CN105929844B - Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing - Google Patents

Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing Download PDF

Info

Publication number
CN105929844B
CN105929844B CN201610265101.0A CN201610265101A CN105929844B CN 105929844 B CN105929844 B CN 105929844B CN 201610265101 A CN201610265101 A CN 201610265101A CN 105929844 B CN105929844 B CN 105929844B
Authority
CN
China
Prior art keywords
constraint
obstacle
raised
convex
optimal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201610265101.0A
Other languages
Chinese (zh)
Other versions
CN105929844A (en
Inventor
白成超
郭继峰
张露文
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Harbin Institute of Technology
Original Assignee
Harbin Institute of Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Harbin Institute of Technology filed Critical Harbin Institute of Technology
Priority to CN201610265101.0A priority Critical patent/CN105929844B/en
Publication of CN105929844A publication Critical patent/CN105929844A/en
Application granted granted Critical
Publication of CN105929844B publication Critical patent/CN105929844B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G05CONTROLLING; REGULATING
    • G05DSYSTEMS FOR CONTROLLING OR REGULATING NON-ELECTRIC VARIABLES
    • G05D1/00Control of position, course, altitude or attitude of land, water, air or space vehicles, e.g. using automatic pilots
    • G05D1/10Simultaneous control of position or course in three dimensions
    • G05D1/101Simultaneous control of position or course in three dimensions specially adapted for aircraft

Landscapes

  • Engineering & Computer Science (AREA)
  • Aviation & Aerospace Engineering (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Automation & Control Theory (AREA)
  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)

Abstract

Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing, belongs to Navigation, Guidance and Control technical field.The present invention, for the optimal Guidance problem under more Obstacles Constraints environment, will propose a kind of optimal soft landing method of guidance of the improvement based on convex optimization on the basis of the former.Firstly, establishing the optimal Second-order cone programming model of fuel that Obstacles Constraints are not added, and standardized;Secondly, carrying out analysis modeling for martian surface protrusion obstacle, and linear transformation is carried out, convert convex constraint for non-convex constraint, be dissolved among Second-order cone programming problem, and establishes the optimal Second-order cone programming model of complete consideration Obstacles Constraints;Carry out the correctness of verification algorithm finally by the simulation analysis of three kinds of different type Obstacles Constraints.Apply it in soft lunar landing research, simulation result shows that new algorithm realizes effectively evading for three-dimensional space obstacle, be rationally utilized around and above obstacle can flight space, while it is optimal to meet fuel.

