CN113639946B - Method for determining mechanism bumping and vibrating conditions during movement of patrol device - Google Patents

Method for determining mechanism bumping and vibrating conditions during movement of patrol device Download PDF

Info

Publication number
CN113639946B
CN113639946B CN202110928297.8A CN202110928297A CN113639946B CN 113639946 B CN113639946 B CN 113639946B CN 202110928297 A CN202110928297 A CN 202110928297A CN 113639946 B CN113639946 B CN 113639946B
Authority
CN
China
Prior art keywords
patrol
wheels
planet
bumping
determining
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
CN202110928297.8A
Other languages
Chinese (zh)
Other versions
CN113639946A (en
Inventor
党兆龙
陈百超
彭松
潘冬
邹猛
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.)
Jilin University
Beijing Institute of Spacecraft System Engineering
Original Assignee
Jilin University
Beijing Institute of Spacecraft System Engineering
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 Jilin University, Beijing Institute of Spacecraft System Engineering filed Critical Jilin University
Priority to CN202110928297.8A priority Critical patent/CN113639946B/en
Publication of CN113639946A publication Critical patent/CN113639946A/en
Application granted granted Critical
Publication of CN113639946B publication Critical patent/CN113639946B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01MTESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
    • G01M7/00Vibration-testing of structures; Shock-testing of structures
    • G01M7/02Vibration-testing by means of a shake table

Abstract

The invention discloses a method for determining a mechanism bumping and vibrating condition when a patrol device moves, which comprises the following steps: determining an unevenness parameter according to the landing area range of the patrol instrument and the statistical characteristics of the surface topography of the planet; determining the maximum amplitude of the patrol instrument during bumping and vibration according to the obstacle crossing height index of the patrol instrument and by combining the wheel layout characteristics of the patrol instrument and the gravitational acceleration of the surface of a planet; and determining the fundamental frequency of the bumping vibration according to the contact length of the wheels of the patrol device or the unevenness of the ground and the moving speed. The invention can determine the bumping environment of the patrol instrument in the moving process and provide test conditions for developing the research and test of an organization.

