
When v ismax≤JT1 2If there is no even acceleration and even deceleration section, T appears2s=T6s0; when the distance of translation is
Figure BDA0002536674330000284
In the mean time, without uniform velocity segment, T appears4s0; when the distance of translation is
Figure BDA0002536674330000285
If there is no uniform velocity section, uniform acceleration section and uniform deceleration section, T appears4s=0,T2s=T6s=0。
Calculating the actual maximum acceleration anowmax=jlT1sActual maximum velocity vnowmax=v3And total translational time Ts=T1s+T2s+T3s+T4s+T5s+T6s+T7s
The velocity schedule for rigid body dead axle rotational increments is similar to the velocity schedule for translational increments. Rotation angle theta according to rigid body fixed axis rotationeMaximum angular velocity ωmaxMaximum angular acceleration αmaxAnd angle of rotation plus acceleration jθThe method comprises the following steps of calculating speed planning in seven stages including an acceleration stage, a uniform acceleration stage, an acceleration reduction stage, a constant speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration reduction stage; wherein:
the angular acceleration is calculated as follows:
Figure BDA0002536674330000281
wherein J is Jθ
The angular acceleration is calculated as follows:
Figure BDA0002536674330000282
the angular velocity is calculated as follows:
Figure BDA0002536674330000291
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The rotation angle is calculated as follows:
Figure BDA0002536674330000292
similar to the translational velocity profile, the rotational velocity profile is jθ=J(t),θ=fθ1(t),ω=fω1(t),α=fα1(t)。
According to bell type increasing/decreasing time T=T,T=TEstablishing a piecewise function of the rotation angle and adding an acceleration J ═ J according to the angleθAngle of rotation and attitude increment thetaeAngular velocity ω of starting and ending of posture adjustments=ωe0, angular acceleration α of starting and ending of pose adjustments=αe0, and the acceleration and deceleration stages are mirror symmetric, resulting in T=T=T=T,T=T;T=T=T=T,T=T
Maximum speed and maximum acceleration in a safe rangeThe beam condition is ω3≤ωmax,Jt1≤αmaxCalculating the acceleration stage time TTime T of uniform acceleration stageDecreasing acceleration stage time TTime T at uniform speed stageAcceleration and deceleration stage time TTime T of uniform deceleration stageTime T of deceleration stage
Calculated according to the speed planning formula, if general conditions exist
Figure BDA0002536674330000293
When ω ismax≤JT1 2When there is no uniform acceleration and uniform deceleration section, T appears=T0; when in use
Figure BDA0002536674330000294
In the mean time, without uniform velocity segment, T appears0; when in use
Figure BDA0002536674330000295
If there is no uniform velocity section, uniform acceleration section and uniform deceleration section, T appears=0,T=T=0。
Calculating the actual maximum angular acceleration αnowmaxActual maximum angular velocity ωnowmaxAnd total time of rotation Tθ=T+T+T+T+T+T+T
B. And (5) carrying out rigid body composite motion speed planning time trimming.
Specifically, two motion time of bell-shaped acceleration/deceleration speed planning respectively carried out on rigid body fixed axis rotation and rigid body translation are trimmed to be interpolation period time TinpIntegral multiple, the translation time and the rotation time are adjusted to be equal, and the time of each stage after the time axis is adjusted and the actual maximum acceleration a of rigid translation after the time axis is adjusted are calculatednow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2max
Calculating the time of each stage after adjusting the time axis and the actual maximum acceleration a of rigid translationnow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2maxThe method specifically comprises the following steps:
the attitude adjusting speed and the acceleration of the airplane need to change smoothly all the time to avoid impact, if the total translation time T in the speed planning timesOr total time of rotation TθNot interpolating the period time TinpIntegral multiple of the above, the actual running time is different from the speed planning time, which results in the actual running speed of the last interpolation period being lower than the planning speed value, and therefore the total translation time T needs to be adjustedsOr total time of rotation TθRounded up to an interpolation period time TinpInteger multiple of (d) is as follows:
Figure BDA0002536674330000301
the rigid body translation and the rigid body dead axle rotation are synchronously carried out, and when the requirement is simultaneously started and finished, the translation time and the dead axle rotation time are adjusted to be the same time, as the following formula:
Tnow=Tnows=Tnowθ=max(Tnows,Tnowθ)
the time of each stage is adjusted proportionally as follows:
rigid body translation time adjustment proportion:
Figure BDA0002536674330000302
rigid body dead axle rotation time adjustment proportion:
Figure BDA0002536674330000303
T1s=T7s=T5s=T3s=T1sKnows,T2s=T6s=T2sKnows,T4s=T4sKnows
T=T=T=T=TKnowθ,T=T=TKnowθ,T=TKnowθ
translation distance S and rotation angle thetaeRemains unchanged, TnowsAnd TnowθThe time is prolonged, the time of each stage is prolonged, and the actual speed, the actual acceleration and the actual jerk are adjusted as follows:
adjusting the actual maximum speed of rigid translation and the actual maximum angular speed of rigid fixed shaft rotation:
Figure BDA0002536674330000304
Figure BDA0002536674330000305
adjusting the actual maximum acceleration of rigid translation and the actual maximum angular acceleration of rigid fixed shaft rotation:
Figure BDA0002536674330000311
Figure BDA0002536674330000312
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure BDA0002536674330000313
Figure BDA0002536674330000314
after the time, speed, acceleration and jerk of each stage are proportionally regulated, the translation amount and rotation angle of rigid body and fixed axle in each stage are not changed before regulation because of Knows≥1,KnowθNot less than 1, the actual maximum speed and maximum acceleration of rigid motion are reduced and still in the required range, and the adjusted speed gauge is obtainedThe following is drawn:
rigid translation: s ═ fs(t);v=fv(t);a=fa(T) where T ∈ [0, Tnow];s∈[0,S];
Rigid body dead axle rotates: theta ═ fθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe]。
And S104, according to the velocity planning of the rigid body compound motion, taking each locator supporting point as a mass point on the rigid body, calculating the maximum velocity and the maximum acceleration on each locator driving shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each locator driving shaft.
Specifically, each locator support point is used as a mass point on a rigid body, the rigid body performs synchronous superposition motion of fixed axis rotation and translation, inverse solution is performed by utilizing a reverse kinematics position, a space circular arc motion track, speed and acceleration of each locator drive shaft are solved, the maximum speed and the maximum acceleration of each locator drive shaft are calculated in a local coordinate system of the locator, and the speed and the acceleration of rigid body composite motion are adjusted according to the speed range and the acceleration range allowed by each locator drive shaft (namely the speed range and the acceleration range allowed by a drive motor on each locator drive shaft); maximum speed v of each shaft for X, Y, Z shafts of known ith positioner to run safelyixmax,viymax,vizmaxMaximum acceleration aixmax,aiymax,aizmaxThe realization process is as follows:
with the ith locator supporting point space arc CiEstablishing a new local coordinate system C with the center of the circle as the origin of coordinatesixyz, local coordinate system CiThe X, Y, Z axis of xyz is parallel to the localizer local coordinate system OiX, Y, Z axis of xyz;
the central angle in the space circular arc motion track is the angle theta of rigid rotation ═ fθ(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiTranslation distance s ═ f in xyzs(t);
Rigid translation direction vector
Figure BDA0002536674330000315
Wherein
Figure BDA0002536674330000316
Corresponding to a local coordinate system CiThe origin of xyz is in the localizer local coordinate system OiVector in xyz direction
Figure BDA0002536674330000317
Figure BDA0002536674330000318
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational position component in xyz is of the form:
fis(t)=[xis(t) yis(t) zis(t)]T
in the formula, xis(t)=uixfs(t),yis(t)=uiyfs(t),zis(t)=uizfs(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational velocity component in xyz is of the form:
fiv(t)=[xiv(t) yiv(t) ziv(t)]T
in the formula, xiv(t)=uixfv(t),yiv(t)=uiyfv(t0,ziv(t)=uizfv(t);
Local coordinate system O of positioneriThe maximum speed of X, Y, Z shaft translation process in xyz is as follows:
viSxmax=max(|xiv(t)|)=|uix|max(fv(t))=|uix|vnow2max
viSymax=max(|yiv(t)|)=|uiy|max(fv(t))=|uiy|vnow2max
viSzmax=max(|ziv(t)|)=|uiz|max(fv(t))=|uiz|vnow2max
local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational acceleration component in xyz is of the form:
fia(t)=[xia(t) yia(t) zia(t)]T
in the formula, xia(t)=uixfa(t),yia(t)=uiyfa(t),zia(t)=uizfa(t);
Local coordinate system O of positioneriThe maximum acceleration of X, Y, Z axis translation process in xyz is as follows:
aiSxmax=max(|xia(t)|)=|uix|max(fa(t))=|uix|anow2max
aiSymax=max(|yia(t)|)=|uiy|max(fa(t))=|uiy|anow2max
aiSzmax=max(|zia(t)|)=|uiz|max(fa(t))=|uiz|anow2max
rigid body local coordinate system O in rigid body fixed axis rotationlAxis of rotation of xyz
Figure BDA0002536674330000321
Rotation angle theta f of rigid body fixed axis rotationθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe];
Before adjusting the posture, the support point of the ith positioner is in the local rigid coordinate system OlPosition vector in xyz
Figure BDA0002536674330000322
I-th locator in rigid local coordinate system OlRadius of rotation in xyz
Figure BDA0002536674330000323
Circle center coordinate
Figure BDA0002536674330000324
Rigid body fixed axis rotation angle theta ═ fθ(t) rigid body rotation Rw,θThe following formula:
Figure BDA0002536674330000331
in the formula, sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ(t(,t∈[0,Tnow],θ∈[0,θe];