Description

Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing
Technical field
The invention belongs to Navigation, Guidance and Control technical field, it is related to the optimal system of avoidance under a kind of more Obstacles Constraints environment Guiding method.
Background technique
Currently, for objects outside Earth soft landing process optimum guidance problems there are many approach applications wherein, but more Avoidance problem under Obstacles Constraints environment does not have preferable solution to propose yet.
Given below is the general solution for the soft landing process optimum guidance problems of objects outside Earth, process Are as follows:
In the Approach phase of entire landing mission, lander is close from menology, can ignore the shadow of moon autobiography at this time It rings, and entire kinetic model is established in a menology fixed coordinate system using landing point as origin.Menology fixed coordinates Shown in the definition of system such as Fig. 1 shows, the vertical menology of ox axis, ox, oy, tri- axis of oz composition right-handed coordinate system.
Since menology does not have air, and complicated control problem is not considered, only consider guidance problems, can obtain the dynamic of Approach phase Mechanical equation:
Wherein,
R --- it is position vector of the lander under oxyz system, r=[rx ry rz]T
V --- it is velocity vector of the lander under oxyz system, v=[vx vy vz]T
A --- it is acceleration of the lander under oxyz system, a=[ax ay az]T
gm--- it is Mars acceleration of gravity;
Tc--- for the net thrust vector (being directed toward lander central axis) of lander engine, Tc=| | Tc| |, it is that it is big It is small;
M --- it is the quality at lander per moment;
α --- it is lander engine burn-up rate, is greater than 0,(geFor terrestrial gravitation acceleration, φ hair The angle of motivation established angle, i.e. jet direction and lander central axis, IspFor engine/motor specific impulse).
Consider the rail that boundary condition, control force size constraint, the constraint of lander attitude angle and ground level constrain Mark fuel optimal problem are as follows:
Objective function:
Meet formula (1) constraint equation and following constraint:
0<T1≤Tc≤T2 (3)
rx≥0 (4)
Wherein T1、T2For control force bound;θaltAs shown in Figure 1, the inclination angle of referred to as lander,It is given for it The upper limit,The effect of the constraint is to guarantee that lander is landed with certain landing angle, without touching before landing The small protrusion of upper ground surface.From the foregoing it is appreciated that, the soft landing optimal Guidance process of existing objects outside Earth is directed to more Obstacles Constraints Avoidance problem under environment provides the scheme of efficiently solving.
Summary of the invention
The object of the present invention is to provide barrier-avoiding methods under a kind of more Obstacles Constraints environment of objects outside Earth soft landing, with solution The certainly avoidance problem during the soft landing optimal Guidance of objects outside Earth under more Obstacles Constraints environment.
The technical solution adopted by the present invention to solve the above technical problem is:
Raised Disorder Model selection
Firstly, a model space geometric is selected for the raised obstacle on menology, to be depicted with the form of mathematics Come, obstacle is made to become a state constraint in entire track optimizing problem.Selection for model, it is necessary to meet on the whole The gabarit of constraint, and there is the ability that can portray most raised obstacles.Herein, using the method for convex optimization come into Row obstacle avoidance also needs to consider selected 3-D geometric model, after mathematical description and certain mathematic(al) manipulation, energy Enough and energy be converted to convex constraint more conveniently.Menology protrusion obstacle is described as pyramid type constraint by comprehensive considerations above, As shown in Figure 2.
(a), (b) shown in Fig. 2, (c) respectively indicate three kinds of unacceptable the barrer types, and (a) is big apex angle obstacle, Qi Banding Angle is larger, and general 30 ° or more;It (b) is small apex angle obstacle, general 30 ° or less;(c) be then (b) a kind of special case, when circular cone Height acquirement is very big, and much higher than the height for the spatial point that lander may pass through, and its semiapex angle obtains very little, at this moment, circular cone The constraint of type can approximately regard that cylindrical type constrains as again, for describing the raised obstacle that those are approximately cylinder.Pass through tune The height and semiapex angle size of full circle cone carry out the raised obstacle of the overwhelming majority on approximate description menology, it can be seen that hinder protrusion Hinder be described as pyramid type constraint there is versatility.
Raised Disorder Model mathematical description
After lander scan process, can obtain these raised obstacles position and rough elevation information, Middle elevation information do not need accurately to know, generally takes a more conservative estimated value;The semiapex angle of circular cone can also be according to need The safety margin wanted takes an estimated value.In short, the circular cone volume ratio practical obstacle volume taken is bigger, safety margin is higher, More can obstacle avoidance, but can also reduce lander can flight space size.