Description

Method for determining mechanism bumping and vibrating conditions during movement of patrol device
Technical Field
The invention belongs to the field of deep space exploration, and particularly relates to a method for determining a mechanism bumping and vibrating condition when a patrol device moves.
Background
When the patrol instrument moves on the surface of a planet (moon and mars), the mechanism on the patrol instrument is in a vibration state due to the complexity of the terrain on the surface of the planet and the soil environment, so that the bumping phenomenon is generated. The occurrence of the pitching phenomenon comes from two aspects: on one hand, the surface of the planet is distributed with impact pits, stones and other unstructured landforms; another aspect is the mobile device nature of the rover. The two components act together to transfer uneven terrain on the surface of the planet to the vehicle body through the wheels and the suspension, and then to a mechanism arranged on the vehicle body.
The topography of the surface of the planet can be divided into features such as slopes, impact pits, rocks and the like; for a specific detection task, the landform and landform characteristics of a landing area are generally concerned, and high-resolution landform data of the landing area can be obtained through remote sensing and other means; for the case of lack of landform data of the landing zone, the landform characteristics of the similar area can be used for approximation.
1) Lunar and Mars surface topography:
the lunar surface terrain is divided into a lunar sea area and a high land area; the moon sea is divided into flat moon sea and rugged moon sea; typical features of lunar terrain are impact pits, slopes, and rocks. The distribution of the impact pits is described by the diameter of the impact pits and the number of the impact pits larger than the diameter; the slope is divided into areas such as flat moons, rugged moons and high lands for description, and a numerical relation curve between a slope base line and the average slope is obtained. The rock also obtains corresponding rock diameter and rock number curve larger than the diameter according to the difference of the distribution area; these are obtained by processing the obtained graphic data in a certain range and can be used as the preliminary basis for developing the research of the landing zone; with the development of the lunar orbit detection technology, a lunar high-precision topographic map is obtained, and topographic analysis of a landing zone can be carried out according to the lunar high-precision topographic map; the traditional power spectrum-based terrain statistical distribution is not used, and high-precision lunar terrain data are directly used.
Taking the lunar surface unevenness as an example, the typical lunar surface unevenness statistical property is shown in fig. 1, and as can be seen from fig. 1, the lunar surface unevenness can be divided into three areas, namely, flat moon (Smooth Mare), rugged moon (Rough Mare), and high land (Rough Upland/hummocky Upland); also shown in fig. 1 are the unevenness of two terrains (Grass Runway and Bonita lavaFlow, Ariz) on the earth.
Compared with lunar terrain, more stones are distributed on the surface of the mars; the distribution of the stones on the surface of the spark is generally exemplified by the number of the occupied areas of the stones; for example, NASA has a statistical distribution of rocks around Pathfinder patrollers with a mean surrounding stone distribution of 18.7%, a minimum of 6.7%, and a maximum of 44.9%.
The topographic features of the surfaces of the moon and the mars are input conditions of jolting and vibration when the development patrol device moves, so that a surface digital elevation model needs to be established according to typical features such as impact pits, stones, slopes and the like.
2) The moving performance of the patrol device is as follows:
when the patrol device moves on the surface of the planet, certain moving capacity is required to be achieved, and a patrol detection task is achieved; the moving capability generally comprises moving speed, obstacle crossing height, maneuvering capability, climbing capability and the like; due to the restriction of the resources of the patrol device, the items of the mobility are required in an independent mode, so that the waste of the resources caused by the overlapping requirements is avoided; for example, the obstacle crossing height index generally refers to the obstacle crossing height on the horizontal ground, and no special requirement is imposed on the obstacle crossing capability on a slope; taking the three-number or four-number Chang E patrol device in China as an example, the moving device adopts a passive main rocker arm and an auxiliary rocker arm plus 6 wheels which are independently driven.
The moving speed is 200m/h, the obstacle crossing height is 200mm, and the maneuvering capability has the pivot steering and the steering between the marching (the steering radius is not more than 1.5 m); the climbing capability is not lower than 20 degrees; when the patrol instrument turns and climbs on the surface of the planet, the surface is flat, so that the mechanism on the patrol instrument cannot shake; only in the obstacle crossing process, the processes of the wheels encountering obstacles, rolling up the obstacles, leaving the obstacles and the like exist, so that the height of wheel axles of the wheels is changed, and the height of a vehicle body is further changed; the shape of the obstacle is shown in fig. 2 to 4, taking a step as an example, and the obstacle crossing process is shown in fig. 2.
Disclosure of Invention
The invention aims to provide a method for determining a mechanism bumping and vibrating condition when a patrol device moves.
A method for determining a mechanism bumping vibration condition when a tour device moves comprises the following steps:
1) the vibration amplitude is based on the obstacle crossing capability of the inspection tour; determining the height of the wheel during obstacle crossing as the maximum amplitude of the bumping vibration according to the obstacle crossing height index of the patrol device and by combining the wheel layout characteristics of the patrol device and the gravity acceleration of the surface of a planet, thereby determining the amplitude of the bumping vibration condition;
2) the fundamental frequency characteristic is based on the contact length and the moving speed of the wheel of the rover; the contact length of the wheel of the patrol instrument is comprehensively determined according to the weight of the patrol instrument on the surface of the planet, the pressure bearing characteristic of the star soil, the width and the diameter D of the wheel and the topographic factors of the surface of the planet.
3) And determining the fundamental frequency condition of the bumping vibration according to the surface unevenness parameter of the planet of the patrolling device and the moving speed of the patrolling device.
The invention has the beneficial effects that:
by adopting the determination method, the maximum amplitude of the patrol instrument during bumping and vibrating can be determined according to the obstacle crossing height index of the patrol instrument and by combining the wheel layout characteristics of the patrol instrument and the gravity acceleration of the surface of a planet; determining the fundamental frequency during bumping and vibration according to the contact length and the moving speed of the wheels of the patrol device; according to the two conditions, the bump test condition in the development process of the patrol instrument mechanism can be determined, and the test condition is created for detecting whether the mechanism meets the requirement of the movement of the star surface of the patrol instrument.
Drawings
FIG. 1 is a graph of statistical characteristics of lunar surface irregularities;
FIG. 2 is a schematic view of the traversing device traveling on level ground during the traversing process;
FIG. 3 is a schematic diagram of the crossing of the steps on the front wheels of the inspection device in the obstacle crossing process of the inspection device;
fig. 4 is a schematic diagram of the obstacle crossing process of the patrolling device, wherein the front wheels and the middle wheels of the patrolling device go up the steps.
Detailed Description
A method for determining a mechanism bumping vibration condition when a tour device moves comprises the following steps:
1) determining an unevenness parameter according to the landing area range of the patrol instrument and the statistical characteristics of the surface topography of the planet;
2) and determining the amplitude condition of the bumping vibration according to the obstacle crossing index of the patrol instrument and the surface gravity acceleration of the target planet required to run by the patrol instrument.
The obstacle crossing height of the patrol instrument is H, and the gravity acceleration of the surface of the planet is gpThe total number of wheels is 2 n. The patrol bump occurs when the patrol crosses an obstacle, and the maximum bump occurs when two wheels on the same side cross the obstacle. For example, a rover has 6 wheels, 3 wheels on one side, and a primary and secondary rocker arm suspension is used. The distances between the front wheels and the middle wheels and between the middle wheels and the rear wheels are equal. The maximum jounce amplitude of the rover then occurs when either the two front wheels or the two rear wheels cross the obstacle; the maximum bump amplitude calculation formula of the patrol instrument vehicle body is as follows:
Figure BDA0003209940460000041
in the ground test, the equivalent amplitude of the pitching vibration is as follows:
Figure BDA0003209940460000042
for a Mars rover, for example, the gravitational acceleration of the Mars surface is
Figure BDA0003209940460000043
The obstacle crossing height is 300mm, and the equivalent amplitude of the pitching vibration is 75 mm.
3) And determining the fundamental frequency condition of the bumping vibration according to the surface unevenness parameter of the planet of the patrolling device and the moving speed of the patrolling device.
The contact length of the wheel of the patrol instrument is comprehensively determined according to the weight of the patrol instrument on the surface of the planet, the pressure bearing characteristic of the star soil, the width and the diameter D of the wheel, the topography of the surface of the planet and other factors. The wheel-to-ground contact length L of the rover wheel can be estimated according to 2/3 of the wheel radius. The moving speed v is the maximum speed of the rover on the horizontal shape of the surface of the planet.
Figure BDA0003209940460000051
Where λ is the wavelength of the Mars surface topography, and is a value of 1/4 that is close to the contact length based on the surface roughness of the planet.
For example, in the case of a Mars rover, the wheel radius of a Mars vehicle is 150mm, and the maximum speed v on a horizontal terrain with a Mars surface is 200m/h 0.05 m/s. The wheel soil contact length is about 0.1m, then f 2 Hz.