In the posture adjusting process, the support point of the ith positioner is in a rigid body local coordinate system OiThe position vector in xyz is
Figure BDA0002536674330000332
Rigid body rotation axis in local coordinate system CiIn xyz are
Figure BDA0002536674330000333
The support point of the ith positioner in the local coordinate system CiPosition C in xyzi(θ) is a function of the rotation angle θ, as follows:
Figure BDA0002536674330000334
Figure BDA0002536674330000335
the support point of the ith positioner in the local coordinate system CiPosition C in xyzi(theta) ofThe component forms are as follows:
Ci(θ)=[xi(θ) yi(θ) zi(θ)]T,xi(θ),yi(θ),zi(θ)
Cithe normal direction vector for any θ position is given by:
Figure BDA0002536674330000336
Figure BDA0002536674330000337
Cithe normal direction vector component for any θ position is of the form:
Figure BDA0002536674330000338
Figure BDA0002536674330000339
Cithe maximum absolute value of the axis component of the normal direction vector X, Y, Z at any θ position is given by:
xintmax=max(|xint(fθ(t))|)=max(|xin(θ)|)
yintmax=max(|yint(fθ(t))|)=max(|yin(θ)|)
zintmax=max(|zint(fθ(t))|)=max(|zin(θ)|)
the airplane is adjusted in posture once and the angle theta is rotatedeSmall, xin(θ),yin(θ),zin(θ),θ∈[0,θe]These are continuous functions in a closed interval, have the most value, generally in the interval end point and the function extreme point, solve xintmax,yintmax,zintmax
CiThe tangential direction vector at any θ position is given by:
Figure BDA0002536674330000341
wherein
Figure BDA0002536674330000342
Figure BDA0002536674330000343
CiThe tangential direction vector component at any θ position is of the form:
Figure BDA0002536674330000344
Figure BDA0002536674330000345
Cithe maximum absolute value of the axial component of the tangential direction vector X, Y, Z at any θ position is given by:
xiτtmax=max(|xiτt(fθ(t))|)=max(|x(θ)|)
yiτtmax=max(|yiτt(fθ(t))|)=max(|y(θ)|)
ziτtmax=max(|ziτt(fθ(t))|)=max(|z(θ)|)
the airplane is adjusted in posture once and the angle theta is rotatedeSmall, x(θ),y(θ),z(θ),θ∈[0,θe]These are continuous functions in a closed interval, with the maxima and minima being generally at the end points of the interval and the extreme points of the function. Solve to xiτtmax,yiτtmax,ziτtmax
The support point of the ith positioner in the local coordinate system CiLinear velocity v in xyz(t)=rifω(t);
The support point of the ith positioner in the local coordinate system CiMaximum linear velocity max (v) in xyz(t))=riωnow2max
The support point of the ith positioner in the local coordinate system CiSpeed of circular arc motion in xyz
Figure BDA0002536674330000346
The support point of the ith positioner in the local coordinate system CiThe circular arc motion velocity component in xyz is of the form:
fivτ(t)=[xivτ(t) yivτ(t) zivτ(t)]T
in the formula, xivτ(t)=v(t)xiτt(fθ(t)),yivτ(t)=v(t)yiτt(fθ(t)),zivτ(t)=v(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiThe time of the maximum linear velocity in the circular motion in xyz and the time when the vector component in each axial direction reaches the maximum value may not overlap, and the maximum linear velocity multiplied by the maximum value of each axial component of the direction vector is not less than the circular motion fivτ(t) maximum speed of each axis, as follows:
max(|xivτ(t)|)=max(v(t)|xiτt(fθ(t))|)≤max(v(t))max(|xiτt(fθ(t))|)
max(|yivτ(t)|)=max(v(t)|yiτt(fθ(t))|)≤max(v(t))max(|yiτt(fθ(t))|)
max(|zivτ(t)|)=max(v(t)|ziτt(fθ(t))|)≤max(v(t))max(|ziτt(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion speed fivτ(t) and translational velocity fiv(t) synchronous superposition speed, moment when the translational speed X, Y, Z shaft component reaches the maximum speed and circular motion speedX, Y, Z, the time when the axle component reaches the maximum speed may not overlap, the sum of the maximum speed of the axle component of the translational speed X, Y, Z and the maximum speed of the axle component of the circular arc motion speed X, Y, Z is larger than the actual maximum speed of the positioner X, Y, Z, if it is smaller than the speed range allowed by each driving axle, it is safe, otherwise, it reduces the speed of the rigid body compound motion, as follows:
vixtest≥max(v(t)|xiτt(fθ(t))|)+max(|xiv(t)|)≥max(|xivτ(t)+xiv(t)|)
viytest≥max(v(t)|yiτt(fθ(t))|)+max(|yiv(t)|)≥max(|yivτ(t)+yiv(t)|)
viztest≥max(v(t)|ziτt(fθ(t))|)+max(|ziv(t)|)≥max(|zivτ(t)+ziv(t)|)
in the formula, xivτ(t)+xiv(t) is the X-axis actual speed, yivτ(t)+yiv(t) is the actual speed of the Y-axis, zivτ(t)+ziv(t) is the Z-axis actual velocity.
vixtest=max(v(t))max(|xiτt(fθ(t))|)+max(|xiv(t)|)=riωnow2maxxiτtmax+|uix|vnow2max
viytest=max(v(t))max(|yiτt(fθ(t))|)+max(|yiv(t)|)=riωnow2maxyiτtmax+|uiy|vnow2max
viztest=max(v(t))max(|ziτt(fθ(t))|)+max(|ziv(t)|)=riωnow2maxziτtmax+|uiz|vnow2max
If v isixtest≤vixmaxIs provided with
Figure BDA0002536674330000351
Otherwise
Figure BDA0002536674330000352
If v isiytest≤viymaxIs provided with
Figure BDA0002536674330000353
Otherwise
Figure BDA0002536674330000354
If v isiztest≤vizmaxIs provided with
Figure BDA0002536674330000355
Otherwise
Figure BDA0002536674330000356
Ith positioner velocity adjustment factor
Figure BDA0002536674330000357
The support point of the ith positioner in the local coordinate system CiTangential acceleration f in xyziaτ(t)=rifα(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of tangential acceleration max (f) in xyziaτ(t))=riαnow2max
The support point of the ith positioner in the local coordinate system CiCircular arc tangential acceleration vector in xyz
Figure BDA0002536674330000358
Figure BDA0002536674330000359
The support point of the ith positioner in the local coordinate system CiThe circular arc tangential acceleration component in xyz is of the form:
a(t)=[xiaτ(t) yiaτ(t) ziaτ(t)]T
in the formula, xiaτ(t)=fiaτ(t)xiττ(fθ(t)),yiaτ(t)=fiaτ(t)yiτt(fθ(t)),ziaτ(t)=fiaτ(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiCentripetal acceleration f in xyzian(t)=rifω 2(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of centripetal acceleration max (f) in xyzian(t))=riωnow2max 2
The support point of the ith positioner in the local coordinate system CiCircular arc normal acceleration vector in xyz
Figure BDA0002536674330000361
Figure BDA0002536674330000362
The support point of the ith positioner in the local coordinate system CiThe circular arc normal acceleration component in xyz is of the form:
ain(t)=[xian(t) yian(t) zian(t)]T
in the formula, xiaθ(t)=fiaτ(t)xiτt(fθ(t))+fian(t)xint(fθ(t));yiaθ(t)=fiaτ(t)yiτt(fθ(t))+fian(t)yint(fθ(t));ziaθ(t)=fiaτ(t)ziτt(fθ(t))+fian(t)zint(fθ(t));
The support point of the ith positioner in the local coordinate system CiThe angular acceleration and angular velocity of the middle circular arc motion in xyz may not be maximized at the same time, and the X, Y, Z-axis normal component and tangential component may not be maximized at the same time, so the circular arc motionAcceleration a(t) X, Y, Z axis component maximum value is not more than maximum value of angular acceleration and angular velocity and each axis normal component and tangential component maximum value are calculated as follows:
max(|xiaθ(t)|)≤max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)
max(|yiaθ(t)|)≤max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)
max(|ziaθ(t)|)≤max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion acceleration a(t) and translational acceleration fia(t) the synchronous superimposed acceleration, because the moment when the shaft component of the translational acceleration X, Y, Z reaches the maximum speed and the moment when the shaft component of the circular arc motion acceleration X, Y, Z reaches the maximum speed may not overlap, the sum of the maximum value of the shaft component of the translational acceleration X, Y, Z and the maximum value of the shaft component of the circular arc motion acceleration X, Y, Z is greater than the actual maximum acceleration of the positioner X, Y, Z, if the sum is smaller than the allowable acceleration range of each driving shaft, the safety is ensured, otherwise, the acceleration and the angular speed of the rigid body composite motion are reduced, as follows:
aixtest≥max(|xiaθ(t)|)+max(|xia(t)|)≥max(|xiaθ(t)+xia(t)|)
aiytest≥max(|yiaθ(t)|)+max(|yia(t)|)≥max(|yiaθ(t)+yia(t)|)
aiztest≥max(|ziaθ(t)|)+max(|zia(t)|)≥max(|ziaθ(t)+zia(t)|)
in the formula, xiaθ(t)+xia(t) is the actual acceleration of the X-axis, yiaθ(t)+yia(t) is the actual addition of the Y axisSpeed, ziaθ(t)+zia(t) is the Z-axis actual acceleration;
aixtest=max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)+max(|xia(t)|)
=riαnow2maxxiτtmax+riωnow2max 2xintmax+|uix|anow2max
aiytest=max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)+max(|yia(t)|)
=riαnow2maxyiτtmax+riωnow2max 2yintmax+|uiy|anow2max
aiztest=max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)+max(|zia(t)|)
=riαnow2maxziτtmax+riωnow2max 2zintmax+|uiz|now2max
if aixtest≤aixmaxIs provided with
Figure BDA0002536674330000371
Otherwise
Figure BDA0002536674330000372
If aiytest≤aiymaxIs provided with
Figure BDA0002536674330000373
Otherwise
Figure BDA0002536674330000374
If aiztest≤aizmaxIs provided with
Figure BDA0002536674330000375
Otherwise
Figure BDA0002536674330000376
Acceleration adjustment coefficient of ith positioner
Figure BDA0002536674330000377
If it is
Figure BDA0002536674330000378
And is
Figure BDA0002536674330000379
The rotational angular velocity of the rigid body is reduced, the centripetal acceleration is reduced, and the adjustment is performed
Figure BDA00025366743300003710
Determining the maximum value of the speed regulating coefficient in the attitude regulating process of the airplane
Figure BDA00025366743300003711
Solving the maximum value of the acceleration regulating coefficient in the process of adjusting the attitude of the airplane
Figure BDA00025366743300003712
And adjusting the speed and the acceleration of rigid translation and fixed shaft rotation according to the speed and the acceleration adjusting coefficient in the attitude adjusting process of the airplane, as follows:
maximum speed of rigid translation and maximum angular speed of rigid fixed shaft rotation:
Figure BDA00025366743300003713
Figure BDA00025366743300003714
maximum acceleration of rigid translationAnd maximum angular acceleration of rigid body dead axle rotation:
Figure BDA00025366743300003715
Figure BDA00025366743300003716
the jerk of rigid translation and the jerk of rigid fixed axis rotation: j is a function ofl=jl2,jθ=jθ2
And S105, planning and finishing the rigid body compound motion speed again.