If cone height be H_h, semiapex angle α,In the fixed landing coordinate system of menology, conical tip is sat It is designated as H=(H_h H_y H_z)T, any time, coordinate of the lander in menology fixed coordinate system is P=(x y z)T, then The cosine value of lander and the angle by the high unit vector of circular cone are as follows:
Wherein n is the unit vector on cone height direction, i.e. n=(1 0 0)T;β is the folder of P-H vector and n vector Angle.
Lander is set to avoid these raised obstacles, the flight path of lander cannot pass through these circular cones, such as Fig. 3 and 4 Shown, lander cannot be below horizontal plane flight first, followed by its line with obstacle vertex must circle element of a cone it Outside, then it needs to meetI.e.
(6) formula deform
Since the final landing point of lander is lower than the height of obstacle certainly,ToFormula (7) just become
Notice that the described constraint of formula (8) is a nonconvex property constraint, the addition of this constraint will be so that entire track Optimization and avoidance problem can not be solved with convex optimization method, therefore, it is necessary to be carried out convexification conversion.
The conversion of Obstacles Constraints convexification
Convexification conversion is carried out to nonconvex property Obstacles Constraints obtained above, is asked so that entire problem turns to a convex optimization Topic, it is more exact that turning to a Second-order cone programming problem.
It is to take single order to the norm constraint contained that by formula (8), this non-convex constraint, which turns to the general thought of convexity constraint, Taylor expansion item makes entirely constraint become a linear restriction, since linear restriction is one kind of convex constraint, also just will Obstacles Constraints are converted to convex constraint.
For convenience of solution, first vector is write as component form:
P-H=(x-H_h y-H_y z-H_z)
If f (P)=norm (P-H),
F (P) can be obtained to component first derivative each in P and to the first derivative f ' (P) of P,
Continue derivation, obtaining its second dervative is
F " (P) is a Hessian matrix, wherein
The first order Taylor of available f (P)
In above formula, 0 < ξ < 1, Pξ=P0+ξ(P-P0).Its single order linear term is taken to obtain to (14)
F (P)=f (P0)+f′(P0)(P-P0) (15)
At this moment, formula (8) constraint becomes a linear restriction
In the case where ignoring second-order remained, linear restriction described in (16) formula, the P in formula are obtained0Can take does not have The lander position at the optimization each timing node in track obtained when avoidance constraint is added, takes P in this way0It can reduce as much as possible Remainder, the linear restriction after making conversion are more constrained close to original.
Approach phase landing fuel optimal problem after Obstacles Constraints are added
DefinitionShared vc=n=[1 0 0]T, then constraint can be write as
Wherein,
The constraint is added in former problem, obtains that existing fuel is optimal, and can be realized the rail of three-dimensional space avoidance Mark optimization problem:
Target function:
Meet:
Avoidance method of guidance considers future under the more Obstacles Constraints environment of a kind of objects outside Earth soft landing proposed by the present invention The reliability and safety of moon exploration task, pinpoint soft landing and effective obstacle avoidance will play conclusive work With.Have correlation technique before and the optimum value derivation algorithm based on convex programming is proposed with regard to accurate soft landing problem, the present invention , for the optimal Guidance problem under more Obstacles Constraints environment, a kind of changing based on convex optimization will be proposed on the basis of the former Into optimal soft landing guidance algorithm.
Main advantages of the present invention are embodied in: being given the circular cone geometry teaching model of menology protrusion obstacle, given this The mathematical description of circular cone Disorder Model, then by non-convex to linear transfor, so that circular cone Obstacles Constraints are dissolved into second order cone rule In the problem of drawing, accomplishes to consider simultaneously that fuel is optimal and obstacle avoidance, the obstacle avoidance of three-dimensional space may be implemented, efficiently use Around and above obstacle can flight space, be no longer the realization obstacle avoidance in the form of plane restriction, waste obstacle about The upper space of beam.
Innovative point of the present invention is: analysis modeling carried out for the raised obstacle on ground day surface, and completes linear transfor, it will Non-convex constraint is converted into convex constraint, is dissolved among Second-order cone programming problem, and establishes the optimal of complete consideration Obstacles Constraints Second-order cone programming model demonstrates the correctness of method by the simulation analysis of three kinds of different type Obstacles Constraints, has and actually answer With value.
The present invention firstly, establishing the optimal Second-order cone programming model of fuel that Obstacles Constraints are not added, and is standardized;Its It is secondary, analysis modeling is carried out for martian surface protrusion obstacle, and carry out linear transformation, converts convex constraint for non-convex constraint, melt Enter among Second-order cone programming problem, and establishes the optimal Second-order cone programming model of complete consideration Obstacles Constraints;Finally by The simulation analysis of three kinds of different type Obstacles Constraints carrys out the correctness of verification algorithm.It applies it in soft lunar landing research, Simulation result shows that new algorithm realizes effectively evading for three-dimensional space obstacle, is rationally utilized around and above obstacle and flies Row space, while it is optimal to meet fuel.