Claims (1)

1. A method for determining a mechanism bumping vibration condition when a tour device moves is characterized by comprising the following steps: the method comprises the following steps:
1) the vibration amplitude is based on the obstacle crossing capability of the inspection tour; determining the height of the wheel during obstacle crossing as the maximum amplitude of the bumping vibration according to the obstacle crossing height index of the patrol device and by combining the wheel layout characteristics of the patrol device and the gravity acceleration of the surface of a planet, thereby determining the amplitude of the bumping vibration condition;
2) the fundamental frequency characteristic is based on the contact length and the moving speed of the wheel of the rover; the contact length of the wheel of the patrol instrument is comprehensively determined according to the weight of the patrol instrument on the surface of the planet, the pressure bearing characteristic of the star soil, the width and the diameter D of the wheel and the topographic factors of the surface of the planet;
3) determining the fundamental frequency condition of the bumping vibration according to the surface unevenness parameter of the planet of the patrolling device and the moving speed of the patrolling device;
the obstacle crossing height of the patrolling device is H, and the gravity acceleration of the surface of the planet is gpThe total number of wheels is 2 n; the patrol device jounces when the patrol device crosses an obstacle, the maximum jounce occurs when two wheels on the same side cross the obstacle, and when the patrol device is provided with 6 wheels, and the number of the wheels on one side is 3, a main rocker arm suspension and an auxiliary rocker arm suspension are adopted; the distances between the front wheels and the middle wheels and between the middle wheels and the rear wheels are equal, so that the maximum bump amplitude of the patrol instrument is calculated when the two front wheels or the two rear wheels cross the obstacle, and the maximum bump amplitude calculation formula of the patrol instrument body is as follows:
Figure FDA0003519910010000011
in the ground test, the equivalent amplitude of the pitching vibration is as follows:
Figure FDA0003519910010000012
the contact length L of the wheels of the patrol device is estimated according to 2/3 of the radius of the wheels; the moving speed v is the maximum speed of the patrol device on the horizontal shape of the surface of the planet;
Figure FDA0003519910010000021
where λ is the wavelength of the Mars surface topography, and is a value of 1/4 which is close to the contact length, based on the surface roughness of the planet.
CN202110928297.8A 2021-08-13 2021-08-13 Method for determining mechanism bumping and vibrating conditions during movement of patrol device Active CN113639946B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110928297.8A CN113639946B (en) 2021-08-13 2021-08-13 Method for determining mechanism bumping and vibrating conditions during movement of patrol device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110928297.8A CN113639946B (en) 2021-08-13 2021-08-13 Method for determining mechanism bumping and vibrating conditions during movement of patrol device