And (3) re-planning the speed of the rigid body translation as follows:
according to the maximum velocity v of rigid translationmaxMaximum acceleration amaxJerk jlVelocity v at the beginning and end of the set of posturess=veAcceleration a at the beginning and end of the set-ups=aeWhen the rigid translation movement amount S obtained in step S101 is 0, the ring-type acceleration/deceleration rigid translation velocity planning calculation is performed according to the velocity planning calculation method in step S103, and the actual maximum velocity v of the rigid translation is calculatednewmaxAnd the actual maximum acceleration anewmax
Recalculating translation run time TsEach stage time T1s,T2s,T3s,T4s,T5s,T6s,T7s(ii) a Wherein T is1s=T7s=T5s=T3s,T2s=T6s
The speed planning time is rounded as follows:
Figure BDA0002536674330000381
and (3) re-planning the speed of the rigid body dead axle rotation, as follows:
maximum angular velocity omega based on rigid body dead axle rotationmaxMaximum angular acceleration αmaxAngular jerk jθSpeed omega of starting and ending of posture adjustments=ωe0, acceleration α for start and end of stance turns=αeThe angular increment θ of the rigid body fixed axis rotation obtained in step S101 is 0ePerforming bell-shaped acceleration/deceleration rigid body fixed-axis rotation speed planning calculation according to the speed planning calculation method in step S103, and calculating the actual maximum angular speed omega of rigid body fixed-axis rotationnewmaxAnd actual maximum angular acceleration αnewmax
Recalculating rigid body dead axle rotation time TθEach stage having a time T,T,T,T,T,T,T(ii) a Wherein T is=T=T=T,T=T
The speed planning time is rounded as follows:
Figure BDA0002536674330000382
the rigid body translation and the rigid body fixed shaft rotation are synchronously carried out, and the translation time and the fixed shaft rotation time are adjusted to be the same time as follows:
Tnew=Tnews=Tnewθ=max(Tnews,Tnewθ)
wherein the time of each stage is proportionally adjusted as follows:
T1s=T7s=T5s=T3s=T1sKnews,T2s=T6s=T2sKnews,T4s=T4sKnews
T=T=T=T=TKnewθ,T=T=TKnewθ,T=TKnewθ
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000383
is just likeAdjusting the proportion of the body translation time;
Figure BDA0002536674330000384
rigid body fixed axis rotation time adjustment proportion;
adjusting the actual speed, the actual acceleration and the actual jerk as follows:
adjusting the actual maximum speed of rigid translation and the actual angular speed of rigid fixed shaft rotation:
Figure BDA0002536674330000385
Figure BDA0002536674330000386
adjusting the actual maximum acceleration of rigid translation and the actual angular acceleration of rigid fixed shaft rotation:
Figure BDA0002536674330000387
Figure BDA0002536674330000388
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure BDA0002536674330000391
Figure BDA0002536674330000392
obtaining an adjusted speed plan:
rigid translation: s ═ fs3(t);v=fv3(t);a=fa3(T) where T ∈ [0, Tnew];s∈[0,S];
Rigid body dead axle rotates: theta ═ fθ3(t);ω=fω3(t);α=fα3(T) where T ∈ [0, Tnew];θ∈[0,θe]。
The speed planning function after time adjustment not only meets the requirement of synchronous rotation and translation of the rigid fixed shaft, but also meets the limitation condition of the angular speed range of the bow height error in the attitude adjusting process, the limitation condition of the speed and the acceleration range of the large part of the airplane in the rigid attitude adjusting process, and the limitation condition of the speed and the acceleration range of the driving shaft of the positioner.
And S106, performing interpolation calculation according to a time division method according to the new speed plan of the rigid body compound motion, and outputting the three-axis instruction coordinate position of each locator.
Specifically, according to a new speed plan of rigid body compound motion, rigid body fixed axis rotation interpolation and rigid body translation interpolation are respectively carried out according to a time division method, the position of each locator supporting point in a global coordinate system is calculated after synchronous superposition, then the locator supporting point is converted into a local coordinate system of each locator, and a three-axis instruction coordinate position of each locator is output, and the implementation process is as follows:
rigid body local coordinate system OlPosition in global coordinate system before origin attitude adjustment of xyz
Figure BDA0002536674330000393
Local coordinate system O of positioneriLocation of origin of xyz in global coordinates
Figure BDA0002536674330000394
The position of the ith locator support point before attitude adjustment, including the position in the global coordinate system
Figure BDA0002536674330000395
In a rigid body local coordinate system OlPosition in xyz
Figure BDA0002536674330000396
And in the localizer local coordinate system OiPosition in xyz
Figure BDA0002536674330000397
The position of the ith locator support point after attitude adjustment is included in the rigid body local coordinate system OlPosition in xyz
Figure BDA0002536674330000398
Position in global coordinates
Figure BDA0002536674330000399
And in the localizer local coordinate system OiPosition in xyz
Figure BDA00025366743300003910
Calculating the interpolation position of the ith positioner supporting point attitude adjusting process as follows:
the rotation angle function of the rigid body fixed axis rotation is as follows:
θ=fθ3(t);ω=fω3(t);α=fα3(t);t∈[0,Tnew];θ∈[0,θe];
rigid body rotation axis in rigid body local coordinate system OlVector of xyz
Figure BDA00025366743300003911
The function of the amount of movement of the rigid translation is:
s=fs3(t);v=fv3(t);a=fa3(t);t∈[0,Tnew];s∈[0,S];
rigid translation direction vector
Figure BDA00025366743300003912
Solving the i-th locator supporting point in the local coordinate system O of the locatorixyz location function
Figure BDA0002536674330000401
The following formula:
Figure BDA0002536674330000402
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000403
for the location vector of the ith locator support point in the global coordinate systemAmount, as follows:
Figure BDA0002536674330000404
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000405
is the position of the origin of the rigid body local coordinate system in the global coordinate system in the pose adjusting process,
Figure BDA0002536674330000406
when the rotation and translation of the rigid body fixed shaft are synchronously superposed, the support point of the ith positioner is in the local coordinate system O of the positioneriThe position calculation formula for xyz is as follows:
Figure BDA0002536674330000407
in the formula (I), the compound is shown in the specification,
Figure BDA0002536674330000408
sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ3(t),t∈[0,Tnew],θ∈[0,θe];
the attitude adjusting process of the ith positioner supporting point is carried out in a local coordinate system O of the positioneriThe position component of xyz is of the form:
Figure BDA0002536674330000409
in the formula (I), the compound is shown in the specification,
Figure BDA00025366743300004010
in order to interpolate the output X-axis command coordinate position,
Figure BDA00025366743300004011
in order to interpolate the output Y-axis command coordinate position,
Figure BDA00025366743300004012
the Z-axis command coordinate position is output for interpolation.
The command position coordinate values of X, Y, Z of all the positioners in the attitude adjusting process are sequentially calculated in the way; in the formula Rw,θAnd fs3And (t) the relation between the rotation angle of the rigid fixed shaft and the translation quantity of the rigid translation is common data of all the positioners, so that the calculation is only needed once in each interpolation period. In the formula
Figure BDA00025366743300004013
Associated with the positioner, but not with the interpolation time t, only for each attitude-adjusting process
Figure BDA00025366743300004014
The calculation is required once and need not be repeated every interpolation period.
And S107, carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each locator, and outputting the actual position of each axis driver.
Because the perpendicularity error exists in the axial direction of three coordinates of the positioner, the processing error of each shaft guide rail causes the straightness error, and the conditions that the two guide rails of each shaft are not parallel and have the changes of bending curvature and bending rate exist, the space positioning error of the actual positioner supporting point after the compensation of the screw compensation needs to be measured besides the reverse clearance compensation and the screw compensation of the single shaft, so that the compensation is carried out.
And an error compensation table is established in advance before pose adjustment. The bidirectional screw compensation can be provided without a reverse clearance compensation table. The unidirectional screw compensation mode needs reverse clearance compensation and screw compensation.
Firstly, X, Y, Z uniaxial reverse clearance measurement and helical compensation error measurement of a local coordinate system of the positioner are carried out, and a uniaxial reverse clearance compensation data table and a uniaxial helical compensation data table are established. The single-shaft reverse clearance compensation data and the single-shaft spiral compensation data are provided, and spiral compensation and reverse compensation functions can be realized. Firstly, starting the functions of screw compensation and space compensation to prepare for space error measurement. And measuring the spatial position error of the supporting point of the locator in the moving process of the local coordinate system of the locator by utilizing equipment such as an online measuring laser tracker in the airplane attitude adjusting equipment.
The measurement method of this embodiment is to divide the effective movement space of the supporting point of the positioner into a plurality of small squares, the positioner controller gives a movement command to the positioner driving motor to make the supporting point reach the top of the square, and the laser tracker and other devices directly read the actual spatial position, measure the spatial position error and record the error in the three-dimensional error data table. Generally, the number of measuring points is not too large, otherwise, the measuring time is long, and the amount of stored data is large.
Therefore, step S107 specifically includes: and performing reverse clearance compensation and pitch error compensation of each axis according to the three-axis instruction coordinate position of each positioner, performing three-axis compensation processing according to spatial error data, and outputting the actual position of each axis driver, wherein the implementation process comprises the following steps:
1) the X, Y, Z axle instruction coordinate position of every locator is read, reverse clearance compensation and pitch error compensation of each axle are carried out, if at unipolar measuring point, reverse clearance compensation data and pitch error compensation data are directly read, if not at unipolar measuring point, linear interpolation is carried out according to the error value of two end points of the unipolar measuring interval, the unipolar pitch error of the unipolar measuring interval of compensation, plus the reverse clearance value.
I-th driver in interpolating output coordinate
Figure BDA0002536674330000411
Compensation of reverse clearance of each shaft and compensation of pitch error.
Figure BDA0002536674330000412
The X axis is at
Figure BDA0002536674330000413
The position corresponds to a spiral compensation and an interval compensation superposition value;
Figure BDA0002536674330000414
y axis is at
Figure BDA0002536674330000415
The position corresponds to a spiral compensation and an interval compensation superposition value;
Figure BDA0002536674330000416
z axis is at
Figure BDA0002536674330000417
The position corresponds to the additive values of the spiral compensation and the interval compensation.
2) Reading X, Y, Z axis instruction coordinate position of each locator, compensating spatial error, directly reading data for compensation if on the grid vertex of spatial error measurement, reading eight vertex error data of the grid for spatial linear interpolation if not on the grid vertex of spatial error measurement in a certain grid, and calculating the spatial error fitting the eight vertices of the grid.
I-th driver in interpolating output coordinate
Figure BDA0002536674330000418
Three-dimensional space compensation value corresponding to each axis
Figure BDA0002536674330000419
Figure BDA00025366743300004110
Interpolating output coordinates
Figure BDA00025366743300004111
A time X-axis spatial error compensation quantity;
Figure BDA00025366743300004112
interpolating output coordinates
Figure BDA00025366743300004113
A temporal Y-axis spatial error compensation amount;
Figure BDA0002536674330000421
interpolation transmissionGo out the coordinate
Figure BDA0002536674330000422
And (5) compensating the space error of the time Z axis.