To objects outside Earth, typically raised obstacle has carried out mathematical modeling to the present invention;Non-linear arrive has been carried out to raised obstacle Linear conversion, it is non-convex to convex conversion;The Approach phase landing fuel optimal problem after Obstacles Constraints are added is established, to tradition Soft landing optimal Guidance problem propose new thinking;By the selection to three kinds of raised Obstacles Constraints, mentioned side is demonstrated The correctness of method and feasibility in use.
Detailed description of the invention
Fig. 1 is menology fixed coordinate system, and Fig. 2 is restricted model schematic diagram, and (a), (b), (c) respectively indicate three kinds in Fig. 2 Unacceptable the barrer types, (a) are big apex angle obstacle, (b) are small apex angle obstacle, are then (c) a kind of special cases of (b).Fig. 3 constraint Model schematic;It can flight range comparison before Fig. 4 approximate processing and processing;Fig. 5 is speed change curves figure;Fig. 6 is reasoning valve Gate koji-making line chart;Fig. 7 is no avoidance track top view;Fig. 8 is that have avoidance track top view;Fig. 9, which is that 1 avoidance of obstacle is contour, to be dissipated Point diagram;Figure 10 is obstacle 1 without the high scatter plot such as avoidance;Figure 11 is the high scatter plots such as 2 avoidance of obstacle;Figure 12 is obstacle 2 without avoidance Contour scatter plot.
Specific embodiment
Specific embodiment 1: as shown in Figures 2 to 4, a kind of more obstacles of objects outside Earth soft landing described in present embodiment The realization process of barrier-avoiding method under constraint environment are as follows:
Step 1: the raised obstacle for objects outside Earth surface is analyzed and constructs raised obstacle mathematical model;
Step 2: the raised obstacle mathematical model is carried out linear transfor, convex constraint is converted by non-convex constraint;
Step 3: the raised obstacle mathematical model after linear transfor is dissolved among Second-order cone programming problem, and establish The optimal Second-order cone programming model of complete consideration Obstacles Constraints;
Step 4: more using the optimal Second-order cone programming model realization objects outside Earth soft landing of complete consideration Obstacles Constraints Optimal avoidance under Obstacles Constraints environment.
Specific embodiment 2: in present embodiment, the raised obstacle described in step 1 for objects outside Earth surface It is analyzed and constructs raised obstacle mathematical model, detailed process are as follows:
Step 1 one, raised Disorder Model selection
The raised Disorder Model of selection meets the gabarit of constraint on the whole, and hinders with that can portray most protrusions The ability hindered;
Obstacle avoidance is carried out using the method for convex optimization, selected 3-D geometric model can be converted to convex constraint, Moonscape protrusion obstacle is described as pyramid type constraint;
By adjusting the height and semiapex angle size of circular cone, carry out the raised obstacle of the overwhelming majority on approximate description menology, it will It is with versatility that raised obstacle, which is described as pyramid type constraint,;
Step 1 two, raised Disorder Model mathematical description
After lander scan process, position and the elevation information of raised obstacle are obtained;
The semiapex angle of circular cone safety margin as needed takes an estimated value;If cone height be H_h, semiapex angle α,In the fixed landing coordinate system of menology, conical tip coordinate is H=(H_h H_y H_z)T, any time, Coordinate of the land device in menology fixed coordinate system is P=(x y z)T, then lander and the folder by the high unit vector of circular cone Cosine of an angle value are as follows:
Wherein n is the unit vector on cone height direction, i.e. n=(1 0 0)T;β is the folder of P-H vector and n vector Angle;
Lander is set to avoid the raised obstacle, the flight path of lander cannot pass through these circular cones, and lander is first It first cannot be below horizontal plane flight, followed by it then must need to meet with the line on obstacle vertex except circle element of a coneI.e.
(6) formula deform
Since the final landing point of lander is lower than the height of obstacle certainly,ToFormula (7) just become
The described constraint of formula (8) is a nonconvex property constraint, and the addition of nonconvex property constraint will be so that entire track optimizing And avoidance problem can not be solved with convex optimization method, therefore, it is necessary to be carried out convexification conversion.
Other steps are same as the specific embodiment one.
Specific embodiment 3: as shown in Figures 2 to 4, present embodiment is described by the raised obstacle in step 2 Mathematical model carries out linear transfor, converts convex constraint (conversion of Obstacles Constraints convexification), detailed process for non-convex constraint are as follows:
Convexification conversion is carried out to nonconvex property Obstacles Constraints, so that entire problem turns to a convex optimization problem, it is more acurrate Be to turn to a Second-order cone programming problem;
