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Frontiers of Mechanical Engineering

ISSN 2095-0233

ISSN 2095-0241(Online)

CN 11-5984/TH

Postal Subscription Code 80-975

2018 Impact Factor: 0.989

Front. Mech. Eng.    2023, Vol. 18 Issue (2) : 24    https://doi.org/10.1007/s11465-022-0740-0
RESEARCH ARTICLE
Design of a novel side-mounted leg mechanism with high flexibility for a multi-mission quadruped earth rover BJTUBOT
Yifan WU, Sheng GUO(), Luquan LI, Lianzheng NIU, Xiao LI
School of Mechanical, Electronic and Control Engineering, Beijing Jiaotong University, Beijing 100044, China
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Abstract

Earth rover is a class of emerging wheeled-leg robots for nature exploration. At present, few methods for these robots’ leg design utilize a side-mounted spatial parallel mechanism. Thus, this paper presents a complete design process of a novel 5-degree-of-freedom (5-DOF) hybrid leg mechanism for our quadruped earth rover BJTUBOT. First, a general approach is proposed for constructing the novel leg mechanism. Subsequently, by evaluating the basic locomotion task (LT) of the rover based on screw theory, we determine the desired motion characteristic of the side-mounted leg and carry out its two feasible configurations. With regard to the synthesis method of the parallel mechanism, a family of concise hybrid leg mechanisms using the 6-DOF limbs and an L1F1C limb (which can provide a constraint force and a couple) is designed. In verifying the motion characteristics of this kind of leg, we select a typical (3-UPRU&RRRR)&R mechanism and then analyze its kinematic model, singularities, velocity mapping, workspace, dexterity, statics, and kinetostatic performance. Furthermore, the virtual quadruped rover equipped with this innovative leg mechanism is built. Various basic and specific LTs of the rover are demonstrated by simulation, which indicates that the flexibility of the legs can help the rover achieve multitasking.

Keywords design synthesis      parallel mechanism      hybrid leg mechanism      screw theory      quadruped robot     
Corresponding Author(s): Sheng GUO   
Just Accepted Date: 09 October 2022   Issue Date: 05 June 2023
 Cite this article:   
Yifan WU,Sheng GUO,Luquan LI, et al. Design of a novel side-mounted leg mechanism with high flexibility for a multi-mission quadruped earth rover BJTUBOT[J]. Front. Mech. Eng., 2023, 18(2): 24.
 URL:  
https://academic.hep.com.cn/fme/EN/10.1007/s11465-022-0740-0
https://academic.hep.com.cn/fme/EN/Y2023/V18/I2/24
Fig.1  Concept of constructing a side-mounted novel leg mechanism for our earth rover. DOF: degree-of-freedom, MP: moving platform.
Fig.2  d-dimensional wrench system on the output link of the side-mounted leg mechanism.
Fig.3  Motion forms only use rotation degree of freedoms: (a) deployable function, (b) omnidirectional motion, (c) Ackerman steering, and (d) pivot steering.
Fig.4  Motion forms only use translation degree of freedoms: (a) active suspension function and (b) walking motion.
Fig.5  Special functions combine different motion forms: (a) adaptive walking, (b) crawling, and (c) jumping.
Fig.6  Wrench of the two feasible configurations of the side-mounted leg mechanism: (a) 5-DOF side-mounted parallel leg mechanism and (b) hybrid leg mechanism using a 4-DOF side-mounted parallel mechanism and a revolute steering joint. DOF: degree-of-freedom.
Fig.7  Some configurations of 3R2T 5-degree-of-freedom parallel mechanisms using a symmetrical structure with F-limbs: (a) 5-5R(R2R2R2R1R1) and (b) 5-3R2P(PPR2R1R1). P: prismatic joint, R: revolute joint, R1: type-1 revolute joint, R2: type-2 revolute joint.
Fig.8  Some configurations of 2R2T 4-degree-of-freedom parallel mechanisms using a symmetrical structure with F-limbs: (a) 4-5R(R2R2R2R1R1) and (b) 4-4R1P(PR2R2R1R1). P: prismatic joint, R: revolute joint, R1: type-1 revolute joint, R2: type-2 revolute joint.
Fig.9  Two examples of 3R2T 5-DOF asymmetrical parallel mechanisms using passive constraining limb: (a) 5-SPS&PPRU and (b) 5-UCU&RRRC. C: cylindrical joint, P: prismatic joint, R: revolute joint, S: spherical joint, U: universal joint.
Fig.10  Construction of the L1F1C-limb. L1F1C: passive constraining limb provides both a constraint force and a constraint couple. DOF: degree-of-freedom.
Joint type 4R feasible limbs 3R1P feasible limbs 2R2P feasible limbs
Only exists basic joints
Exists equivalent cylindrical pairs ?
Exists equivalent universal joints
Tab.1  Feasible L1F1C limbs for side-mounting
Fig.11  Two examples of 2R2T 4-degree-of-freedom asymmetrical parallel mechanisms using the L1F1C limb: (a) 3-UCU&PPU and (b) 3-SPS&RRRR. C: cylindrical joint, P: prismatic joint, R: revolute joint, S: spherical joint, U: universal joint.
Fig.12  Conceptual diagram of the side-mounted (3-UPRU&RRRR)&R hybrid leg mechanism. P: prismatic joint, P: prismatic joint with actuation, R: revolute joint, R: revolute joint with actuation, U: universal joint.
Fig.13  Schema diagram of the 3-UPRU&RRRR parallel mechanism (left) and the (3-UPRU&RRRR)&R hybrid leg mechanism (right). P: prismatic joint with actuation, R: revolute joint, R: revolute joint with actuation, U: universal joint.
Fig.14  Schematic diagram of the limbs in the 3-UPRU&RRRR parallel mechanism: (a) UPRU limb and (b) RRRR limb.
Fig.15  Singularity configurations of the side-mounted 3-UPRU&RRRR mechanism: (a) three UPRU limbs are parallel, (b) the axial vectors of all limbs intersect at one point, (c) the rank of the of all limbs’ axial vectors is less than four, (d) the 1st and 2nd joints of the RRRR limb are concentric, (e) OBD′ and DE′ are stretching collinear, and (f) OBD′ and DE′ are folding collinear.
Structural parameterValue/mm
?BOBAi?BOBA1=[175,0,170.5]T, ?BOBA2=[?175,0,170.5]T, ?BOBA3=[0,420,170.5]T
|?OBD|220
|?DE|225
|?EOP|582
?POPBi?POPB1=[?803,?80,21.5]T, ?POPB2=[803,?80,21.5]T, ?POPB3=[0,160,21.5]T
Tab.2  Important structural parameters of the 3-UPRU&RRRR mechanism
Fig.16  Velocity mapping analysis of the side-mounted 3-UPRU&RRRR mechanism: (a) initial configuration of the mechanism, (b) desired trajectory of the moving platform, (c) position and orientation curve of the moving platform, (d) velocity curve of the moving platform, (e) driver position curve, (f) driver actual speed curve, (g) driver calculated speed curve, and (h) error between the actual and calculated driver speed. qi (i = 1,2,…,6) are the six virtual drive joints considered when calculating the driving speed through the Jacobian matrix, in which q1 corresponds to l1, q2 to l2, q3 to l3, and q4 to θ, while q5 and q6 do not correspond to any drive joints in the mechanism, they are only for analysis.
Fig.17  Workspace of the side-mounted 3-UPRU&RRRR parallel mechanism: (a) α′ = 0, γ′ = 0 in spatial view, (b) α′ = 0, γ′ = 0 in plane, (c) α′ = ?10°, γ′ = 0 in plane, (d) α′ = 20°, γ′ = 0 in plane, (e) α′ = 0, γ′ = ?30° in plane, and (f) α′ = 0, γ′ = 30° in plane.
Fig.18  Workspace of the 3-UPRU&RRRR hybrid leg mechanism: (a) in spatial view, (b) in spatial view without limitations, (c) top view, (d) left view, and (e) front view.
Fig.19  Dexterity map of the 3-UPRU&RRRR mechanism in initial posture and ultimate posture: (a) α′ = ?10°, γ′ = 0°, (b) α′ = 0°, γ′ = 0°, (c) α′ = 20°, γ′ = 0°, (d) α′ = 0°, γ′ = ?30°, and (e) α′ = 0°, γ′ = 30°. LCI: local condition index.
Fig.20  Global conditioning index of the 3-UPRU&RRRR mechanism under different postures: (a) ηω, (b) ηv, and (c) boxplot of ηω and ηv.
Fig.21  Static simulation of the side-mounted leg under different common force conditions: (a) condition 1, (b) condition 2, (c) condition 3, and (d) condition 4.
Fig.22  Driving force and torque of actuators of the side-mounted leg in static simulation: (a) condition 1, (b) condition 2, (c) condition 3, and (d) condition 4.
Fig.23  Kinetostatic simulation for a composite translation of the leg: (a) timing diagram, (b) driving force and torque of actuator, and (c) position of actuator.
Fig.24  Kinetostatic simulation for posture adjustment of the leg: (a) timing diagram, (b) driving force and torque of actuator, and (c) position of actuator.
Fig.25  Model of the quadruped rover BJTUBOT using the novel side-mounted 3-UPRU&RRRR&R hybrid leg mechanism.
Fig.26  Different forms of motion of the side-mounted leg mechanism in the virtual model of BJTUBOT for simulation: (a) MF1, (b) MF2, (c) MF3, (d) MF4, and (e) MF5.
Fig.27  Omnidirectional locomotion of the rover: (a) t = 0 s, (b) t = 1 s, (c) t = 3 s, (d) t = 5 s, (e) t = 10 s, (f) t = 11 s, (g) t = 13 s, and (h) t = 14 s.
Fig.28  Ackerman steering locomotion of the rover: (a) t = 0 s, (b) t = 5 s, (c) t = 12 s, and (d) t = 22 s. CoM: center of mass.
Fig.29  Pivot steering locomotion of the rover: (a) t = 0 s, (b) t = 1 s, (c) t = 9 s, (d) t = 14 s, (e) t = 20s, (f) t = 25 s, (g) t = 26 s, and (h) t = 28 s.
Fig.30  Active suspension system function of the rover: (a) t = 0 s, (b) t = 4 s without suspension, (c) t = 8 s without suspension, (d) t = 11 s without suspension, (e) t = 4 s with suspension, (f) t = 8 s with suspension, and (g) t = 11 s with suspension. CoM: center of mass.
Fig.31  Basic walking locomotion of the rover: (a) t = 0 s, (b) t = 1 s, (c) t = 2 s, (d) t = 3 s, (e) t = 4 s, (f) t = 5 s, (g) t = 6 s, (h) t = 7 s, (i) t = 8 s, (j) t = 9 s, (k) t = 10 s, and (l) t = 11 s.
Fig.32  Crawling locomotion of the rover: (a) t = 0 s, (b) t = 4 s, (c) t = 7 s, and (d) t = 10 s. CoM: center of mass.
Fig.33  Jumping locomotion of the rover: (a) t = 0 s, (b) t = 1 s, (c) t = 2 s, (d) t = 4 s, (e) t = 8 s, (f) t = 10 s, (g) t = 12 s, and (h) t = 14 s. CoM: center of mass.
Abbreviations
CCylindrical joint
COMCenter of mass
DOFDegree-of-freedom
GCIGlobal conditioning index
L1F1CPassive constraining limb provides both a constraint force and a constraint couple