3) And after the reverse clearance compensation, the pitch error compensation and the space error compensation of each shaft are carried out, the actual position of each shaft driver is output.
T-time interpolation coordinate of ith driver
Figure BDA0002536674330000423
After various error compensation calculations, outputting a position instruction of each servo drive shaft at the moment t:
Figure BDA0002536674330000424
the compensated position of the X servo driver;
Figure BDA0002536674330000425
position compensated by the Y servo driver;
Figure BDA0002536674330000426
the compensated position of the Z servo driver.
Error compensation calculations are performed for all drivers in turn. And finally, uniformly sending the compensated position instructions of all the driving shafts to each servo driver at the output moment of the interpolation period, thereby realizing the spatial position compensation and effectively improving the spatial position precision of each locator supporting point.
Those skilled in the art will appreciate that all or part of the steps in the method for implementing the above embodiments may be implemented by a program to instruct associated hardware, and the corresponding program may be stored in a computer-readable storage medium.
Example 2:
as shown in fig. 2, the present embodiment provides a three-coordinate positioner pose adjusting operation and control system, which is applied to the digital assembly of an aircraft, and the system includes a first solution module 201, a second solution module 202, a first planning and trimming module 203, an adjustment module 204, a second planning and trimming module 205, an interpolation calculation module 206, and a compensation module 207, and the specific functions of each module are as follows:
the first calculating module 201 is used for establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, and calculating the translational movement amount and the translational direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body in fixed-axis rotation according to the attitude adjusting instruction.
And the second calculating module 202 is configured to calculate a circle center and a radius of a spatial circular arc trajectory of each locator in the rigid body fixed axis rotation process by using each locator support point as a mass point on the rigid body according to a rotation axis vector of the rigid body fixed axis rotation, a rigid body rotation center position, and a current position of each locator support point, and calculate a corresponding circular arc angular velocity range and a corresponding rigid body angular velocity range according to an allowable error of each circular arc trajectory.
And the first planning and finishing module 203 is used for planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range which are allowed by the attitude adjustment of the large part of the airplane.
And the adjusting module 204 is configured to calculate the maximum speed and the maximum acceleration of each positioner driving shaft by using each positioner supporting point as a mass point on the rigid body according to the velocity plan of the rigid body compound motion, and adjust the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each positioner driving shaft.
And a second planning and trimming module 205, configured to, after adjusting the velocity and acceleration of the rigid body compound motion, plan and trim the velocity of the rigid body compound motion again.
And the interpolation calculation module 206 is configured to perform interpolation calculation according to a time division method according to the new velocity plan of the rigid body compound motion, and output a three-axis instruction coordinate position of each locator.
And the compensation module 207 is used for performing spatial compensation according to the three-axis instruction coordinate position and the spatial error data of each positioner and outputting the actual position of each axis driver.
The specific implementation of each module in this embodiment may refer to embodiment 1, which is not described herein any more; it should be noted that the system provided in this embodiment is only illustrated by the division of the functional modules, and in practical applications, the functions may be distributed by different functional modules according to needs, that is, the internal structure is divided into different functional modules to complete all or part of the functions described above.
Example 3:
as shown in fig. 3, the present embodiment provides a pose controller, which includes a processor 301, a memory 302 and a transmission unit 303, where the processor 301 is configured to provide calculation and control capabilities, the memory 302 stores a computer program, and when the processor 301 executes the computer program stored in the memory 302, the pose controller implements the three-coordinate locator pose controlling method of embodiment 1, as follows:
establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, and resolving a translational movement amount and a translational direction vector of the rigid body, and a rotation angle and a rotation axis vector of the rigid body fixed axis rotation according to an attitude adjusting instruction;
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, and calculating a corresponding circular arc angular velocity range and a rigid body angular velocity range according to the allowable error of each circular arc track;
planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and a rotation angular speed range, an angular acceleration range, a translation speed range and a translation acceleration range which are allowed by attitude adjustment of a large part of the airplane;
according to the velocity planning of the rigid body compound motion, taking each locator supporting point as a mass point on the rigid body, calculating the maximum velocity and the maximum acceleration on each locator driving shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
after the speed and the acceleration of the rigid body compound motion are adjusted, the rigid body compound motion speed is planned and maintained again;
according to the new speed plan of the rigid body compound motion, carrying out interpolation calculation according to a time segmentation method, and outputting a three-axis instruction coordinate position of each locator;
and carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each positioner, and outputting the actual position of each axis driver.
Example 4:
the present embodiment provides a storage medium, which is a computer-readable storage medium, and stores a computer program, and when the computer program is executed by a processor, the method for adjusting, attitude, and operation and control of a three-coordinate positioner of embodiment 1 is implemented as follows:
establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, and resolving a translational movement amount and a translational direction vector of the rigid body, and a rotation angle and a rotation axis vector of the rigid body fixed axis rotation according to an attitude adjusting instruction;
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, and calculating a corresponding circular arc angular velocity range and a rigid body angular velocity range according to the allowable error of each circular arc track;
planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and a rotation angular speed range, an angular acceleration range, a translation speed range and a translation acceleration range which are allowed by attitude adjustment of a large part of the airplane;
according to the velocity planning of the rigid body compound motion, taking each locator supporting point as a mass point on the rigid body, calculating the maximum velocity and the maximum acceleration on each locator driving shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
after the speed and the acceleration of the rigid body compound motion are adjusted, the rigid body compound motion speed is planned and maintained again;
according to the new speed plan of the rigid body compound motion, carrying out interpolation calculation according to a time segmentation method, and outputting a three-axis instruction coordinate position of each locator;
and carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each positioner, and outputting the actual position of each axis driver.
It should be noted that the computer readable storage medium of the present embodiment may be a computer readable signal medium or a computer readable storage medium or any combination of the two. A computer readable storage medium may be, for example, but not limited to, an electronic, magnetic, optical, electromagnetic, infrared, or semiconductor system, apparatus, or device, or any combination of the foregoing. More specific examples of the computer readable storage medium may include, but are not limited to: an electrical connection having one or more wires, a portable computer diskette, a hard disk, a Random Access Memory (RAM), a read-only memory (ROM), an erasable programmable read-only memory (EPROM or flash memory), an optical fiber, a portable compact disc read-only memory (CD-ROM), an optical storage device, a magnetic storage device, or any suitable combination of the foregoing. In the present embodiment, a computer readable storage medium may be any tangible medium that can contain, or store a program for use by or in connection with an instruction execution system, apparatus, or device. In this embodiment, however, a computer readable signal medium may comprise a propagated data signal with a computer readable program embodied therein, for example, in baseband or as part of a carrier wave. Such a propagated data signal may take many forms, including, but not limited to, electro-magnetic, optical, or any suitable combination thereof. A computer readable signal medium may also be any computer readable storage medium that is not a computer readable storage medium and that can communicate, propagate, or transport a program for use by or in connection with an instruction execution system, apparatus, or device. The computer program embodied on the computer readable storage medium may be transmitted using any appropriate medium, including but not limited to: electrical wires, optical cables, RF (radio frequency), etc., or any suitable combination of the foregoing.
The flowchart and block diagrams in the figures illustrate the architecture, functionality, and operation of possible implementations of methods, systems, and gesture controllers according to various embodiments described above. In this regard, each block in the flowchart or block diagrams may represent a module, segment, or portion of code, which comprises one or more executable instructions for implementing the specified logical function(s). It should also be noted that, in some alternative implementations, the functions noted in the block may occur out of the order noted in the figures. For example, two blocks shown in succession may, in fact, be executed substantially concurrently, or the blocks may sometimes be executed in the reverse order, depending upon the functionality involved. It will also be noted that each block of the block diagrams and/or flowchart illustration, and combinations of blocks in the block diagrams and/or flowchart illustration, can be implemented by special purpose hardware-based systems which perform the specified functions or acts, or combinations of special purpose hardware and computer instructions. The modules described in the above embodiments may be implemented by software or hardware.
The foregoing description is only exemplary of the preferred embodiments of the invention and is illustrative of the principles of the technology employed. It will be appreciated by those skilled in the art that the scope of the disclosure in the embodiments described above is not limited to the particular combination of features described above, and that other embodiments can be made by any combination of features described above or their equivalents without departing from the spirit of the disclosure. For example, the above features and (but not limited to) the features with similar functions disclosed in the above embodiments are mutually replaced to form the technical solution.
It will be understood by those skilled in the art that the present invention is not limited to the particular embodiments described above, but is capable of various obvious changes, rearrangements and substitutions as will now become apparent to those skilled in the art without departing from the scope of the invention. Therefore, although the present invention has been described in greater detail by the above embodiments, the present invention is not limited to the above embodiments, and may include other equivalent embodiments without departing from the spirit of the present invention, and the scope of the present invention is determined by the scope of the appended claims.

Claims (18)

1. A three-coordinate positioner posture adjusting operation and control method is applied to airplane digital assembly and is characterized by comprising the following steps:
establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, and resolving a translational movement amount and a translational direction vector of the rigid body, and a rotation angle and a rotation axis vector of the rigid body fixed axis rotation according to an attitude adjusting instruction;
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, and calculating a corresponding circular arc angular velocity range and a rigid body angular velocity range according to the allowable error of each circular arc track;
planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and a rotation angular speed range, an angular acceleration range, a translation speed range and a translation acceleration range which are allowed by attitude adjustment of a large part of the airplane;
according to the velocity planning of the rigid body compound motion, taking each locator supporting point as a mass point on the rigid body, calculating the maximum velocity and the maximum acceleration on each locator driving shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
after the speed and the acceleration of the rigid body compound motion are adjusted, the rigid body compound motion speed is planned and maintained again;
according to the new speed plan of the rigid body compound motion, carrying out interpolation calculation according to a time segmentation method, and outputting a three-axis instruction coordinate position of each locator;
and carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each positioner, and outputting the actual position of each axis driver.