It is that one is taken to the norm constraint contained by the general thought that non-convex constraint turns to the constraint of a convexity shown in formula (8) Rank Taylor expansion item makes entirely constraint become a linear restriction, since linear restriction is one kind of convex constraint, also just will Obstacles Constraints are converted to convex constraint;
For convenience of solution, first vector is write as component form:
P-H=(x-H_h y-H_y z-H_z)
If f (P)=norm (P-H),
F (P) can be obtained to component first derivative each in P and to the first derivative f ' (P) of P,
Continue derivation, obtaining its second dervative is
F " (P) is a Hessian matrix, wherein
The first order Taylor of available f (P)
In above formula, 0 < ξ < 1, Pξ=P0+ξ(P-P0);Its single order linear term is taken to obtain to (14)
F (P)=f (P0)+f′(P0)(P-P0) (15)
At this moment, formula (8) constraint becomes a linear restriction
In the case where ignoring second-order remained, linear restriction described in (16) formula, the P in formula are obtained0It takes and is not added The lander position at the optimization each timing node in track that avoidance obtains when constraining, takes P in this way0It can reduce as much as possible remaining , the linear restriction after making conversion is more constrained close to original.
F (P) is the Taylor expansion of pure mathematics, is explained without what meaning.Here P is exactly to represent lander to consolidate in menology Three-dimensional coordinate under position fixing system.f″(Pξ) it is exactly 2 order derivatives;ξ(P-P0) it is in P0A certain neighborhood in.
Other steps are the same as one or two specific embodiments.
Specific embodiment 4: present embodiment is in step 3, the raised obstacle mathematics by after linear transfor Model is dissolved among Second-order cone programming problem, and establishes the optimal Second-order cone programming model of complete consideration Obstacles Constraints, tool Body process are as follows:
DefinitionShared vc=n=[1 0 0]T, then constraint is write as
Formula (17) is exactly to derive to the deformation constrained above, and Q is intermediate variable, and it is following described for being worth;
Wherein,
The constraint is added in former problem, obtains that fuel is optimal, and realizes that the track optimizing of three-dimensional space avoidance is asked The target function of topic:
Target function:
Meet:
Wherein:
Eu=[I3 03×1],Ex=[I6 06×1],γk=[04×4k I6 04×4(n-k)]4×4(n+1), (k=0,1 ..., n)
A∈R7×7,B∈R7×4
Other steps are identical as specific embodiment one, two or three.
The present invention and its technical effect generated are described in more detail with reference to the accompanying drawing:
Simulation parameter design
It is emulated using MATLAB yalmip Optimization Toolbox.Simulation parameter such as table 1.
The setting of 1 initial parameter of table
Table1 Initial parameters:
Take two obstacles as multiple obstacle simulation examples here.It is as follows:
Obstacle 1: apex coordinate [500 40-83], 10 ° of obstacle semiapex angle, relaxation factor 1.
Obstacle 2: apex coordinate [1500 50-350], 10 ° of obstacle semiapex angle, relaxation factor 1.
Analysis of simulation result
Fig. 5,6 give the velocity variations and thrust valve door controlling curve of lander.Final hovering coordinate is [30.8091 -0.477208 -0.266704] m, speed are [- 0.49179 0.028592 0.081788]m/s.Meet the requirements model It encloses, it was demonstrated that the correctness of constraint.
Fig. 7,8 give not plus Obstacles Constraints and have added Obstacles Constraints optimization track in three dimensions and its plane Projection.It apparent can be observed from two top views, before adding avoidance, the journey overwhelming majority is same behind original optimization track In one plane, two size obstacles are passed through, are not passed through the center of obstacle certainly;In addition avoidance optimization track exists after avoidance Journey not in the same plane, but makees to evade among two size obstacles flight afterwards, and substantially it is seen that with around Winged form carrys out obstacle avoidance.
Four contour scatter plots shown in Fig. 9~12, which give, to be added avoidance and does not add avoidance flight path respectively with respect to two The change in location of obstacle.Not plus before avoidance, the point between x=961.5261 to x=673.482 is inside obstacle 2, x= 366.541 to the point between x=186.1168 inside obstacle 1, namely former optimization track has greatly in two barriers Hinder inside;In addition all the points press the tendency direction of each node all except the circle of corresponding height after avoidance, adjacent two The line of point does not all have intersection point with inner circle (the smaller circle of line side radius), namely does not have two o'clock line across obstacle Situation illustrates that lander successfully avoids obstacle, and flight path is bonded compared with obstacle, and taking full advantage of can flight space.
Can to sum up obtain, by the way that conical Obstacles Constraints are added, using Second-order cone programming method, realize fuel it is optimal and Two purposes of obstacle avoidance.Emulation gives the simulation result of three kinds of small apex angle, big apex angle, more obstacles different type obstacles, from Simulation result above finds out that this method is more satisfactory.
In addition, the very low obstacle of some height can also use model above to add entire optimization problem as Obstacles Constraints In, but general restriction acts on very little, what effect do not had in exhausted big a part of flight course, is only contacted to earth in lander One section of preceding track can just play effect of contraction, and at this moment these constraints can be handled as plane restriction substantially.