Publications (2)

Publication Number Publication Date
CN113639946A CN113639946A (en) 2021-11-12
CN113639946B true CN113639946B (en) 2022-04-08

Family

ID=78421461

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110928297.8A Active CN113639946B (en) 2021-08-13 2021-08-13 Method for determining mechanism bumping and vibrating conditions during movement of patrol device

Country Status (1)

Country Link
CN (1) CN113639946B (en)

Family Cites Families (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3990039A (en) * 1975-04-07 1976-11-02 Miller Larry D Tuned ground motion detector utilizing principles of mechanical resonance
US8091833B2 (en) * 2008-02-29 2012-01-10 Insitu, Inc. Vibration isolation devices and associated systems and methods
CN103921955A (en) * 2014-03-28 2014-07-16 北京空间飞行器总体设计部 Patroller pit digging and attitude adjusting method for moon probe projects
CN106383367B (en) * 2015-07-31 2018-07-10 中国计量科学研究院 Absolute gravity measurement method and apparatus
CN109018056B (en) * 2018-08-09 2021-03-16 北京航空航天大学 Multifunctional bionic robot system with two-foot four-wheel variable walking mechanism
CN109094676B (en) * 2018-08-22 2021-05-14 北京理工大学 Ejection mechanism based on spring energy storage
CN110929402A (en) * 2019-11-22 2020-03-27 哈尔滨工业大学 Probabilistic terrain estimation method based on uncertain analysis
CN111238848B (en) * 2020-01-22 2022-08-19 哈尔滨工业大学 Vibration loading mechanism and performance testing device for Mars vehicle moving system

Also Published As

Publication number Publication date
CN113639946A (en) 2021-11-12

Similar Documents

Publication Publication Date Title
Heverly et al. Traverse performance characterization for the Mars Science Laboratory rover
Wakabayashi et al. Design and mobility evaluation of tracked lunar vehicle
Wettergreen et al. Design and field experimentation of a prototype lunar prospector
Du et al. Numerical analysis on tractive performance of off-road wheel steering on sand using discrete element method
CN113639946B (en) Method for determining mechanism bumping and vibrating conditions during movement of patrol device
Wang et al. Dynamic rocker-bogie: kinematical analysis in a high-speed traversal stability enhancement
Wasfy et al. Next-generation NATO reference mobility model complex terramechanics–Part 2: Requirements and prototype
Toha et al. System modelling of rocker-bogie mechanism for disaster relief
Li et al. Design and analysis of steering and lifting mechanisms for forestry vehicle chassis
Arunkumar et al. Optimum Design of Stair-Climbing Robots Using Taguchi Method.
Yang et al. Mechanical analysis and performance optimization for the lunar rover’s vane-telescopic walking wheel
Dunker et al. A biologically inspired robot for lunar in-situ resource utilization
Wallin et al. Learning multiobjective rough terrain traversability
CN114182604B (en) Vibrating robot
CN109278884A (en) A kind of walking dolly
Nishio et al. Study of a Planetary Exploration Rover with a Hinge-type Center-of-gravity Shift Mechanism
McTamaney et al. Mars Rover concept development
Ibrahim et al. Effects of Wheel Grouser Angle of Attack on Simulated Robot Wheel Performance on Soft Sand with High Slip Condition
Leppänen Automatic locomotion mode control of wheel-legged robots
Calleja-Huerta et al. Vertical and horizontal stresses from a lightweight autonomous field robot during repeated wheeling
Sravya et al. Design and simulation of interplanetary lunar rover
Hamid et al. Ugv locomotion system for rough terrain
Zhang et al. Lin Li
JP2020168970A (en) Unmanned survey vehicle
Łopatka et al. Loads analysis of skid steer robot drive system

Legal Events

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