2. The attitude adjusting, operation and control method of a three-coordinate positioner according to claim 1, wherein the establishing of the rigid body local coordinate system and the positioner local coordinate system of the large part of the aircraft specifically comprises:
establishing a global coordinate system Oxyz for a relative ground reference system;
establishing a rigid local coordinate system O for a large aircraft partlxyz, the X, Y, Z axial direction of the local rigid body coordinate system is parallel to the X, Y, Z axial direction of the global coordinate system, the rotation center of the local rigid body coordinate system is set as the origin of the global coordinate system, and the coordinate in the global coordinate system before the origin of the local coordinate system is adjusted to the attitude is Ol(px,py,pz)T
Establishing a locator local coordinate system O for the ith locatorixyz, the X, Y, Z axial direction of the local coordinate system of the positioner is the driving moving direction of the supporting point of the positioner along the X, Y, Z axis of the positioner, the origin of the local coordinate system of the positioner is the supporting point position after the X, Y, Z axis of the positioner returns to zero, and the coordinate of the origin of the local coordinate system of the ith positioner in the global coordinate system is Oi(oix,oiy,oiz)TThe coordinate of the ith locator supporting point in the global coordinate system is Pi(pix,piy,piz)T
3. The three-coordinate positioner pose adjusting operation and control method according to claim 1, wherein the calculation of the translation movement amount and the translation direction vector of the rigid body and the rotation angle and the rotation axis vector of the rigid body fixed axis rotation according to the pose adjusting instruction specifically comprises:
resolving the translational motion quantity of the rigid body as follows:
Figure FDA0002536674320000021
resolving the translation direction vector of the rigid body as follows:
Figure FDA0002536674320000022
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000023
firstly, rotating the rigid body around the Z axis by an angle A, then rotating the rigid body around the Y axis by an angle B, and finally rotating the rigid body around the X axis by an angle C, wherein the angle A is as follows:
Figure FDA0002536674320000024
wherein s1 ═ sin (a), c1 ═ cos (a), s2 ═ sin (b), c2 ═ cos (b), s3 ═ sin (c), c3 ═ cos (c);
resolving the rotation angle of the rigid body fixed shaft rotation, as follows:
Figure FDA0002536674320000025
solving a rotating shaft vector of the rigid body fixed shaft rotation, and adopting the following formula:
Figure FDA0002536674320000026
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000027
Figure FDA0002536674320000028
4. a three-coordinate locator attitude adjusting operation and control method according to claim 1, wherein the method specifically comprises the steps of calculating the center and radius of a spatial circular arc trajectory of each locator in the rigid body fixed axis rotation process by using each locator support point as a rigid body upper mass point according to a rotation axis vector of the rigid body fixed axis rotation, a rigid body rotation center position and the current position of each locator support point, and calculating the corresponding circular arc angular velocity range and rigid body angular velocity range according to each circular arc trajectory allowable error, and specifically comprises the following steps:
according to the rotating shaft vector of the rigid body fixed shaft rotation, the rigid body rotating center position and the current position of each locator supporting point, taking each locator supporting point as a rigid body upper mass point, and calculating the circle center and the radius of a space circular arc track of each locator in the rigid body fixed shaft rotation process, wherein the following formula is as follows:
Figure FDA0002536674320000031
Figure FDA0002536674320000032
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000033
is the circle center position of the spatial circular arc track of the ith positioner in the rotating process of the rigid body fixed shaft,
Figure FDA0002536674320000034
in the local rigid body coordinate system O before the orientation adjustment for the ith support point of the positionerlThe position in the xyz is determined by the position,
Figure FDA0002536674320000035
rotation axis vector for rigid body fixed axis rotation, riRadius of the spatial circular arc track of the ith positioner in the rigid body dead axle rotation process:
let TinpTo interpolate the cycle time, HerrFor error in height of bow, LcTo interpolate the cycle output chord length, the following equation is used:
Lc 2=8Herrri+4Herr 2
calculating the height error HerrThe chord length of (c) is as follows:
Figure FDA0002536674320000036
in the formula, Lc=VTinpo=ωiriTinpThen, then
Figure FDA0002536674320000037
If the ith positioner adjusts the attitude according to the allowable height error HerrThen, the rotational angular velocity ω of the rigid body is requirediMaximum, and bow height error HerrRadius r when constantiGreater allowable rigid body rotational angular velocity ωiThe smaller;
and solving the maximum radius in the space circular arc track radii of all the positioners as follows:
rmax=max(r1,r2,r3,…,ri,…,rN)
during interpolation, the interpolation period time TinpThe same angular speeds are the same when the rigid body fixed shaft rotates a plurality of circular arcs;
calculating the bow height error HerrRigid body winding meeting the requirements
Figure FDA0002536674320000038
Maximum rotational angular velocity, as follows:
Figure FDA0002536674320000039
5. the attitude-adjusting operation and control method of the three-coordinate positioner according to claim 1, wherein the rigid body composite motion speed planning and modification is performed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range which are allowed by the attitude adjustment of the large part of the airplane, and specifically comprises the following steps:
according to the maximum value of the angular velocity of the rigid body, the maximum angular velocity omega required by the strength of the rigid body fixed-axis rotating structure is adjustedmax=min(ωmax1,ωmax2);
Maximum angular acceleration α allowed by airplane large component attitude adjustmentmaxMaximum translational velocity vmaxMaximum translational acceleration amaxMaximum angular velocity omega required by strength of rigid body fixed-axis rotating structuremax=min(ωmax1,ωmax2) Velocity v at the beginning and end of the set of posturess=ve0, acceleration a at the beginning and end of posture adjustments=aeRotation angle theta of rigid body fixed axis rotationeAnd the translational movement quantity S of the rigid body, respectively carrying out bell-shaped acceleration/deceleration rigid body composite motion speed planning calculation, and calculating the actual maximum acceleration a of each stage time and translational movementnowmaxActual maximum translational velocity vnowmaxActual maximum angular acceleration of rotation αnowmaxAnd the actual maximum angular velocity ωnowmaxAnd then carrying out rigid body composite motion speed planning time trimming.
6. The attitude-adjusting operation and control method for a three-coordinate positioner according to claim 5, wherein the calculation of the rigid body composite motion speed plan for bell-type acceleration/deceleration specifically comprises:
according to the translational movement quantity S and the maximum translational speed v of the rigid bodymaxMaximum translational acceleration amaxAnd translation plus acceleration jlThe method comprises the following steps of performing speed planning calculation in seven stages including an acceleration stage, a uniform acceleration stage, a deceleration stage, a uniform speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration stage; wherein:
the acceleration is calculated as follows:
Figure FDA0002536674320000041
wherein J is Jl
The acceleration is calculated as follows:
Figure FDA0002536674320000042
the velocity is calculated as follows:
Figure FDA0002536674320000043
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The translation movement amount is calculated as follows:
Figure FDA0002536674320000051
the translation speed is planned to be s ═ fs1(t),v=fv1(t),a=fa1(t),js=J(t);
According to bell type increasing/decreasing time T1s=T3s,T5s=T7sVelocity v at the beginning and end of the set of posturess=veAcceleration a at the beginning and end of the set-ups=ae0, and the acceleration and deceleration stages are mirror symmetric, resulting in T1s=T7s=T5s=T3s,T2s=T6s
The maximum speed and the maximum acceleration are limited as v in the safety range3≤vmax,Jt1≤amaxCalculating the acceleration stage time T1sTime T of uniform acceleration stage2sDecreasing acceleration stage time T3sTime T at uniform speed stage4sAcceleration and deceleration stage time T5sTime T of uniform deceleration stage6sTime T of deceleration stage7s
Calculating the actual maximum acceleration anowmax=jlT1sActual maximum velocity vnowmax=v3And total translational time Ts=T1s+T2s+T3s+T4s+T5s+T6s+T7s
Rotation angle theta according to rigid body fixed axis rotationeMaximum angular velocity ωmaxMaximum angular acceleration αmaxAnd angle of rotation plus acceleration jθThe method comprises the following steps of calculating speed planning in seven stages including an acceleration stage, a uniform acceleration stage, an acceleration reduction stage, a constant speed stage, an acceleration and deceleration stage, a uniform deceleration stage and a deceleration reduction stage; wherein:
the angular acceleration is calculated as follows:
Figure FDA0002536674320000052
wherein J is Jθ
The angular acceleration is calculated as follows:
Figure FDA0002536674320000061
the angular velocity is calculated as follows:
Figure FDA0002536674320000062
in the formula, T1=t1,T2=t2-t1,T3=t3-t2;T4=t4-t3,T5=t5-t4,T6=t6-t5;T7=t7-t6,T1=T3,T5=T7
The rotation angle is calculated as follows:
Figure FDA0002536674320000063
speed planning of a rotationIs jθ=J(t),θ=fθ1(t),ω=fω1(t),α=fα1(t);
According to bell type increasing/decreasing time T=T,T=TEstablishing a piecewise function of the rotation angle and adding an acceleration J ═ J according to the angleθAngle of rotation and attitude increment thetaeAngular velocity ω of starting and ending of posture adjustments=ωe0, angular acceleration α of starting and ending of pose adjustments=αe0, and the acceleration and deceleration stages are mirror symmetric, resulting in T=T=T=T,T=T;T=T=T=T,T=T
The maximum speed and the maximum acceleration are limited to be omega in a safety range3≤ωmax,Jt1≤αmaxCalculating the acceleration stage time TTime T of uniform acceleration stageDecreasing acceleration stage time TTime T at uniform speed stageAcceleration and deceleration stage time TTime T of uniform deceleration stageTime T of deceleration stage
Calculating the actual maximum angular acceleration αnowmaxActual maximum angular velocity ωnowmaxAnd total time of rotation Tθ=T+T+T+T+T+T+T
7. The three-coordinate positioner pose adjusting, operation and control method according to claim 5, wherein the rigid body composite motion speed planning time shaping specifically comprises:
two motion time trimming to interpolation period time T for bell-type acceleration/deceleration speed planning of rigid body fixed axis rotation and rigid body translation respectivelyinpIntegral multiple, the translation time and the rotation time are adjusted to be equal, and the time of each stage after the time axis is adjusted and the actual maximum acceleration of rigid translation are calculatedanow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2max
8. The attitude adjusting operation and control method for the three-coordinate positioner according to claim 7, wherein the time of each stage after the time axis is adjusted and the actual maximum acceleration a of the rigid translation are calculatednow2maxActual maximum velocity v of rigid translationnow2maxActual maximum angular acceleration α of rigid body fixed axis rotationnow2maxActual maximum angular velocity omega of rigid body fixed axis rotationnow2maxThe method specifically comprises the following steps:
total translational time TsOr total time of rotation TθRounded up to an interpolation period time TinpInteger multiple of (d) is as follows:
Figure FDA0002536674320000071
the rigid body translation and the rigid body dead axle rotation are synchronously carried out, and when the requirement is simultaneously started and finished, the translation time and the dead axle rotation time are adjusted to be the same time, as the following formula:
Tnow=Tnows=Tnowθ=max(Tnows,Tnowθ)
the time of each stage is adjusted proportionally as follows:
rigid body translation time adjustment proportion:
Figure FDA0002536674320000072
rigid body dead axle rotation time adjustment proportion:
Figure FDA0002536674320000073
T1s=T7s=T5s=T3s=T1sKnows,T2s=T6s=T2sKnows,T4s=T4sKnows
T=T=T=T=TKnowθ,T=T=TKnowθ,T=TKnowθ
translation distance S and rotation angle thetaeRemains unchanged, TnowsAnd TnowθThe time is prolonged, the time of each stage is prolonged, and the actual speed, the actual acceleration and the actual jerk are adjusted as follows:
adjusting the actual maximum speed of rigid translation and the actual maximum angular speed of rigid fixed shaft rotation:
Figure FDA0002536674320000074
Figure FDA0002536674320000075
adjusting the actual maximum acceleration of rigid translation and the actual maximum angular acceleration of rigid fixed shaft rotation:
Figure FDA0002536674320000076
Figure FDA0002536674320000081
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure FDA0002536674320000082
Figure FDA0002536674320000083
after the time, speed, acceleration and jerk of each stage are adjusted in proportion, the rigid translation movement amount and the rigid fixed axis rotation angle of each stage are kept unchanged with the speed before adjustment, and the adjusted speed is planned as follows:
rigid bodyTranslation: s ═ fs(t);v=fv(t);a=fa(T) where T ∈ [0, Tnow];s∈[0,s]
Rigid body dead axle rotates: theta ═ fθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe]。
9. The three-coordinate positioner attitude adjusting operation and control method according to claim 1, wherein the method comprises, according to a velocity plan of rigid body compound motion, using each positioner support point as a mass point on a rigid body, calculating a maximum velocity and a maximum acceleration on each positioner drive shaft, and adjusting the velocity and the acceleration of the rigid body compound motion according to a velocity range and an acceleration range allowed by each positioner drive shaft, specifically comprising:
and taking each locator support point as a mass point on the rigid body, carrying out synchronous superposition motion of fixed axis rotation and translation on the rigid body, solving a space circular arc motion track, a speed and an acceleration of each locator drive shaft by utilizing inverse kinematics position inverse solution, calculating the maximum speed and the maximum acceleration on each locator drive shaft in a locator local coordinate system, and adjusting the speed and the acceleration of rigid body composite motion according to the speed range and the acceleration range allowed by each locator drive shaft.
10. A three-coordinate positioner attitude adjusting operation and control method according to claim 9, wherein each positioner support point is used as a rigid body upper mass point, the rigid body performs synchronous superimposed motion of fixed axis rotation and translation, a space circular arc motion track, speed and acceleration of each positioner drive shaft are solved by inverse kinematics position inverse solution, the maximum speed and the maximum acceleration of each positioner drive shaft are calculated in a positioner local coordinate system, and the speed and the acceleration of rigid body composite motion are adjusted according to the speed range and the acceleration range allowed by each positioner drive shaft, specifically comprising:
with the ith locator supporting point space arc CiEstablishing a new local coordinate system C with the center of the circle as the origin of coordinatesixyz, local coordinate system CiThe X, Y, Z axis of xyz is parallel to the localizer local coordinate system OiX, Y, Z axis of xyz;
the central angle in the space circular arc motion track is the angle theta of rigid rotation ═ fθ(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiTranslation distance s ═ f in xyzs(t);
Rigid translation direction vector
Figure FDA0002536674320000087
Wherein
Corresponding to a local coordinate system CiThe origin of xyz is in the localizer local coordinate system OiVector in xyz direction
Figure FDA0002536674320000085
Figure FDA0002536674320000086
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational position component in xyz is of the form:
fis(t)=[xis(t) yis(t) zis(t)]T
in the formula, xis(t)=uixfs(t),yis(t)=uiyfs(t),zis(t)=uizfs(t);
Local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational velocity component in xyz is of the form:
fiv(t)=[xiv(t) yiv(t) ziv(t)]T
in the formula, xiv(t)=uixfv(t),yiv(t)=uiyfv(t),ziv(t)=uizfv(t);
Local coordinate system O of positioneriThe maximum speed of X, Y, Z shaft translation process in xyz is as follows:
viSxmax=max(|xiv(t)|)=|uix|max(fv(t))=|uix|vnow2max
viSymax=max(|yiv(t)|)=|uiy|max(fv(t))=|uiy|vnow2max
viSzmax=max(|ziv(t)|)=|uiz|max(fv(t))=|uiz|vnow2max
local coordinate system C in rigid body translation processiThe origin of xyz is in the localizer local coordinate system OiThe translational acceleration component in xyz is of the form:
fia(t)=[xia(t) yia(t) zia(t)]T
in the formula, xia(t)=uixfa(t),yia(t)=uiyfa(t),zia(t)=uizfa(t);
Local coordinate system O of positioneriThe maximum acceleration of X, Y, Z axis translation process in xyz is as follows:
aiSxmax=max(|xia(t)|)=|uix|max(fa(t))=|uix|anow2max
aiSymax=max(|yia(t)|)=|uiy|max(fa(t))=|uiy|anow2max
aiSzmax=max(|zia(t)|)=|uiz|max(fa(t))=|uiz|anow2max
rigid body local coordinate system O in rigid body fixed axis rotationlAxis of rotation of xyz
Figure FDA0002536674320000092
Rotation angle theta f of rigid body fixed axis rotationθ(t);ω=fω(t);α=fα(T) where T ∈ [0, Tnow];θ∈[0,θe];
Before adjusting the posture, the support point of the ith positioner is in the local rigid coordinate system OlPosition vector in xyz
Figure FDA0002536674320000093
I-th locator in rigid local coordinate system OlRadius of rotation in xyz
Figure FDA0002536674320000094
Circle center coordinate
Figure FDA0002536674320000091
Rigid body fixed axis rotation angle theta ═ fθ(t) rigid body rotation Rw,θThe following formula:
Figure FDA0002536674320000101
in the formula, sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ(t),t∈[0,Tnow],θ∈[0,θe](ii) a In the posture adjusting process, the support point of the ith positioner is in a rigid body local coordinate system OlThe position vector in xyz is
Figure FDA00025366743200001011
Rigid body rotation axis in local coordinate system CiIn xyz are
Figure FDA00025366743200001012
The support point of the ith positioner in the local coordinate system CiPosition C in xyzi(θ) is a function of the rotation angle θ, as follows:
Figure FDA0002536674320000102
Figure FDA0002536674320000103
the support point of the ith positioner in the local coordinate system CiPosition C in xyziThe component form of (θ) is as follows:
Ci(θ)=[xi(θ) yi(θ) zi(θ)]T,xi(θ),yi(θ),zi(θ)
Cithe normal direction vector for any θ position is given by:
Figure FDA0002536674320000104
Figure FDA0002536674320000105
Cithe normal direction vector component for any θ position is of the form:
Figure FDA0002536674320000106
Figure FDA0002536674320000107
Cithe maximum absolute value of the axis component of the normal direction vector X, Y, Z at any θ position is given by:
xintmax=max(|xint(fθ(t))|)=max(|xin(θ)|)
yintmax=max(|yint(fθ(t))|)=max(|yin(θ)|)
zintmax=max(|zint(fθ(t))|)=max(|zin(θ)|)
Cithe tangential direction vector at any θ position is given by:
Figure FDA0002536674320000108
wherein
Figure FDA0002536674320000109
Figure FDA00025366743200001010
CiThe tangential direction vector component at any θ position is of the form:
Figure FDA0002536674320000111
Figure FDA0002536674320000112
Cithe maximum absolute value of the axial component of the tangential direction vector X, Y, Z at any θ position is given by:
xiτtmax=max(|xiτt(fθ(t))|)=max(|x(θ)|)
yiτtmax=max(|yiτt(fθ(t))|)=max(|y(θ)|)
ziτtmax=max(|ziτt(fθ(t))|)=max(|z(θ)|)
the support point of the ith positioner in the local coordinate system CiLinear velocity v in xyz(t)=rifω(t);
The support point of the ith positioner in the local coordinate system CiMaximum linear velocity max (v) in xyz(t))=riωnow2max
The support point of the ith positioner in the local coordinate system CiSpeed of circular arc motion in xyz
Figure FDA0002536674320000113
The support point of the ith positioner in the local coordinate system CiThe circular arc motion velocity component in xyz is of the form:
fivτ(t)=[xivτ(t) yivτ(t) zivτ(t)]T
in the formula, xivτ(t)=v(t)xiτt(fθ(t)),yivτ(t)=v(t)yiτt(fθ(t)),zivτ(t)=v(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiThe maximum linear velocity of the circular arc motion in xyz multiplied by the maximum value of each axial component of the direction vector is not less than the circular arc motion fivτ(t) maximum speed of each axis, as follows:
max(|xivτ(t)|)=max(v(t)|xiτt(fθ(t))|)≤max(v(t))max(|xiτt(fθ(t))|)
max(|yivτ(t)|)=max(v(t)|yiτt(fθ(t))|)≤max(v(t))max(|yiτt(fθ(t))|)
max(|zivτ(t)|)=max(v(t)|ziτt(fθ(t))|)≤max(v(t))max(|ziτt(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion speed fivτ(t) and translational velocity fiv(t) the sum of the synchronous superposition speed, the maximum speed of the shaft component of the translational speed X, Y, Z and the maximum speed of the shaft component of the circular motion speed X, Y, Z is greater than the actual maximum speed of the positioner X, Y, Z, if the sum is less than the allowable speed range of each driving shaft, the safety is ensured, otherwise, the speed of the rigid body compound motion is reduced, and the method comprises the following steps:
vixtest≥max(v(t)|xiτt(fθ(t))|)+max(|xiv(t)|)≥max(|xivτ(t)+xiv(t)|)
viytest≥max(v(t)|yiτt(fθ(t))|)+max(|yiv(t)|)≥max(|yivτ(t)+yiv(t)|)
viztest≥max(v(t)|ziτt(fθ(t))|)+max(|ziv(t)|)≥max(|zivτ(t)+ziv(t)|)
in the formula, xivτ(t)+xiv(t) is the X-axis actual speed, yivτ(t)+yiv(t) is the actual speed of the Y-axis, zivτ(t)+ziv(t) is the Z-axis actual speed;
vixtest=max(v(t))max(|xiτt(fθ(t))|)+max(|xiv(t)|)=riωnow2maxxiτtmax+|uix|vnow2max
viytest=max(v(t))max(|yiτt(fθ(t))|)+max(|yiv(t)|)=riωnow2maxyiτtmax+|uiy|vnow2max
viztest=max(v(t))max(|ziτt(fθ(t))|)+max(|ziv(t)|)=riωnow2maxziτtmax+|uiz|vnow2max
if v isixtest≤vixmaxIs provided with
Figure FDA0002536674320000124
Otherwise
Figure FDA0002536674320000121
If v isiytest≤viymaxIs provided with
Figure FDA0002536674320000125
Otherwise
Figure FDA0002536674320000122
If v isiztest≤vizmaxIs provided with
Figure FDA0002536674320000126
Otherwise
Figure FDA0002536674320000123
Ith positioner velocity adjustment factor
Figure FDA0002536674320000127
The support point of the ith positioner in the local coordinate system CiTangential acceleration f in xyziaτ(t)=rifα(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of tangential acceleration max (f) in xyziaτ(t))=riαnow2max
The support point of the ith positioner in the local coordinate system CiCircular arc tangential acceleration vector in xyz
Figure FDA0002536674320000128
Figure FDA0002536674320000129
The support point of the ith positioner in the local coordinate system CiThe circular arc tangential acceleration component in xyz is of the form:
a(t)=[xiaτ(t) yiaτ(t) ziaτ(t)]T
in the formula, xiaτ(t)=fiaτ(t)xiτt(fθ(t)),yiaτ(t)=fiaτ(t)yiτt(fθ(t)),ziaτ(t)=fiaτ(t)ziτt(fθ(t));
The support point of the ith positioner in the local coordinate system CiCentripetal acceleration f in xyzian(t)=rifω 2(t);
The support point of the ith positioner in the local coordinate system CiMaximum value of centripetal acceleration max (f) in xyzian(t))=riωnow2max 2
The support point of the ith positioner in the local coordinate system CiCircular arc normal acceleration vector in xyz
Figure FDA00025366743200001210
Figure FDA00025366743200001211
The support point of the ith positioner in the local coordinate system CiThe circular arc normal acceleration component in xyz is of the form:
ain(t)=[xian(t) yian(t) zian(t)]T
in the formula, xiaθ(t)=fiaτ(t)xiτt(fθ(t))+fian(t)xint(fθ(t));yiaθ(t)=fiaτ(t)yiτt(fθ(t))+fian(t)yint(fθ(t));ziaθ(t)=fiaτ(t)ziτt(fθ(t))+fian(t)zint(fθ(t));
The support point of the ith positioner in the local coordinate system CiCircular arc motion acceleration a in xyz(t) X, Y, Z axis component maximum value is not more than maximum value of angular acceleration and angular velocity and each axis normal component and tangential component maximum value are calculated as follows:
max(|xiaθ(t)|)≤max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)
max(|yiaθ(t)|)≤max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)
max(|ziaθ(t)|)≤max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)
the support point of the ith positioner is in the local coordinate system O of the positioneriThe motion speed in xyz is the circular motion acceleration a(t) and translational acceleration fia(t) the sum of the synchronous superimposed acceleration, the maximum value of the shaft component of the translational acceleration X, Y, Z and the maximum value of the shaft component of the circular arc motion acceleration X, Y, Z is greater than the actual maximum acceleration of the positioner X, Y, Z, if the sum is smaller than the allowable acceleration range of each driving shaft, the safety is ensured, otherwise, the acceleration and the angular speed of the rigid body composite motion are reduced, and the method comprises the following steps:
aixtest≥max(|xiaθ(t)|)+max(|xia(t)|)≥max(|xiaθ(t)+xia(t)|)
aiytest≥max(|yiaθ(t)|)+max(|yia(t)|)≥max(|yiaθ(t)+yia(t)|)
aiztest≥max(|ziaθ(t)|)+max(|zia(t)|)≥max(|ziaθ(t)+zia(t)|)
in the formula, xiaθ(t)+xia(t) is the actual acceleration of the X-axis, yiaθ(t)+yia(t) is the actual acceleration of the Y-axis, ziaθ(t)+zia(t) is the Z-axis actual acceleration;
aixtest=max(fiaτ(t))max(|xiτt(fθ(t))|)+max(fian(t))max(|xint(fθ(t))|)+max(|xia(t)|)
=riαnow2maxxiτtmax+riωnow2nax 2xintmax+|uix|anow2max
aiytest=max(fiaτ(t))max(|yiτt(fθ(t))|)+max(fian(t))max(|yint(fθ(t))|)+max(|yia(t)|)
=riαnow2maxyiτtmax+riωnow2max 2yintmax+|uiy|anow2max
aiztest=max(fiaτ(t))max(|ziτt(fθ(t))|)+max(fian(t))max(|zint(fθ(t))|)+max(|zia(t)|)
=riαnow2maxziτtmax+riωnow2max 2zintmax+|uiz|anow2max
if aixtest≤aixmaxIs provided with
Figure FDA0002536674320000135
Otherwise
Figure FDA0002536674320000131
If aiytest≤aiymaxIs provided with
Figure FDA0002536674320000136
Otherwise
Figure FDA0002536674320000132
If aiztest≤aizmaxIs provided with
Figure FDA0002536674320000137
Otherwise
Figure FDA0002536674320000133
Acceleration adjustment coefficient of ith positioner
Figure FDA0002536674320000138
If it is
Figure FDA0002536674320000139
And is
Figure FDA0002536674320000134
The rotational angular velocity of the rigid body is reduced, the centripetal acceleration is reduced, and the adjustment is performed
Figure FDA0002536674320000141
Determining the maximum value of the speed regulating coefficient in the attitude regulating process of the airplane
Figure FDA0002536674320000142
Solving the maximum value of the acceleration regulating coefficient in the process of adjusting the attitude of the airplane
Figure FDA0002536674320000143
And adjusting the speed and the acceleration of rigid translation and fixed shaft rotation according to the speed and the acceleration adjusting coefficient in the attitude adjusting process of the airplane, as follows:
maximum speed of rigid translation and maximum angular speed of rigid fixed shaft rotation:
Figure FDA0002536674320000144
Figure FDA0002536674320000145
maximum acceleration of rigid translation and maximum angular acceleration of rigid fixed axis rotation:
Figure FDA0002536674320000146
Figure FDA0002536674320000147
rigid translation acceleration and rigid fixed axis rotation acceleration:jl=jl2,jθ=jθ2
11. The three-coordinate positioner pose adjusting operation and control method according to claim 1, wherein the planning and the trimming of the rigid body compound motion speed are performed again, and specifically the method comprises the following steps:
and (3) re-planning the speed of the rigid body translation as follows:
according to the maximum velocity v of rigid translationmaxMaximum acceleration amaxJerk jlVelocity v at the beginning and end of the set of posturess=veAcceleration a at the beginning and end of the set-ups=aeWhen the rigid translation movement quantity S is equal to 0, the ring-type acceleration/deceleration rigid translation speed planning calculation is carried out, and the actual maximum speed v of the rigid translation is calculatednewmaxAnd the actual maximum acceleration anewmax
Recalculating translation run time TsEach stage time T1s,T2s,T3s,T4s,T5s,T6s,T7s(ii) a Wherein T is1s=T7s=T5s=T3s,T2s=T6s
The speed planning time is rounded as follows:
Figure FDA0002536674320000148
and (3) re-planning the speed of the rigid body dead axle rotation, as follows:
maximum angular velocity omega based on rigid body dead axle rotationmaxMaximum angular acceleration αmaxAngular jerk jθSpeed omega of starting and ending of posture adjustments=ωe0, acceleration α for start and end of stance turns=αeAngle increment theta of rigid body fixed axis rotationePerforming bell-shaped acceleration/deceleration planning calculation on the rotation speed of the rigid body fixed shaft to calculate the actual maximum angular speed omega of the rigid body fixed shaft rotationnewmaxAnd maximum angular acceleration αnewmax
Recalculating rigid body dead axle rotation time TθEach stage having a time T,T,T,T,T,T,T(ii) a Wherein T is=T=T=T,T=T
The speed planning time is rounded as follows:
Figure FDA0002536674320000151
the rigid body translation and the rigid body fixed shaft rotation are synchronously carried out, and the translation time and the fixed shaft rotation time are adjusted to be the same time as follows:
Tnew=Tnews=Tnewθ=max(Tnews,Tnewθ)
wherein the time of each stage is proportionally adjusted as follows:
T1s=T7s=T5s=T3s=T1sKnews,T2s=T6s=T2sKnews,T4s=T4sKnews
T=T=T=T=TKnewθ,T=T=TKnewθ,T=TKnewθ
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000152
adjusting the proportion of rigid translation time;
Figure FDA0002536674320000153
rigid body fixed axis rotation time adjustment proportion;
adjusting the actual speed, the actual acceleration and the actual jerk as follows:
rigid translationAdjusting the actual maximum speed and the actual angular speed of the rotation of the rigid body fixed shaft:
Figure FDA0002536674320000154
Figure FDA0002536674320000155
adjusting the actual maximum acceleration of rigid translation and the actual angular acceleration of rigid fixed shaft rotation:
Figure FDA0002536674320000156
Figure FDA0002536674320000157
the actual jerk of rigid translation and the actual jerk of rigid fixed axis rotation are adjusted:
Figure FDA0002536674320000158
Figure FDA0002536674320000159
obtaining an adjusted speed plan:
rigid translation: s ═ fs3(t);v=fv3(t);a=fa3(T) where T ∈ [0, Tnew];s∈[0,S];
Rigid body dead axle rotates: theta ═ fθ3(t);ω=fω3(t);α=fα3(T) where T ∈ [0, Tnew];θ∈[0,θe]。
12. A three-coordinate locator attitude-adjusting operation and control method according to any one of claims 1 to 11, wherein the interpolation calculation is performed according to a time division method according to a new velocity plan of rigid body compound motion, and a three-axis command coordinate position of each locator is output, specifically comprising:
according to the new speed plan of rigid body composite motion, rigid body fixed axis rotation interpolation and rigid body translation interpolation are respectively carried out according to a time division method, the position of each locator supporting point in a global coordinate system is calculated after synchronous superposition, then the locator supporting point is converted into a local coordinate system of each locator, and the three-axis instruction coordinate position of each locator is output.