Claims (1)

1. barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing, which is characterized in that the realization of the method Journey are as follows:
Step 1: the raised obstacle for objects outside Earth surface is analyzed and constructs raised obstacle mathematical model;
Step 2: the raised obstacle mathematical model is carried out linear transfor, convex constraint is converted by non-convex constraint;
Step 3: the raised obstacle mathematical model after linear transfor is dissolved among Second-order cone programming problem, and establish complete The considerations of Obstacles Constraints optimal Second-order cone programming model;
Step 4: utilizing the more obstacles of optimal Second-order cone programming model realization objects outside Earth soft landing of complete consideration Obstacles Constraints Optimal avoidance under constraint environment;
Raised obstacle mathematical model is analyzed and constructed to raised obstacle described in step 1 for objects outside Earth surface, tool Body process are as follows:
Step 1 one, raised Disorder Model selection
The raised Disorder Model of selection meets the gabarit of constraint on the whole, and has and can portray most raised obstacles Ability;
Obstacle avoidance is carried out using the method for convex optimization, selected 3-D geometric model can be converted to convex constraint, by the moon Ball surface protrusion obstacle is described as pyramid type constraint;
By adjusting the height and semiapex angle size of circular cone, carry out the raised obstacle of the overwhelming majority on approximate description menology, it will be raised It is with versatility that obstacle, which is described as pyramid type constraint,;
Step 1 two, raised Disorder Model mathematical description
After lander scan process, position and the elevation information of raised obstacle are obtained;
The semiapex angle of circular cone safety margin as needed takes an estimated value;If cone height be H_h, semiapex angle α,In the fixed landing coordinate system of menology, conical tip coordinate is H=(H_h H_y H_z)T, any time, Coordinate of the land device in menology fixed coordinate system is P=(x y z)T, then lander and the folder by the high unit vector of circular cone Cosine of an angle value are as follows:
Wherein n is the unit vector on cone height direction, i.e. n=(1 0 0)T;β is the angle of P-H vector and n vector;
Lander is set to avoid the raised obstacle, the flight path of lander cannot pass through these circular cones, and lander is first not It can fly lower than horizontal plane, followed by it then must need to meet with the line on obstacle vertex except circle element of a coneI.e.
(6) formula deform
Since the final landing point of lander is lower than the height of obstacle certainly,ToFormula (7) is just Become
The described constraint of formula (8) is a nonconvex property constraint, and the addition of nonconvex property constraint will be so that entire track optimizing and keep away Barrier problem can not be solved with convex optimization method, therefore, it is necessary to be carried out convexification conversion;
It is described that the raised obstacle mathematical model is subjected to linear transfor in step 2, convex constraint is converted by non-convex constraint, Detailed process are as follows:
Convexification conversion is carried out to nonconvex property Obstacles Constraints, so that entire problem turns to a convex optimization problem, it is more exact that Turn to a Second-order cone programming problem;
It is to take single order safe to the norm constraint contained by the general thought that non-convex constraint shown in formula (8) turns to the constraint of a convexity Expansion item is strangled, so that entirely constraint is become a linear restriction, since linear restriction is one kind of convex constraint, also just by obstacle Constraints conversion is at convex constraint;
For convenience of solution, first vector is write as component form:
P-H=(x-H_h y-H_y z-H_z)
If f (P)=norm (P-H),
F (P) can be obtained to component first derivative each in P and to the first derivative f ' (P) of P,
Continue derivation, obtaining its second dervative is
F " (P) is a Hessian matrix, wherein
The first order Taylor of available f (P)
In above formula, 0 < ξ < 1, Pξ=P0+ξ(P-P0);Its single order linear term is taken to obtain to (14)
F (P)=f (P0)+f′(P0)(P-P0) (15)
At this moment, formula (8) constraint becomes a linear restriction
In the case where ignoring second-order remained, linear restriction described in (16) formula, the P in formula are obtained0It takes and avoidance is not added about The lander position at the optimization each timing node in track obtained when beam, takes P in this way0Remainder can be reduced as much as possible, make to turn Linear restriction after changing more is constrained close to original;
In step 3, the raised obstacle mathematical model by after linear transfor is dissolved among Second-order cone programming problem, and Establish the optimal Second-order cone programming model of complete consideration Obstacles Constraints, detailed process are as follows:
DefinitionShared vc=n=[1 0 0]T, then constraint is write as
Wherein,
The constraint is added in former problem, obtains that fuel is optimal, and realize the track optimizing problem of three-dimensional space avoidance Target function:
Target function:
Meet:
||SΨkp+S(Φky0kg4)||≤-cTΨkp-cTky0kg4)
Wherein:
C=[- tan (θalt) 0 0 0 0 0 0]T
eσ=[01×31]T,ez=[01×6 1]T,eh=[1 01×6]T,Eu= [I3 03×1],Ex=[I6 06×1],Υk=[04×4k I6 04×4(n-k)]4×4(n+1), (k=0,1 ..., n) A ∈ R7×7,B∈R7×4
CN201610265101.0A 2016-04-26 2016-04-26 Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing Active CN105929844B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610265101.0A CN105929844B (en) 2016-04-26 2016-04-26 Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610265101.0A CN105929844B (en) 2016-04-26 2016-04-26 Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing

Publications (2)

Publication Number Publication Date
CN105929844A CN105929844A (en) 2016-09-07
CN105929844B true CN105929844B (en) 2019-01-08

Family

ID=56836225

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610265101.0A Active CN105929844B (en) 2016-04-26 2016-04-26 Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing

Country Status (1)

Country Link
CN (1) CN105929844B (en)

Families Citing this family (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108120442B (en) * 2017-12-12 2021-02-12 北京理工大学 Multi-rotor unmanned aerial vehicle flight path generation method based on second-order cone planning
CN108388135B (en) * 2018-03-30 2020-11-10 上海交通大学 Mars landing trajectory optimization control method based on convex optimization
CN109540126B (en) * 2018-12-03 2020-06-30 哈尔滨工业大学 Inertial vision integrated navigation method based on optical flow method
CN109828600B (en) * 2019-01-09 2020-07-24 北京理工大学 Time-optimal rapid three-dimensional obstacle avoidance path planning method
CN110542423B (en) * 2019-07-23 2021-06-11 北京控制工程研究所 Moon soft landing vertical approach obstacle avoidance guidance method
CN111486851B (en) * 2020-04-27 2021-09-03 中国人民解放军国防科技大学 Method and device for planning short-distance relative motion three-dimensional obstacle avoidance track of spacecraft
CN111982129B (en) * 2020-08-24 2022-03-08 哈尔滨工业大学 Comprehensive global path planning method based on lunar surface digital elevation map
CN112051854B (en) * 2020-09-23 2021-07-16 北京理工大学 Rapid planning method for optimal trajectory of lunar soft landing considering complex constraints
CN112507461B (en) * 2020-12-15 2021-07-23 北京航天自动控制研究所 Starting method of engine at power soft landing stage of carrier rocket
CN112644738B (en) * 2021-01-19 2021-09-17 哈尔滨工业大学 Planet landing obstacle avoidance trajectory constraint function design method
CN112987783A (en) * 2021-02-18 2021-06-18 北京理工大学 Complex small celestial body surface landing obstacle avoidance constant thrust control method
CN113124878B (en) * 2021-04-21 2023-12-22 哈尔滨工业大学 Moon surface large-scale road topology network construction method, system and device
CN113296536B (en) * 2021-05-24 2022-04-05 哈尔滨工业大学 Unmanned aerial vehicle three-dimensional obstacle avoidance algorithm based on A-star and convex optimization algorithm
CN113232025B (en) * 2021-06-07 2022-04-22 上海大学 Mechanical arm obstacle avoidance method based on proximity perception
CN113467241B (en) * 2021-07-06 2022-09-16 北京理工大学 Method for optimizing burn-up of convex curvature landing track
CN113917943B (en) * 2021-10-14 2022-07-12 哈尔滨工业大学 Moon soft landing optimal guidance method and system based on safe landing passage and storage medium
CN117806333B (en) * 2024-02-29 2024-05-24 北京大学 Target tracking track planning method and device for maintaining visibility in complex environment