LCILocal condition index
LTLocomotion task
MFMotion form
PPrismatic joint
PPrismatic joint with actuation
RRevolute
RRevolute joint with actuation
R1Type-1 revolute joint
R2Type-2 revolute joint
SSpherical joint
TTranslation
UUniversal joint
Variables
aiVector ?OBAi
Baiai in the base coordinate
AFrobenius norm of matrix Am×n
biVector ?OPBi
Bbibi in the base coordinate
dDimension of the wrench system
dVector ?CD
d'Vector ?OBD
eVector ?DE
e'Vector ?OBE
fConstraint force
FA support force or static friction
F1Support force along the y-axis
F2, F3Static frictions along the x- and z-axis, respectively
F1(t), F2(t), F3(t)Time-varying functions of F1, F2, and F3, respectively
GGravity force
hHeight of the side-mounted base along the y-axis
JJacobian matrix of the 3-UPRU&RRRR parallel mechanism
Jc_RRRRConstraint Jacobian for the RRRR limbs
Jk_UPRUActuation Jacobian for the UPRU limbs
JvLinear velocity mapping part of J
JωAngular velocity mapping part of J
kVector ?OPK
Bkk in the base coordinate
Pkk in the moving platform coordinate
Wkk in the wheel coordinate
k(J)Condition number of the Jacobian matrix J
liLength of the vector ?AiBi
liVector ?AiBi
l˙iLinear velocity of the P joint
lmaxMaximum length of the P joint
lminMinimum length of the P joint
L˙Vector which contains all velocities of the P joints
mConstraint couple
MTorque caused by friction
M(t)Time-varying function of M
NSupport force
OBOriginal point of the base coordinate system
OPOriginal point of the moving platform coordinate system
OWOriginal point of the leg-end coordinate system
pVector ?OBOP
pWVector ?OBOW
BpWPosition vector of the leg-end in the base coordinate
q˙ijIntensity of the jth joint in the ith limb
Q˙Velocity vector of all joints
rLocation vector of the twist $
riLocation vector of the ith twist or screw $i
rdrLocation vector of the dth constraint screw S/dr
BRPRotation matrix from the moving platform frame to the base frame
BRWRotation matrix from the leg-end frame to the base frame
PRWRotation matrix from the leg-end frame to the moving platform frame
WRPInverse of PRW
sDirection vector of the twist $
siDirection vector of the ith twist or screw $i
sijDirection vector of S/ij
sdrDirection vector of the dth constraint screw S/dr
tTime
uliUnit vector of P joint
udUnit vector of the linkage CD
Buliuli in the base coordinate
BvVector v in the base frame
BvOPLinear velocity of moving platform
PvVector v in the moving platform frame
WvVector v in the leg-end frame
wWidth of the side-mounted base along the x-axis
wVector ?KOW
WSWorkspcae
xx-axis of the base coordinate system
x˙Velocity in the x direction
xPx-axis of the moving platform coordinate system
x(t)Position function on the x-axis
X˙Velocity of moving platform
yy-axis of the base coordinate system
y˙Velocity in the y direction
yPy-axis of the moving platform coordinate system
y(t)Position function on the y-axis
zz-axis of the base coordinate system
zPz-axis of the moving platform coordinate system
αAttitude angle about the x-axis
α˙Velocity of α
αRotation angle about the xP-axis
α(t)Orientation function about α'
βAttitude angle about the y-axis
β˙Velocity of β
γAttitude angle about the z-axis
γ˙Velocity of γ
γ'Rotation angle about the zP-axis
γ(t)Orientation function about γ'
ηiValue of GCI
ηv, ηωGCI of the linear and angular motions, respectively
θRotation angle of the R joint in the RRRR limb
θ˙Angular velocity of active R joint
θ˙inIntensity or angular velocity of the passive joints
φRotation angle of the steering R joint connected with the leg-end
BωAngular velocity of moving platform
δQ˙Driving velocity deviation
$A screw or a twist
$rA wrench system
$iith twist or screw
S/ijUnit screw of the jth joint in the ith limb
S/PInstantaneous twist of the moving platform
S/drdth constraint screw
S/irReciprocal screws for the ith UPRU limb
δS/PVelocity deviation of the moving platfrom
  
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