13. A three-coordinate locator attitude-adjusting operation and control method according to claim 12, wherein the rigid body fixed-axis rotation interpolation and the rigid body translation interpolation are respectively performed according to a time division method according to a new speed plan of rigid body compound motion, the position of each locator support point in a global coordinate system is calculated after synchronous superposition, then the position is converted into a local coordinate system of each locator, and a three-axis instruction coordinate position of each locator is output, specifically comprising:
rigid body local coordinate system OlPosition in global coordinate system before origin attitude adjustment of xyz
Figure FDA0002536674320000161
Local coordinate system O of positioneriLocation of origin of xyz in global coordinates
Figure FDA0002536674320000162
The position of the ith locator support point before attitude adjustment, including the position in the global coordinate system
Figure FDA0002536674320000163
In a rigid body local coordinate system OlPosition in xyz
Figure FDA0002536674320000164
And in the localizer local coordinate system OiPosition in xyz
Figure FDA0002536674320000165
The position of the ith locator support point after attitude adjustment is included in the rigid body local coordinate system OlPosition in xyz
Figure FDA0002536674320000166
Position in global coordinates
Figure FDA0002536674320000167
And in the localizer local coordinate system OiPosition in xyz
Figure FDA0002536674320000168
Calculating the interpolation position of the ith positioner supporting point attitude adjusting process as follows:
the rotation angle function of the rigid body fixed axis rotation is as follows:
θ=fθ3(t);ω=fω3(t);α=fα3(t);t∈[0,Tnew];θ∈[0,θe];
rigid body rotation axis in rigid body local coordinate system OlVector of xyz
Figure FDA00025366743200001612
The function of the amount of movement of the rigid translation is:
s=fs3(t);v=fv3(t);a=fa3(t);t∈[0,Tnew];s∈[0,S];
rigid translation direction vector
Figure FDA0002536674320000169
Solving the i-th locator supporting point in the local coordinate system O of the locatorixyz location function
Figure FDA00025366743200001613
The following formula:
Figure FDA00025366743200001610
in the formula (I), the compound is shown in the specification,
Figure FDA00025366743200001614
for the position vector of the ith localizer support point in the global coordinate system, the following equation is used:
Figure FDA00025366743200001611
in the formula (I), the compound is shown in the specification,
Figure FDA00025366743200001615
is the position of the origin of the rigid body local coordinate system in the global coordinate system in the pose adjusting process,
Figure FDA0002536674320000171
when the rotation and translation of the rigid body fixed shaft are synchronously superposed, the support point of the ith positioner is in the local coordinate system O of the positioneriThe position calculation formula for xyz is as follows:
Figure FDA0002536674320000172
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000173
sθ=sin(θ),cθ=cos(θ),vθ=1-cos(θ),θ=fθ3(t),t∈[0,Tnew],θ∈[0,θe];
the attitude adjusting process of the ith positioner supporting point is carried out in a local coordinate system O of the positioneriThe position component of xyz is of the form:
Figure FDA0002536674320000174
in the formula (I), the compound is shown in the specification,
Figure FDA0002536674320000175
in order to interpolate the output X-axis command coordinate position,
Figure FDA0002536674320000177
in order to interpolate the output Y-axis command coordinate position,
Figure FDA0002536674320000176
the Z-axis command coordinate position is output for interpolation.
14. A three-coordinate positioner attitude adjusting operation and control method according to any one of claims 1 to 11, wherein the performing spatial compensation according to the three-axis commanded coordinate position and the spatial error data of each positioner and outputting the actual position of each axis driver specifically comprises:
and performing reverse clearance compensation and pitch error compensation of each axis according to the three-axis instruction coordinate position of each positioner, performing three-axis compensation processing according to the spatial error data, and outputting the actual position of each axis driver.
15. The method as claimed in claim 14, wherein the step of performing the reverse clearance compensation and the pitch error compensation of each axis according to the three-axis command coordinate position of each positioner, and performing the three-axis compensation processing according to the spatial error data to output the actual position of each axis driver comprises:
reading X, Y, Z shaft instruction coordinate position of each locator, performing reverse clearance compensation and pitch error compensation of each shaft, if the locator is at a single-shaft measuring point, directly reading reverse clearance compensation data and pitch error compensation data, if the locator is not at the single-shaft measuring point, performing linear interpolation according to error values of two end points of the single-shaft measuring interval, compensating the single-shaft pitch error of the single-shaft measuring interval, and adding a reverse clearance value;
reading X, Y, Z axis instruction coordinate position of each locator, performing spatial error compensation, directly reading data for compensation if the position is on the grid vertex of the spatial error measurement, reading eight vertex error data of a grid for spatial linear interpolation if the position is not on the grid vertex of the spatial error measurement in a certain grid, and solving the spatial error fitted by the eight vertices of the grid;
and after the reverse clearance compensation, the pitch error compensation and the space error compensation of each shaft are carried out, the actual position of each shaft driver is output.
16. A three-coordinate locator posture adjusting, transporting and controlling system is applied to airplane digital assembly and is characterized by comprising:
the first resolving module is used for establishing a local coordinate system of a rigid body of a large part of the airplane and a local coordinate system of a positioner, resolving the translational movement amount and the translational direction vector of the rigid body, and the rotation angle and the rotation axis vector of the rigid body in fixed-axis rotation according to the attitude adjusting instruction;
the second resolving module is used for resolving the circle center and the radius of a space circular arc track of each locator in the rigid body fixed axis rotation process according to the rotating shaft vector of the rigid body fixed axis rotation, the rigid body rotating center position and the current position of each locator supporting point as the mass point on the rigid body, and resolving the corresponding circular arc angular speed range and the rigid body angular speed range according to the allowable error of each circular arc track;
the first planning and finishing module is used for planning and finishing the rigid body composite motion speed according to the rigid body angular speed range, and the rotation angular speed range, the angular acceleration range, the translation speed range and the translation acceleration range which are allowed by the attitude adjustment of the large airplane component;
the adjusting module is used for calculating the maximum speed and the maximum acceleration of each locator driving shaft by taking each locator supporting point as a mass point on the rigid body according to the velocity plan of the rigid body composite motion, and adjusting the velocity and the acceleration of the rigid body composite motion according to the velocity range and the acceleration range allowed by each locator driving shaft;
the second planning and trimming module is used for re-planning and trimming the rigid body composite motion speed after adjusting the speed and the acceleration of the rigid body composite motion;
the interpolation calculation module is used for carrying out interpolation calculation according to a time division method according to a new speed plan of rigid body compound motion and outputting a three-axis instruction coordinate position of each locator;
and the compensation module is used for carrying out space compensation according to the three-axis instruction coordinate position and the space error data of each locator and outputting the actual position of each axis driver.
17. A pose controller comprising a processor and a memory for storing a program executable by the processor, wherein the processor implements the pose control method of the three-coordinate positioner according to any one of claims 1 to 15 when executing the program stored in the memory.
18. A storage medium storing a program, wherein the program, when executed by a processor, implements the three coordinate positioner pose controlling method according to any one of claims 1 to 15.
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Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112613130A (en) * 2021-03-05 2021-04-06 成都飞机工业(集团)有限责任公司 Dimensional positioning pose simulation matching method based on two three-coordinate positioners
CN113156894A (en) * 2021-04-07 2021-07-23 东莞普莱信智能技术有限公司 Speed planning method for chip packaging control and chip packaging control device
CN113580142A (en) * 2021-08-20 2021-11-02 天津大学 Non-redundant geometric error model analytic modeling method for robot based on momentum theory
CN114115116A (en) * 2021-11-24 2022-03-01 上海维宏电子科技股份有限公司 Method, device, processor and computer readable storage medium for realizing speed planning processing for numerical control system
CN116400647A (en) * 2023-06-08 2023-07-07 成都飞机工业(集团)有限责任公司 Multi-axis interpolation motion control method and device, storage medium and electronic equipment

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ES206611A1 (en) * 1951-12-04 1954-05-01 Lightning Fasteners Ltd Improvements in machines to join top topics to sliding closures (Machine-translation by Google Translate, not legally binding)
US4531167A (en) * 1983-08-25 1985-07-23 Pioneer Research, Inc. Servowriter system for magnetic disc drives
US20070245728A1 (en) * 2006-04-25 2007-10-25 Henri Duong Anti-pollution motors/engines run by air/liquid/gas cycle, spring force, pump, energy blades
CN101362512A (en) * 2008-09-19 2009-02-11 浙江大学 Pose alignment system and method of aircraft part based on four locater
CN101362515A (en) * 2008-09-19 2009-02-11 浙江大学 Path planning method of aircraft pose alignment
CN102519441A (en) * 2011-12-06 2012-06-27 南京航空航天大学 Method for measuring positioning points based on laser tracker in docking process of airplane parts
CN206717703U (en) * 2017-03-27 2017-12-08 四川大金不锈钢有限公司 A kind of blade retainer fixture
CN109808914A (en) * 2019-01-23 2019-05-28 南京航空航天大学 A kind of Large Aircraft Components trailing type posture adjusting system locator coordinate automatic identifying method
CN110618659A (en) * 2019-10-11 2019-12-27 天津工业大学 Five-axis linear interpolation-oriented translation axis and rotation axis coordinated motion planning control method

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
ES206611A1 (en) * 1951-12-04 1954-05-01 Lightning Fasteners Ltd Improvements in machines to join top topics to sliding closures (Machine-translation by Google Translate, not legally binding)
US4531167A (en) * 1983-08-25 1985-07-23 Pioneer Research, Inc. Servowriter system for magnetic disc drives
US20070245728A1 (en) * 2006-04-25 2007-10-25 Henri Duong Anti-pollution motors/engines run by air/liquid/gas cycle, spring force, pump, energy blades
CN101362512A (en) * 2008-09-19 2009-02-11 浙江大学 Pose alignment system and method of aircraft part based on four locater
CN101362515A (en) * 2008-09-19 2009-02-11 浙江大学 Path planning method of aircraft pose alignment
CN102519441A (en) * 2011-12-06 2012-06-27 南京航空航天大学 Method for measuring positioning points based on laser tracker in docking process of airplane parts
CN206717703U (en) * 2017-03-27 2017-12-08 四川大金不锈钢有限公司 A kind of blade retainer fixture
CN109808914A (en) * 2019-01-23 2019-05-28 南京航空航天大学 A kind of Large Aircraft Components trailing type posture adjusting system locator coordinate automatic identifying method
CN110618659A (en) * 2019-10-11 2019-12-27 天津工业大学 Five-axis linear interpolation-oriented translation axis and rotation axis coordinated motion planning control method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
薛宏等: "《大飞机活动翼面机器人自动制孔应用研究》", 《航空制造技术》 *

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112613130A (en) * 2021-03-05 2021-04-06 成都飞机工业(集团)有限责任公司 Dimensional positioning pose simulation matching method based on two three-coordinate positioners
CN113156894A (en) * 2021-04-07 2021-07-23 东莞普莱信智能技术有限公司 Speed planning method for chip packaging control and chip packaging control device
CN113156894B (en) * 2021-04-07 2021-10-01 东莞普莱信智能技术有限公司 Speed planning method for chip packaging control and chip packaging control device
CN113580142A (en) * 2021-08-20 2021-11-02 天津大学 Non-redundant geometric error model analytic modeling method for robot based on momentum theory
CN113580142B (en) * 2021-08-20 2023-10-13 天津大学 Robot redundancy-free geometric error model analytical modeling method based on rotation theory
CN114115116A (en) * 2021-11-24 2022-03-01 上海维宏电子科技股份有限公司 Method, device, processor and computer readable storage medium for realizing speed planning processing for numerical control system
CN116400647A (en) * 2023-06-08 2023-07-07 成都飞机工业(集团)有限责任公司 Multi-axis interpolation motion control method and device, storage medium and electronic equipment
CN116400647B (en) * 2023-06-08 2023-09-29 成都飞机工业(集团)有限责任公司 Multi-axis interpolation motion control method and device, storage medium and electronic equipment

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