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102800189A (en) * 2012-07-22 2012-11-28 江南大学 Method for optimizing intelligent parking path in environment of Internet of things
CN103487802A (en) * 2013-09-18 2014-01-01 电子科技大学 Scanning radar angle super-resolution imaging method
CN104238565A (en) * 2014-09-30 2014-12-24 清华大学 Robust control and distribution method applied to fault-tolerant flight control system

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070179685A1 (en) * 2005-09-29 2007-08-02 Mark Milam Trajectory generation using non-uniform rational B-splines

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102800189A (en) * 2012-07-22 2012-11-28 江南大学 Method for optimizing intelligent parking path in environment of Internet of things
CN103487802A (en) * 2013-09-18 2014-01-01 电子科技大学 Scanning radar angle super-resolution imaging method
CN104238565A (en) * 2014-09-30 2014-12-24 清华大学 Robust control and distribution method applied to fault-tolerant flight control system

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
Behcşet Acşıkmesşe.ETC.Enhancements on the Convex Programming Based Powered Descent Guidance Algorithm for Mars Landing.《AIAA/AAS Astrodynamics Specialist Conference》.2008,
Ronald R Sostaric.Powered descent trajectory guidance and some con-siderations for human lunar landing.《AAS 30th AnnualAAS Guidance and Control Conference》.2007,
林晓辉等.基于凸优化理论的含约束月球定点着陆轨道优化.《宇航学报》.2013,

Also Published As

Publication number Publication date
CN105929844A (en) 2016-09-07

Similar Documents

Publication Publication Date Title
CN105929844B (en) Barrier-avoiding method under a kind of more Obstacles Constraints environment of objects outside Earth soft landing
CN103728980A (en) Spacecraft relative orbit control method
CN104267734B (en) A kind of Mars complex topographic area safe landing orbit generation method of optimal-fuel
CN104309822B (en) A kind of spacecraft single impulse water-drop-shaped based on parameter optimization is diversion track Hovering control method
Wallace et al. Orbital operations for Phobos and Deimos exploration
Liu Autonomous trajectory planning by convex optimization
Sands et al. Nonredundant single-gimbaled control moment gyroscopes
CN103926835A (en) Lander power descending branch optimal control method based on disturbance observer
CN109696917A (en) A kind of spacecraft intersects barrier-avoiding method and system automatically
Munoz Rapid path-planning algorithms for autonomous proximity operations of satellites
CN108614420A (en) Star cluster grade satellite fault tolerant control method based on Non-Linear Programming
CN110562493A (en) Mars power descending trajectory planning method based on vector trajectory
CN105912819A (en) Quick design method of earth-moon L1 Lagrange point transfer orbit
Starek et al. Real-time, propellant-optimized spacecraft motion planning under Clohessy-Wiltshire-Hill dynamics
Wilmer Space domain awareness assessment of cislunar periodic orbits for lagrange point surveillance
Parker Targeting low-energy ballistic lunar transfers
Chen et al. Integrated guidance and control for microsatellite real-time automated proximity operations
Li et al. Optimal real-time approach and capture of uncontrolled spacecraft
Crews Increasing slew performance of reaction wheel attitude control systems
Saeki et al. Analytical and experimental investigation of base–extension separation mechanism for spacecraft landing
Çelik et al. Reliability analysis of ballistic landing in binary asteroid 65803 (1996GT) Didymos under uncertainty and GNC error considerations
Chen et al. Trajectory design for the Moon departure libration point mission in full ephemeris model
JP2023031461A (en) Satellite constellation formation method, satellite constellation, and analyzer
Shi et al. Trajectory optimization for proximity operations around tumbling geometrical constraints via legendre polynomials
Tang et al. Dynamic and sliding mode control of space netted pocket system capturing and attitude maneuver non-cooperative target

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant