CN109079850B - D-H system and D-H parameter determination method of multi-axis robot based on axis invariance - Google Patents

D-H system and D-H parameter determination method of multi-axis robot based on axis invariance Download PDF

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CN109079850B
CN109079850B CN201810933322.XA CN201810933322A CN109079850B CN 109079850 B CN109079850 B CN 109079850B CN 201810933322 A CN201810933322 A CN 201810933322A CN 109079850 B CN109079850 B CN 109079850B
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CN109079850A (en
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居鹤华
石宝钱
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B25HAND TOOLS; PORTABLE POWER-DRIVEN TOOLS; MANIPULATORS
    • B25JMANIPULATORS; CHAMBERS PROVIDED WITH MANIPULATION DEVICES
    • B25J19/00Accessories fitted to manipulators, e.g. for monitoring, for viewing; Safety devices combined with or specially adapted for use in connection with manipulators
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Abstract

The invention discloses a multi-axis robot D-H system and D-H parameter determination method based on axis invariants. Defining a one-dimensional coordinate axis which is composed of an original point and a unit base and is a direction reference line with scales, wherein the scales of the points on the axis are coordinates; the shaft invariants are parameterized natural coordinate bases, are elements of a multi-shaft system, and are equivalent to the translation and rotation of a coordinate system fixedly connected with the fixed shaft invariants; the indexes in the D-H system conform to the father indexes; determining a D-H system through a fixed shaft invariant, determining a middle point and a D-H system origin point, and obtaining a unit coordinate vector; and obtaining the attitude according to the rotation characteristic of the vector. The method is based on the structural parameters of the axis invariants, does not need to establish an intermediate coordinate system, avoids measurement errors caused by introducing the intermediate coordinate system, and ensures the accuracy of determining the D-H system and the D-H parameters. The method has an important function of improving the absolute positioning and attitude determination precision of the robot.

Description

D-H system and D-H parameter determination method of multi-axis robot based on axis invariance
Technical Field
The invention relates to a D-H system and D-H parameter determination method for a multi-axis robot, and belongs to the technical field of robots.
Background
When the robot applies D-H system modeling and D-H parameters to calculate inverse kinematics, the absolute positioning and attitude determination precision of a robot system is far lower than the repeated precision of the system due to the existence of machining and assembling errors; meanwhile, the D-H system establishing and D-H parameter determining processes in the prior art are complicated, and when the degree of freedom of the system is high, the manual completion of the process is low in reliability. Therefore, there is a need to solve the problem of determining the D-H system and D-H parameters by a computer. Meanwhile, the high-precision D-H system and D-H parameters are the basis for the accurate operation of the robot and the development of the Teaching-Playback (Teaching and playing) robot to the autonomous robot.
Disclosure of Invention
The invention aims to solve the technical problem of providing a D-H system and a D-H parameter determination method of a multi-axis robot based on axis invariance, which does not need to establish an intermediate coordinate system, avoids measurement errors caused by introducing the intermediate coordinate system, ensures the accuracy of determining the D-H system and the D-H parameter, and improves the absolute positioning and attitude determination accuracy of the robot.
In order to solve the technical problems, the invention adopts the following technical scheme:
a method for determining D-H system and D-H parameters of a multi-axis robot based on axis invariance is characterized in that,
defining a one-dimensional coordinate axis l from an origin OlAnd a unit radical elIs formed by a scaleThe scale of the point S on the axis l is the coordinate; basis vector e in whole formlRepresenting an objective unit direction, the component form being noted
Figure BDA0001767186460000011
Namely, the three-dimensional space-time-domain three-dimensional space-time domain;
Figure BDA0001767186460000012
is the unit volume of the rod l in the x-axis under the D-H system,
Figure BDA0001767186460000013
in the same way, the same applies when the rod is l';
base vector elIs a reaction of with F[l]Any vector of consolidation, like the base vector
Figure BDA0001767186460000014
Is and
Figure BDA0001767186460000015
any vector, axis invariant of consolidation
Figure BDA0001767186460000016
Is F[l]And
Figure BDA0001767186460000017
a common reference group; the shaft invariants are parameterized natural coordinate bases, are elements of a multi-shaft system, and are equivalent to the translation and rotation of a coordinate system fixedly connected with the fixed shaft invariants;
when the system is in a zero position, the natural coordinate system is used as a reference, and coordinate axis vectors are obtained through measurement
Figure BDA0001767186460000018
In the kinematic pairAxial vector during motion
Figure BDA00017671864600000110
Is an invariant; axial vectorAnd joint variables
Figure BDA00017671864600000112
Uniquely identifying kinematic pairThe rotational relationship of (a);
Figure BDA00017671864600000114
are respectively a connecting rod piece
Figure BDA00017671864600000115
Coordinate axis vectors and kinematic pairs of the rod pieces l are similar to those of other rod pieces;
natural coordinate system
Figure BDA00017671864600000116
Corresponding D-H is described as
Figure BDA00017671864600000117
F[l']The same process is carried out; kinematic pair
Figure BDA00017671864600000118
The corresponding axes are denoted by
Figure BDA00017671864600000119
That is, the indexes in the D-H system conform to the parent indexes;
determining a D-H system by fixing axis invariants, comprising the steps of:
determining intermediate points
Figure BDA0001767186460000021
And D-H is origin Ol′
【1】 Order toAnd zl′Respectively passing through the axes by constant amountsAndand is
Figure BDA0001767186460000025
Wherein,is that
Figure BDA0001767186460000027
The unit coordinate vector of (a) is,
Figure BDA00017671864600000252
the expression form of (1) is a projector, and represents a projection vector or a projection sequence of a vector or a second-order tensor to a reference base, namely a coordinate vector or a coordinate array;
【2】
Figure BDA0001767186460000028
is defined as
Figure BDA0001767186460000029
To
Figure BDA00017671864600000210
The male vertical line of (a);
【3】 To obtain
Figure BDA00017671864600000211
Wherein
Figure BDA00017671864600000212
Is that
Figure BDA00017671864600000213
A unit coordinate vector of (a);
【4】 Rotation characteristics according to vectorTo obtainIs represented by
Figure BDA00017671864600000215
To F[l']In an attitude of, i.e. by the rod member
Figure BDA00017671864600000216
Rotate to the rod l'.
In the step (3),
in the formula,is axis invariant
Figure BDA00017671864600000219
The cross-multiplication matrix of (a) is,
Figure BDA00017671864600000220
is a shaft
Figure BDA00017671864600000221
The unit coordinate vector of (a) is,
Figure BDA00017671864600000222
is a shaft
Figure BDA00017671864600000223
The unit coordinate vector of (2).
In the step (4),
Figure BDA00017671864600000224
Figure BDA00017671864600000225
is that
Figure BDA00017671864600000226
Unit seatThe vector of the standard is marked on the basis of the standard vector,
Figure BDA00017671864600000227
is represented by
Figure BDA00017671864600000228
To F[l']In a posture of being composed of
Figure BDA00017671864600000229
Rotate to l'.
In step [ 2 ], ifThen
Figure BDA00017671864600000231
In the formula,is a shaft
Figure BDA00017671864600000234
The unit coordinate vector of (a) is,
Figure BDA00017671864600000235
is that
Figure BDA00017671864600000236
A unit coordinate vector of (a);
Figure BDA00017671864600000237
is a rod piece
Figure BDA00017671864600000238
From the origin to the rod
Figure BDA00017671864600000239
OfTranslation vector of the point.
In step [ 2 ], if
Figure BDA00017671864600000240
And is
Figure BDA00017671864600000241
Then
Figure BDA00017671864600000242
In the formula,
Figure BDA00017671864600000243
is a rod piece
Figure BDA00017671864600000244
The origin of the rod l to the origin of the rod l;
Figure BDA00017671864600000245
is axis invariant
Figure BDA00017671864600000246
A cross-product matrix of; 03=[0 0 0]T
In step [ 2 ], if
Figure BDA00017671864600000247
And is
Figure BDA00017671864600000248
Then
Figure BDA00017671864600000249
And is
Figure BDA00017671864600000250
Is represented by the formula (12) andto obtain
Figure BDA0001767186460000031
In the formula,is a rod piece
Figure BDA0001767186460000033
The origin of the rod l to the origin of the rod l;
Figure BDA0001767186460000034
is a rod piece
Figure BDA0001767186460000035
To the i' origin of the rod.
And the method also comprises a D-H parameter determination step based on the fixed axis invariant.
Determining D-H parameters
Figure BDA0001767186460000036
And
Figure BDA0001767186460000037
and
Figure BDA0001767186460000038
are respectively rod pieces
Figure BDA0001767186460000039
To the rod piece
Figure BDA00017671864600000310
The wheelbase and the offset of the wheel,
Figure BDA00017671864600000311
Figure BDA00017671864600000312
in the formula,
Figure BDA00017671864600000313
is a shaft
Figure BDA00017671864600000314
A unit coordinate vector of (a);
Figure BDA00017671864600000315
is a rod piece
Figure BDA00017671864600000316
The origin of the rod l to the origin of the rod l;is a rod piece
Figure BDA00017671864600000318
From the origin to the rod
Figure BDA00017671864600000319
The translation vector of the origin of (a);
Figure BDA00017671864600000320
is a rod piece
Figure BDA00017671864600000321
From the origin to the rod
Figure BDA00017671864600000322
The origin of the translation vector.
Order to
Figure BDA00017671864600000323
Defined by the angle of twist of the shaft
Figure BDA00017671864600000324
In the formula,
Figure BDA00017671864600000325
is a shaft
Figure BDA00017671864600000326
To the shaft
Figure BDA00017671864600000327
The twist angle of (c).
Order toDefined by the angle of rotation of the joint
Figure BDA00017671864600000329
In the formula,
Figure BDA00017671864600000330
is a shaft
Figure BDA00017671864600000331
Zero position of (a).
The invention achieves the following beneficial effects:
the invention provides and analyzes a D-H system and a D-H parameter determination method based on fixed axis invariants. The model engineering application of the CE3 rover demonstrates the correctness of this principle. The invention has simple chain symbol system and expression form of axis invariant, has pseudo code function, accurate physical meaning, and ensures reliability of engineering realization; based on the structural parameters of the axis invariant, an intermediate coordinate system does not need to be established, so that the measurement error caused by introducing the intermediate coordinate system is avoided, and the accuracy of determining the D-H system and the D-H parameters is ensured. The method has an important function of improving the absolute positioning and attitude determination precision of the robot.
Drawings
FIG. 1 a natural coordinate system and axis chain;
FIG. 2 is a fixed axis invariant;
FIG. 3 is a diagram illustrating the relationship between the natural coordinate system and the D-H system.
Detailed Description
The invention is further described below with reference to the accompanying drawings. The following examples are only for illustrating the technical solutions of the present invention more clearly, and the protection scope of the present invention is not limited thereby.
Define 1 natural coordinate axes: a unit reference axis having a fixed origin, referred to as being coaxial with the axis of motion or measurement, is a natural coordinate axis, also referred to as the natural reference axis.
Defining 2 a natural coordinate system: as shown in fig. 1, if the multi-axis system D is located at the zero position, the directions of all cartesian body coordinate systems are the same, and the origin of the body coordinate system is located on the axis of the moving shaft, the coordinate system is a natural coordinate system, which is simply referred to as a natural coordinate system.
The natural coordinate system has the advantages that: (1) the coordinate system is easy to determine; (2) the joint variable at zero is zero; (3) the system postures at the zero position are consistent; (4) and accumulated errors of measurement are not easily introduced.
From definition 2, it can be seen that the natural coordinate system of all the rods coincides with the orientation of the base or world system when the system is in the zero position. With the system in zero position
Figure BDA0001767186460000041
Time, natural coordinate system
Figure BDA0001767186460000042
Vector around axis
Figure BDA0001767186460000043
Angle of rotationWill be provided with
Figure BDA0001767186460000045
Go to F[l]
Figure BDA0001767186460000046
In that
Figure BDA0001767186460000047
Coordinate vector of
Figure BDA0001767186460000048
At F[l]Coordinate vector of
Figure BDA0001767186460000049
Is constant, i.e. has
Figure BDA00017671864600000410
According to the formula, the method has the advantages that,
Figure BDA00017671864600000411
or
Figure BDA00017671864600000412
Independent of adjacent coordinate systems
Figure BDA00017671864600000413
And F[l](ii) a So it is called
Figure BDA00017671864600000414
Or
Figure BDA00017671864600000415
Is axis invariant. When invariance is not emphasized, the method can be called a coordinate axis vector (axis vector for short).
Figure BDA00017671864600000416
OrCharacterized by being a bodyCoordinate vector of reference unit common to body l, and reference point
Figure BDA00017671864600000419
And OlIs irrelevant. Body
Figure BDA00017671864600000420
The body l is a rod or a shaft.
The axis invariants are essentially different from coordinate axes:
(1) the coordinate axis is a reference direction with a zero position and unit scales, and can describe the position of translation along the direction, but cannot completely describe the rotation angle around the direction, because the coordinate axis does not have a radial reference direction, namely, the zero position representing rotation does not exist. In practical applications, the radial reference of the shaft needs to be supplemented. For example: in the Cartesian system F[l]In the rotation around lx, ly or lz is used as a reference zero position. The coordinate axes themselves are 1D, with 3 orthogonal 1D reference axes constituting a 3D cartesian frame.
(2) The axis invariant is a 3D spatial unit reference axis, which is itself a frame. It itself has a radial reference axis, i.e. a reference null. The spatial coordinate axes and their own radial reference axes may define cartesian frames. The spatial coordinate axis may reflect three basic reference properties of the motion axis and the measurement axis.
The axis vector of the chainless index is recorded in the literature
Figure BDA00017671864600000421
And is called the Euler Axis (Euler Axis), and the corresponding joint Angle is called the Euler Angle. The present application is no longer followed by the euler axis, but rather is referred to as the axis invariant because the axis invariant has the following properties:
【1】 Given rotation transformation array
Figure BDA00017671864600000422
Since it is a real matrix whose modes are unity, it has a real eigenvalue λ1And two complex eigenvalues λ conjugated to each other2=eAnd lambda3=e-iφ(ii) a Wherein: i is a pure imaginary number. Therefore, | λ1|·||λ2||·||λ31, to obtain lambda11. Axial vector
Figure BDA00017671864600000423
Is a real eigenvalue λ11, is an invariant;
【2】 Is a 3D reference shaft, not only having an axial reference direction, but also having a radial reference null, as will be described in section 3.3.1.
【3】 Under a natural coordinate system:i.e. axial invariant
Figure BDA0001767186460000052
Is a very special vector, has invariance to the derivative of time and has very good mathematical operation performance;
for an axis invariant, its absolute derivative is its relative derivative. Since the axis invariant is a natural reference axis with invariance, its absolute derivative is always a zero vector. Thus, the axis invariants have invariance to the time differential. Comprises the following steps:
Figure BDA0001767186460000053
【4】 In a natural coordinate system, passing an axial vector
Figure BDA0001767186460000054
And joint variables
Figure BDA0001767186460000055
Can directly describe the rotating coordinate array
Figure BDA0001767186460000056
It is not necessary to establish a separate system for the rods other than the roots. Meanwhile, the measurement precision of the system structure parameters can be improved by taking the only root coordinate system to be defined as reference;
【5】 Using axial vectors
Figure BDA0001767186460000057
The method has the advantages that a completely parameterized unified multi-axis system kinematics and dynamics model comprising a topological structure, a coordinate system, a polarity, a structure parameter and a mechanics parameter is established.
Factor vector elIs a reaction of with F[l]Any vector, base vector, of consolidation
Figure BDA0001767186460000058
Is and
Figure BDA0001767186460000059
any vector of consolidation, in turn
Figure BDA00017671864600000510
Is F[l]And
Figure BDA00017671864600000511
a common unit vector, therefore
Figure BDA00017671864600000512
Is F[l]And
Figure BDA00017671864600000513
a common basis vector. Thus, the axis is invariantIs F[l]And
Figure BDA00017671864600000515
common reference base. The axis invariants are parameterized natural coordinate bases, and are primitives of the multi-axis system. The translation and rotation of the fixed shaft invariant are equivalent to the translation and rotation of a coordinate system fixedly connected with the fixed shaft invariant.
When the system is in a zero position, the natural coordinate system is used as a reference, and coordinate axis vectors are obtained through measurement
Figure BDA00017671864600000516
In the kinematic pair
Figure BDA00017671864600000517
Axial vector during motionIs not changedAn amount; axial vector
Figure BDA00017671864600000519
And joint variables
Figure BDA00017671864600000520
Uniquely identifying kinematic pair
Figure BDA00017671864600000521
The rotational relationship of (1).
Thus, with the natural coordinate system, only a common reference frame need be determined when the system is in the null position, rather than having to determine individual body coordinate systems for each rod in the system, as they are uniquely determined by the axis invariants and the natural coordinates. When performing system analysis, the other natural coordinate systems, apart from the base system, to which the bars are fixed, only occur conceptually, and are not relevant to the actual measurement. The theoretical analysis and engineering functions of a natural coordinate system on a multi-axis system (MAS) are as follows:
(1) the measurement of the structural parameters of the system needs to be measured by a uniform reference system; otherwise, not only is the engineering measurement process cumbersome, but the introduction of different systems introduces greater measurement errors.
(2) A natural coordinate system is applied, and except for the root rod piece, the natural coordinate systems of other rod pieces are naturally determined by the structural parameters and the joint variables, so that the kinematics and dynamics analysis of the MAS system is facilitated.
(3) In engineering, the method can be applied to optical measurement equipment such as a laser tracker and the like to realize the accurate measurement of the invariable of the fixed shaft.
(4) As the kinematic pairs R and P, the spiral pair H and the contact pair O are special cases of the cylindrical pair C, the MAS kinematics and dynamics analysis can be simplified by applying the cylindrical pair.
Definition 3 invariant: the quantities that are not measured in dependence on a set of coordinate systems are called invariant.
Define 4 rotational coordinate vectors: vector around coordinate axis
Figure BDA0001767186460000061
Rotated to an angular position
Figure BDA0001767186460000062
Coordinate vector ofIs composed of
Figure BDA0001767186460000064
Define 5 translation coordinate vectors: vector along coordinate axis
Figure BDA0001767186460000065
Translation to linear position
Figure BDA0001767186460000066
Coordinate vector of
Figure BDA0001767186460000067
Is composed of
Figure BDA0001767186460000068
Define 6 natural coordinates: taking the vector of the natural coordinate axis as a reference direction, and marking the angular position or linear position of the zero position of the system as qlCalled natural coordinates; weighing the quantity mapped one by one with the natural coordinate as a joint variable; wherein:
Figure BDA0001767186460000069
define 7 mechanical zero: for kinematic pairAt an initial time t0Zero position of time, joint absolute encoder
Figure BDA00017671864600000611
Not necessarily zero, which is called mechanical zero;
hence the joint
Figure BDA00017671864600000612
Control amount of
Figure BDA00017671864600000613
Is composed of
Defining 8 natural motion vectors: will be represented by natural coordinate axis vectors
Figure BDA00017671864600000615
And natural coordinate qlDetermined vectorReferred to as natural motion vectors. Wherein:
Figure BDA00017671864600000617
the natural motion vector realizes the unified expression of the translation and rotation of the shaft. Vectors to be determined from natural coordinate axis vectors and joints, e.g.
Figure BDA00017671864600000618
Called free motion vector, also called free helix. Obviously, axial vector
Figure BDA00017671864600000619
Is a specific free helix.
Define 9 the joint space: by joint natural coordinates qlThe space represented is called joint space.
Define a 10-bit shape space: a cartesian space expressing a position and a posture (pose for short) is called a configuration space, and is a dual vector space or a 6D space.
Defining 11 a natural joint space: with reference to natural coordinate system and by joint variables
Figure BDA00017671864600000620
Indicating that there must be at system zero
Figure BDA00017671864600000621
Is called the natural joint space.
As shown in FIG. 2, a given linkOrigin OlPosition-dependent vector
Figure BDA00017671864600000623
Constrained axis vector
Figure BDA00017671864600000624
Is a fixed axis vector, is denoted asWherein:
axial vector
Figure BDA0001767186460000071
Is the natural reference axis for the natural coordinates of the joint. Due to the fact thatIs an axis invariant, so it is calledFor the invariants of fixed axes, it characterizes kinematic pairs
Figure BDA0001767186460000074
The natural coordinate axis is determined. Fixed shaft invariant
Figure BDA0001767186460000075
Is a chain link
Figure BDA0001767186460000076
Natural description of structural parameters.
Defining 12 a natural coordinate axis space: the fixed axis invariant is used as a natural reference axis, and a space represented by corresponding natural coordinates is called a natural coordinate axis space, which is called a natural axis space for short. It is a 3D space with 1 degree of freedom.
As shown in figure 2 of the drawings, in which,
Figure BDA0001767186460000077
and
Figure BDA0001767186460000078
without rod omegalIs a constant structural reference.Determines the axis l relative to the axis
Figure BDA00017671864600000710
Five structural parameters of (a); and joint variable qlTogether, the rod omega is expressed completelylThe 6D bit shape. Given aThe natural coordinate system of the fixed rod can be determined by the structural parameters
Figure BDA00017671864600000712
And joint variables
Figure BDA00017671864600000713
And (4) uniquely determining. Balance shaft invariant
Figure BDA00017671864600000714
Fixed shaft invariant
Figure BDA00017671864600000715
Variation of joint
Figure BDA00017671864600000716
And
Figure BDA00017671864600000717
is naturally invariant. Obviously, invariant by a fixed axis
Figure BDA00017671864600000718
And joint variables
Figure BDA00017671864600000719
Natural invariance of constituent jointsAnd from a coordinate system
Figure BDA00017671864600000721
To F[l]Determined spatial configuration
Figure BDA00017671864600000722
Having a one-to-one mapping relationship, i.e.
Figure BDA00017671864600000723
Given a multi-axis system D ═ T, a, B, K, F, NT }, in the system null position, only the base or inertial frame is established, as well as the reference points O on the axeslOther rod coordinate systems are naturally determined. Essentially, only the base or inertial frame need be determined.
Given a structural diagram with a closed chain connected by kinematic pairs, any kinematic pair in a loop can be selected, and a stator and a mover which form the kinematic pair are divided; thus, a loop-free tree structure, called Span tree, is obtained. T represents a span tree with direction to describe the topological relation of tree chain motion.
I is a structural parameter; a is an axis sequence, F is a rod reference system sequence, B is a rod body sequence, K is a kinematic pair type sequence, and NT is a sequence of constraint axes, i.e., a non-tree.
Figure BDA00017671864600000724
For taking an axis sequence
Figure BDA00017671864600000725
Is a member of (1). The revolute pair R, the prismatic pair P, the helical pair H and the contact pair O are special cases of the cylindrical pair C.
The basic topological symbol and operation for describing the kinematic chain are the basis for forming a kinematic chain topological symbol system, and are defined as follows:
【1】 The kinematic chain is identified by a partially ordered set (].
【2】A[l]Is a member of the axis-taking sequence A; since the axis name l has a unique number corresponding to A[l]Number of (2), therefore A[l]The computational complexity is O (1).
【3】
Figure BDA00017671864600000726
Is a father axis of the taking axis l; shaft
Figure BDA00017671864600000727
The computational complexity of (2) is O (1). The computation complexity O () represents the number of operations of the computation process, typically referred to as the number of floating point multiplies and adds. The calculation complexity is very complicated by the expression of the times of floating point multiplication and addition, so the main operation times in the algorithm circulation process are often adopted; such as: joint pose, velocity, acceleration, etc.
【4】
Figure BDA0001767186460000081
For taking an axis sequenceA member of (a);
Figure BDA0001767186460000083
the computational complexity is O (1).
【5】llkTo take the kinematic chain from axis l to axis k, the output is represented as
Figure BDA0001767186460000084
And is
Figure BDA0001767186460000085
Cardinal number is recorded as $llk|。llkThe execution process comprises the following steps: executeIf it is
Figure BDA0001767186460000087
Then execute
Figure BDA0001767186460000088
Otherwise, ending.llkThe computational complexity is O (# |)llk|)。
【6】ll is a child of axis l. The operation is represented in
Figure BDA0001767186460000089
Finding the address k of the member l; thus, a sub-A of the axis l is obtained[k]. Due to the fact that
Figure BDA00017671864600000810
Has no off-order structure, thereforelThe computational complexity of l is
Figure BDA00017671864600000811
【7】lL denotes obtaining a closed sub-tree consisting of the axis L and its sub-tree, l l is a subtree containing no L; recursive executionll, the computational complexity is
Figure BDA00017671864600000812
【8】 Adding and deleting operations of branches, subtrees and non-tree arcs are also necessary components; thus, the variable topology is described by a dynamic Span tree and a dynamic graph. In the branchllkIn, if
Figure BDA00017671864600000813
Then remember
Figure BDA00017671864600000814
Figure BDA00017671864600000815
Namely, it isRepresenting the child of member m taken in the branch.
The following expression or expression form is defined:
the shafts and the rod pieces have one-to-one correspondence; quantity of property between axes
Figure BDA00017671864600000817
And the amount of attribute between the rods
Figure BDA00017671864600000818
Has the property of order bias.
Appointing:
Figure BDA00017671864600000833
representing attribute placeholders; if the attribute P or P is location-related, then
Figure BDA00017671864600000819
Is understood to be a coordinate system
Figure BDA00017671864600000820
To F[l]The origin of (a); if the property P or P is directional, thenIs understood to be a coordinate systemTo F[l]
Figure BDA00017671864600000823
And
Figure BDA00017671864600000824
are to be understood as a function of time t, respectively
Figure BDA00017671864600000825
And
Figure BDA00017671864600000826
and is
Figure BDA00017671864600000827
And
Figure BDA00017671864600000828
is t0A constant or array of constants at a time. But in the body
Figure BDA00017671864600000829
And
Figure BDA00017671864600000830
should be considered a constant or an array of constants.
In the present application, the convention: in a kinematic chain symbolic operation system, attribute variables or constants with partial order include indexes representing partial order in name; or the upper left corner and the lower right corner, or the upper right corner and the lower right corner; the direction of the parameters is always from the upper left corner index to the lower right corner index of the partial order index or from the upper right corner index to the lower right corner index. For example:can be briefly described as (representing k to l) translation vectors;
Figure BDA00017671864600000832
represents the line position (from k to l);krlrepresents a translation vector (from k to l); wherein: r represents a "translation" attribute symbolAnd the other attribute symbols correspond to: the attribute token phi represents "rotate"; the attribute symbol Q represents a "rotation transformation matrix"; the attribute symbol l represents "kinematic chain"; attribute character u represents a "unit vector"; the attribute symbol ω represents "angular velocity"; the angle index i represents an inertial coordinate system or a geodetic coordinate system; other corner marks can be other letters and can also be numbers.
The symbolic specification and convention of the application are determined according to the principle that the sequence bias of the kinematic chain and the chain link are the basic unit of the kinematic chain, and reflect the essential characteristics of the kinematic chain. The chain index represents the connection relation, and the upper right index represents the reference system. The expression of the symbol is simple and accurate, and is convenient for communication and written expression. Meanwhile, the data are structured symbolic systems, which contain elements and relations for forming each attribute quantity, thereby facilitating computer processing and laying a foundation for automatic modeling of a computer. The meaning of the index needs to be understood through the context of the attribute symbol; such as: if the attribute symbol is of a translation type, the index at the upper left corner represents the origin and the direction of a coordinate system; if the attribute is of the pivot type, the top left indicator represents the direction of the coordinate system.
(1)lS-a point S in the bar l; and S denotes a point S in space.
(2)
Figure BDA0001767186460000091
Origin O of bar kkTo the origin O of the rod llA translation vector of (a);
krl
Figure BDA0001767186460000092
in a natural coordinate system F[k]The coordinate vector from k to l;
(3)
Figure BDA0001767186460000093
-origin OkTo point lSA translation vector of (a);
Figure BDA0001767186460000094
Figure BDA0001767186460000095
at F[k]A lower coordinate vector;
(4)
Figure BDA0001767186460000096
-origin OkA translation vector to point S;
krS
Figure BDA0001767186460000097
at F[k]A lower coordinate vector;
(5)
Figure BDA0001767186460000098
-a connecting rod member
Figure BDA0001767186460000099
And a kinematic pair of the rod piece l;
Figure BDA00017671864600000910
kinematic pair
Figure BDA00017671864600000911
An axis vector of (a);
Figure BDA00017671864600000912
and
Figure BDA00017671864600000913
Figure BDA00017671864600000914
are respectively at
Figure BDA00017671864600000915
And F[l]A lower coordinate vector;is an axis invariant, being a structural constant;
Figure BDA00017671864600000917
as rotation vector, rotation vector/angle vector
Figure BDA00017671864600000918
Is a free vector, i.e., the vector is free to translate;
(6)
Figure BDA00017671864600000919
along the axisThe linear position (translational position) of (c),
-about an axis
Figure BDA00017671864600000922
The angular position of (a), i.e. joint angle, joint variable, is a scalar;
(7) when the index of the lower left corner is 0, the index represents a mechanical zero position; such as:
-a translation shaft
Figure BDA00017671864600000924
The mechanical zero position of the magnetic field sensor,
Figure BDA00017671864600000925
-a rotating shaftMechanical zero position of (a);
(8) 0-three-dimensional zero matrix; 1-a three-dimensional identity matrix;
(9) appointing: "\ indicates continuationSymbol;
Figure BDA00017671864600000932
representing attribute placeholders; then
Power symbolTo represent
Figure BDA00017671864600000933
To the x-th power of; the right upper corner is marked with ^ or
Figure BDA00017671864600000928
A representation separator; such as:
Figure BDA00017671864600000929
or
Figure BDA00017671864600000930
Is composed of
Figure BDA00017671864600000931
To the x power of.
Figure BDA0001767186460000101
To represent
Figure BDA0001767186460000102
The transpose of (1) indicates transposing the set, and no transpose is performed on the members; such as:
Figure BDA0001767186460000104
the projection symbol is a projection vector or a projection sequence of a vector or a second-order tensor to a reference base, namely a coordinate vector or a coordinate array, and the projection is dot product operation "·"; such as: position vector
Figure BDA0001767186460000105
In a coordinate system F[k]The projection vector in (1) is recorded as
Figure BDA0001767186460000107
Is a cross multiplier; such as:
Figure BDA0001767186460000108
is axis invariant
Figure BDA0001767186460000109
A cross-product matrix of; given any vector
Figure BDA00017671864600001010
Is cross-multiplication matrix of
Figure BDA00017671864600001011
The cross-multiplication matrix is a second order tensor.
Cross-multiplier operations have a higher priority than projecters
Figure BDA00017671864600001012
The priority of (2). Projecting sign
Figure BDA00017671864600001013
Is higher priority than the member access character
Figure BDA00017671864600001014
Or
Figure BDA00017671864600001015
Member access signPriority higher than power symbol
Figure BDA00017671864600001017
(10) Projection vector of unit vector in geodetic coordinate systemUnit zero vector
Figure BDA00017671864600001019
(11)Zero position by origin
Figure BDA00017671864600001021
To the origin OlIs translated by the vector of
Figure BDA00017671864600001022
Representing the location structure parameter.
(12)iQlA rotation transformation matrix in relative absolute space;
(13) taking the vector of the natural coordinate axis as a reference direction, and marking the angular position or linear position of the zero position of the system as qlCalled natural coordinates; variation of jointNatural joint coordinate phil
(14) For a given ordered set r ═ 1,4,3,2]TRemember r[x]The representation takes the x-th row element of the set r. Frequently remembered [ x ]]、[y]、[z]And [ omega ]]This is shown with the elements in columns 1, 2, 3 and 4.
(15)iljRepresents a kinematic chain from i to j;llktaking a kinematic chain from an axis l to an axis k;
given kinematic chain
Figure BDA00017671864600001024
If n represents a Cartesian rectangular system, it is calledIs a Cartesian axis chain; if n represents a natural reference axis, then call
Figure BDA00017671864600001026
Is a natural axis chain.
(16) Rodrigues quaternion expression form:
Figure BDA00017671864600001027
euler quaternion expression:
Figure BDA00017671864600001028
quaternion (also called axis quaternion) representation of invariants
Figure BDA00017671864600001029
Such as position vectors
Figure BDA00017671864600001030
The projection vector on three Cartesian coordinate axes is
Figure BDA00017671864600001031
Definition of
Figure BDA00017671864600001032
Due to the fact thatlrlSThe top left indicator indicates the reference frame,lrlSnot only indirectly represent displacement vector
Figure BDA00017671864600001033
And the displacement coordinate vector is directly expressed, namely, the dual functions of the vector and the coordinate vector are realized.
1. D-H system modeling method based on fixed axis invariant
As shown in fig. 3, a ═ 0,1, …, k],F={F[l]|l∈A},Wherein: f[l]Is a natural coordinate system, F[l′]Is a D-H series; and is provided with
A is an axis sequence, and F is a rod reference system sequence;
under the adjacent natural coordinate system, the adjacent rods l and
Figure BDA0001767186460000113
have the same coordinates;
i-fixed axis invariants;
one-dimensional coordinate axis l is defined by the origin OlAnd a unit radical elThe structure is that the direction reference line is provided with scales; which are the primitives that make up the reference frame. The scale of point S on axis i is the coordinate. Basis vector e in whole formlRepresenting an objective unit direction; its component form is described as
Figure BDA0001767186460000114
I.e., composed of three independent ordered symbols, representing three independent degrees of freedom.
Figure BDA0001767186460000115
Is the unit product of the x-axis of the axis l under the D-H system,the same is true.
Factor vector elIs a reaction of with F[l]Any vector, base vector, of consolidation
Figure BDA0001767186460000117
Is andany vector of consolidation, in turn
Figure BDA0001767186460000119
Is F[l]And
Figure BDA00017671864600001110
a common unit vector, therefore
Figure BDA00017671864600001111
Is F[l]And
Figure BDA00017671864600001112
a common basis vector. Thus, the axis is invariantIs F[l]And
Figure BDA00017671864600001114
common reference base. The axis invariants are parameterized natural coordinate bases, and are primitives of the multi-axis system. The translation and rotation of the fixed shaft invariant are equivalent to the translation and rotation of a coordinate system fixedly connected with the fixed shaft invariant.
When the system is in a zero position, the natural coordinate system is used as a reference, and coordinate axis vectors are obtained through measurementIn the kinematic pair
Figure BDA00017671864600001116
Axial vector during motion
Figure BDA00017671864600001117
Is an invariant; axial vector
Figure BDA00017671864600001118
And joint variables
Figure BDA00017671864600001119
Uniquely identifying kinematic pair
Figure BDA00017671864600001120
The rotational relationship of (1).
The D-H system plays an important role in the inverse kinematics calculation of the robot. Given a multi-axis system, any state is taken as the zero position of the system. Natural coordinate system
Figure BDA00017671864600001121
Corresponding D-H is described as
Figure BDA00017671864600001122
According to the numbering habit of the D-H coordinate system, the kinematic pair
Figure BDA00017671864600001123
The corresponding axes are denoted by
Figure BDA00017671864600001124
I.e. the indices in the D-H system are used to follow parent indices, unlike the numbering of the natural coordinate system to follow child indices.
First, an intermediate point is determined
Figure BDA00017671864600001125
And D-H is origin Ol′
【1】 Order toAnd zl′Respectively passing through the axes by constant amounts
Figure BDA00017671864600001127
And
Figure BDA00017671864600001128
and is
【2】Is defined as
Figure BDA00017671864600001131
To nlThe male vertical line of (1) includes three cases.
[ 2.1 ] ifThen 0rl′Available axis invariantAnd
Figure BDA00017671864600001135
and (4) showing.
Figure BDA0001767186460000121
Figure BDA0001767186460000122
Due to the fact thatAnd is
Figure BDA0001767186460000124
To obtain
Figure BDA0001767186460000125
Resolution of formula (3) to
Figure BDA0001767186460000126
Bringing formula (4) into formula (1)
Figure BDA0001767186460000127
For a natural coordinate system, there are
Rewriting the formula (7), the formula (5) and the formula (6) as follows:
and is
Figure BDA00017671864600001211
The formula (7) and the formula (9) can be expressed as follows
In general,
Figure BDA0001767186460000131
for presentation
Figure BDA0001767186460000132
The null direction.
Figure BDA0001767186460000133
Is a shaftA unit coordinate vector of (a);
[ 2.2 ] obviously, ifAnd is
Figure BDA0001767186460000136
To obtainAnd is
Figure BDA0001767186460000138
[ 2.3 ] if
Figure BDA0001767186460000139
And isThen
Figure BDA00017671864600001311
And is
Figure BDA00017671864600001312
Is represented by the formula (12) and
Figure BDA00017671864600001313
to obtain
Figure BDA00017671864600001314
【3】 To obtain
Figure BDA00017671864600001315
Figure BDA00017671864600001316
Figure BDA00017671864600001317
Is a shaft
Figure BDA00017671864600001318
A unit coordinate vector of (a);
【4】 From formula (15) to
Figure BDA00017671864600001319
Based on rotation of the vector, the base vector
Figure BDA00017671864600001332
And base vector elIs defined as the outer dot product of
Figure BDA00017671864600001321
Is a shaftA unit coordinate vector of (a);
Figure BDA00017671864600001324
is represented by
Figure BDA00017671864600001325
To F[l']In a posture of being composed of
Figure BDA00017671864600001326
Rotate to l'.
Thus, the D-H series is determined by fixing the axis invariant.
2. D-H parameter determination method based on fixed shaft invariant
As shown in figure 3 of the drawings,
Figure BDA00017671864600001327
is a shaft
Figure BDA00017671864600001328
The unit coordinate vector of (2).
Figure BDA00017671864600001329
Figure BDA00017671864600001330
Order toDefined by the angle of twist of the shaft
Figure BDA0001767186460000141
Order to
Figure BDA0001767186460000142
Defined by the angle of rotation of the joint
Figure BDA0001767186460000143
Wherein: a islAnd clAre respectively a shaft
Figure BDA0001767186460000144
Wheelbase and offset, α, to the axis llIs a shaft
Figure BDA0001767186460000145
The angle of twist to the axis l is,is a shaft
Figure BDA0001767186460000147
Zero position of (a).
In conclusion, the fixed shaft does not change
Figure BDA0001767186460000148
And
Figure BDA0001767186460000149
can conveniently express the D-H parameter
Figure BDA00017671864600001410
And
Figure BDA00017671864600001411
can express zero position at the same time
Figure BDA00017671864600001412
The D-H system and D-H parameter determination based on the fixed axis invariant has the following functions:
【1】 The problem that the D-H system and the D-H parameters are difficult to realize in engineering is solved; since the determination of the D-H system and D-H parameters requires the use of optical features, which are usually located inside and outside the rod, it is not possible to measure them accurately in engineering. Whereas the fixed axis invariants can be measured indirectly by means of an optical measuring device such as a laser tracker.
【2】 The accuracy of the D-H system and the D-H parameters is ensured; the process of determining the D-H system and the D-H parameters needs to meet the orthogonality requirement, and is difficult to meet in engineering. When a multi-axis system is designed, the D-H system and the D-H parameters determined according to a drawing are greatly different from the engineering D-H system and the engineering D-H parameters, and errors caused by machining and system assembly need to be considered. The fixed shaft invariant measured by engineering can obtain accurate structural parameters represented by the fixed shaft invariant on the premise of ensuring the precision of the measuring equipment, thereby ensuring the precision of a D-H system and D-H parameters.
The above description is only a preferred embodiment of the present invention, and it should be noted that, for those skilled in the art, several modifications and variations can be made without departing from the technical principle of the present invention, and these modifications and variations should also be regarded as the protection scope of the present invention.

Claims (8)

1. A method for determining D-H system and D-H parameters of a multi-axis robot based on axis invariance is characterized in that,
defining a one-dimensional coordinate axis l from an origin OlAnd a unit radical elThe method comprises the following steps that a one-dimensional coordinate axis l is a direction reference line with scales, and the scales of a point S on the coordinate axis l are coordinates; basis vector e in whole formlRepresenting an objective unit direction, the component form being noted
Figure FDA0002266212720000011
I.e. by three independent ordersSymbolic composition, representing three independent degrees of freedom;
Figure FDA0002266212720000012
is a unit base of the bar member l on the x-axis under the D-H system,
Figure FDA0002266212720000013
in the same way, the same applies when the rod is l';
base vector elIs a reaction of with F[l]Any vector of consolidation, like the base vector
Figure FDA0002266212720000014
Is andany vector, axis invariant of consolidation
Figure FDA0002266212720000016
Is F[l]Anda common reference group; the shaft invariants are parameterized natural coordinate bases, are elements of a multi-shaft system, and are equivalent to the translation and rotation of a coordinate system fixedly connected with the fixed shaft invariants; f[l]Is a natural coordinate system;
when the system is in a zero position, the axis invariant is measured by taking the natural coordinate system as a referenceIn the kinematic pair
Figure FDA0002266212720000019
The axes are not changed when in motion
Figure FDA00022662127200000110
Is an invariant; axial invariant
Figure FDA00022662127200000111
And joint variables
Figure FDA00022662127200000112
Uniquely identifying kinematic pair
Figure FDA00022662127200000113
The rotational relationship of (a);
Figure FDA00022662127200000114
are respectively a connecting rod piece
Figure FDA00022662127200000115
The shaft invariance and the kinematic pair of the rod piece I are the same as those of other rod pieces;
natural coordinate system
Figure FDA00022662127200000116
Corresponding D-H is described as
Figure FDA00022662127200000117
F[l']The same process is carried out; kinematic pair
Figure FDA00022662127200000118
The corresponding axes are denoted by
Figure FDA00022662127200000119
That is, the indexes in the D-H system conform to the parent indexes;
determining a D-H system by fixing axis invariants, comprising the steps of:
determining intermediate points
Figure FDA00022662127200000120
And D-H is origin Ol′
【1】 Order to
Figure FDA00022662127200000121
And zl′Respectively passing through the axes by constant amounts
Figure FDA00022662127200000122
And
Figure FDA00022662127200000123
and is
Figure FDA00022662127200000124
Wherein,is that
Figure FDA00022662127200000125
The unit coordinate vector of (a) is,
Figure FDA00022662127200000127
the expression form of (1) is a projector, and represents a projection vector or a projection sequence of a vector or a second-order tensor to a reference base, namely a coordinate vector or a coordinate array;
【2】
Figure FDA00022662127200000128
is defined as
Figure FDA00022662127200000129
To
Figure FDA00022662127200000130
The male vertical line of (a);
【3】 To obtain
Figure FDA00022662127200000131
WhereinIs that
Figure FDA00022662127200000133
A unit coordinate vector of (a);
【4】 According to the rotation characteristic of the vector, theIs represented by
Figure FDA00022662127200000135
To F[l']In an attitude of, i.e. by the rod memberRotating to a rod l';
the method also comprises a D-H parameter determination step based on the fixed shaft invariant;
determining D-H parametersAnd
Figure FDA00022662127200000138
Figure FDA00022662127200000139
and
Figure FDA00022662127200000140
are respectively rod pieces
Figure FDA00022662127200000141
To the rod piece
Figure FDA00022662127200000142
The wheelbase and the offset of the wheel,
Figure FDA00022662127200000143
Figure FDA00022662127200000144
in the formula,
Figure FDA00022662127200000145
is a shaft
Figure FDA00022662127200000146
A unit coordinate vector of (a);
Figure FDA00022662127200000147
is a rod piece
Figure FDA00022662127200000148
The origin of the rod l to the origin of the rod l;is a rod piece
Figure FDA00022662127200000150
From the origin to the rod
Figure FDA00022662127200000151
The translation vector of the origin of (a);
Figure FDA00022662127200000152
is a rod piece
Figure FDA00022662127200000153
From the origin to the rodThe origin of the translation vector.
2. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
in the step (3),
Figure FDA00022662127200000155
in the formula,
Figure FDA0002266212720000021
is axis invariant
Figure FDA0002266212720000022
The cross-multiplication matrix of (a) is,is a shaft
Figure FDA0002266212720000024
The unit coordinate vector of (a) is,
Figure FDA0002266212720000025
is a shaftThe unit coordinate vector of (2).
3. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
in the step (4),
Figure FDA0002266212720000027
Figure FDA0002266212720000028
is that
Figure FDA0002266212720000029
The unit coordinate vector of (a) is,
Figure FDA00022662127200000210
is represented byTo F[l']In a posture of being composed of
Figure FDA00022662127200000212
Rotate to l'.
4. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
in step [ 2 ], if
Figure FDA00022662127200000213
Then
Figure FDA00022662127200000214
Figure FDA00022662127200000215
In the formula,
Figure FDA00022662127200000216
is a shaft
Figure FDA00022662127200000217
The unit coordinate vector of (a) is,
Figure FDA00022662127200000218
is that
Figure FDA00022662127200000219
A unit coordinate vector of (a);
Figure FDA00022662127200000220
is a rod piece
Figure FDA00022662127200000221
From the origin to the rod
Figure FDA00022662127200000222
The origin of the translation vector.
5. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
in step [ 2 ], if
Figure FDA00022662127200000223
And is
Figure FDA00022662127200000224
Then
In the formula,
Figure FDA00022662127200000226
is a rod piece
Figure FDA00022662127200000227
The origin of the rod l to the origin of the rod l;
Figure FDA00022662127200000228
is axis invariant
Figure FDA00022662127200000229
A cross-product matrix of; 03=[0 0 0]T
6. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
in step [ 2 ], if
Figure FDA00022662127200000230
And is
Figure FDA00022662127200000231
Then
Figure FDA00022662127200000232
And is
Figure FDA00022662127200000233
Is represented by the formula (12) and
Figure FDA00022662127200000234
to obtain
Figure FDA00022662127200000235
In the formula,
Figure FDA00022662127200000236
is a rod piece
Figure FDA00022662127200000237
The origin of the rod l to the origin of the rod l;is a rod piece
Figure FDA00022662127200000239
To the i' origin of the rod,
Figure FDA00022662127200000240
is a rod piece
Figure FDA00022662127200000241
From the origin to the rodThe translation vector of the origin of the image,lrl′is a translation vector from the origin of the rod l to the origin of the rod l', 03=[0 0 0]T
7. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
order toDefined by the angle of twist of the shaft
Figure FDA00022662127200000244
In the formula,
Figure FDA0002266212720000031
is a shaft
Figure FDA0002266212720000032
To the shaft
Figure FDA0002266212720000033
The twist angle of (c).
8. The method for determining D-H system and D-H parameters of an axis-invariant multi-axis robot as claimed in claim 1,
order to
Figure FDA0002266212720000034
Defined by the angle of rotation of the joint
Figure FDA0002266212720000035
In the formula,
Figure FDA0002266212720000036
is a shaft
Figure FDA0002266212720000037
Zero position of (a).
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