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Proceedings VCM 2012 24 a simple walking control method for biped robot

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Abstract: This paper proposes a simple walking control method for a 10 degree of freedom (DOF) biped robot with stable and humanlike walking using simple hardware configuration. The biped robot is modeled as a 3D inverted pendulum. From dynamic model of the 3D inverted pendulum and under the assumption that center of mass (COM) of the biped robot moves on a horizontal constraint plane, zero moment point (ZMP) equations of the biped robot depending on the coordinate of the center of the pelvis link obtained from the dynamic model of the biped robot are given based on the D’Alembert’s principle. A walking pattern is generated based on ZMP tracking control systems that are constructed to track the ZMP of the biped robot to zigzag ZMP reference trajectory decided by the footprint of the biped robot. An optimal tracking controller is designed to control the ZMP tracking control system. When the ZMP of the biped robot is controlled to track the x and y ZMP reference trajectories that always locates the ZMP of the biped robot inside stable region known as area of the footprint, a trajectory of the COM is generated as a stable walking pattern of the biped robot. Based on the stable walking pattern of the biped robot, a stable walking control method of the biped robot is proposed by using the inverse kinematics. From the trajectory of the COM of the biped robot and an arc referenceinput of the swinging leg, the inverse kinematics solved by the solid geometry method is used to compute the angles of each joint of the biped robot. These angles are used as references angles. Because the reference angles of the biped robot are computed from the stable walking pattern of the biped robot, the walking of the biped robot is stable if the angles of each joint of the biped robot are controlled to track those reference angles. The stable walking control method of the biped robot is implemented by simple hardware using PIC18F4431 and dsPIC30F6014. The simulation and experimental results show the effectiveness of this proposed control method Keywords: Optimal Tracking Controller; ZMP Tracking Control System; Biped Robot.

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A Simple Walking Control Method for Biped Robot

with Stable Gait

Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, *Tran Quang Thuan

Ho Chi Minh City University of Technology, Vietnam

* Posts and Telecommunications Institute of Technology branch Hochiminh city

e-Mail: phuongkorea2005@yahoo.com

Abstract:

This paper proposes a simple walking control method for a 10 degree of freedom (DOF) biped robot with stable and human-like walking using simple hardware configuration The biped robot is modeled as a 3D inverted pendulum From dynamic model of the 3D inverted pendulum and under the assumption that center of mass (COM) of the biped robot moves on a horizontal constraint plane, zero moment point (ZMP) equations of the biped robot depending on the coordinate of the center of the pelvis link obtained from the dynamic model

of the biped robot are given based on the D’Alembert’s principle A walking pattern is generated based on ZMP tracking control systems that are constructed to track the ZMP of the biped robot to zigzag ZMP reference trajectory decided by the footprint of the biped robot An optimal tracking controller is designed to control the ZMP tracking control system When the ZMP of the biped robot is controlled to track the x and y ZMP reference trajectories that always locates the ZMP of the biped robot inside stable region known as area

of the footprint, a trajectory of the COM is generated as a stable walking pattern of the biped robot Based on the stable walking pattern of the biped robot, a stable walking control method of the biped robot is proposed by using the inverse kinematics From the trajectory of the COM of the biped robot and an arc reference input of the swinging leg, the inverse kinematics solved by the solid geometry method is used to compute the angles of each joint of the biped robot These angles are used as references angles Because the reference angles of the biped robot are computed from the stable walking pattern of the biped robot, the walking of the biped robot is stable if the angles of each joint of the biped robot are controlled to track those reference angles The stable walking control method of the biped robot is implemented by simple hardware using PIC18F4431 and dsPIC30F6014 The simulation and experimental results show the effectiveness of this proposed control

method

Keywords: Optimal Tracking Controller; ZMP Tracking Control System; Biped Robot

1 Introduction

Research on humanoid robots and biped robots

locomotion is currently one of the most exciting

topics in the field of robotics and there exist many

ongoing projects Although some of those works

have already demonstrated very reliable dynamic

biped walking [11], it is still important to

understand the theoretical background of the biped

robot The biped robot performs its locomotion

relatively to the ground while it is keeping its

balance and not falling down Since there is no

base link fixed on the ground or the base, the gait

planning and control of the biped robot is very

important but difficult Up so far, numerous

approaches have been proposed The common

method of these numerous approaches is to restrict

zero moment point (ZMP) within a stable region to

protect the biped robot from falling down [2]

In the recent years, a great amount of scientific

and engineering research has been devoted to the

development of legged robots able to attain gait patterns more or less similar to human beings Towards this objective, many scientific papers have been published, focusing on different aspects

of the problem Sunil, Agrawal and Abbas [3] proposed motion control of a novel planar biped with nearly linear dynamics They introduced a biped robot that the model was nearly linear The motion control for trajectory following used nonlinear control method Park [4] proposed impedance control for biped robot locomotion so that both legs of the biped robot were controlled

by the impedance control, where the desired impedance at the hip and the swing foot was specified Huang and Yoshihiko [5] introduced sensory reflex control for humanoid walking so that the walking control consisted of a feedforward dynamic pattern and a feedback sensory reflex In these papers, the moving of the body of the robot was assumed to be only on the sagittal plane The

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biped robot was controlled based on the dynamic

model The ZMP of the biped robot was measured

by sensors so that the structure of the biped robot

was complex and the biped robot required a high

speed controller hardware system

This paper presents a stable walking control of a

biped robot by using the inverse kinematics with

simple hardware configuration based on the

walking pattern which is generated by ZMP

tracking control systems The robot’s body can

move on the sagittal and the lateral planes

Furthermore, the walking pattern is generated

based on the ZMP of the biped robot so that the

stability of the biped robot during walking or

running is guaranteed without the sensor system to

measure the ZMP of the biped robot In addition,

the simple inverse kinematics using the solid

geometry is used to obtain angles of each joints of

the biped robot based on the stable walking

pattern The biped robot is modeled as a 3D

inverted pendulum [1] The ZMP tracking control

system is constructed based on the ZMP equations

to generate a trajectory of COM A continuous

time optimal tracking controller is also designed to

control the ZMP tracking control system From the

trajectory of the COM, the inverse kinematics of

the biped robot is solved by the solid geometry

method to obtain angles of each joint of the biped

robot It is used to control walking of the biped

robot

2 Mathematic Model Of The Biped Robot

A new biped robot developed in this paper has 10

DOF as shown in Fig 1

Fig 1 Configuration of 10 DOF biped robot

The biped robot consists of five links that are one

torso, two links in each leg those are upper link

and lower link, and two feet The two legs of the

biped robot are connected with torso via two DOF

rotating joints which are called hip joints Hip

joints can rotate the legs in the angles  5 for right leg and  7 for left leg on sagittal plane, and in the angles  4 for right leg and  6 for left leg on in frontal plane The upper links are connected with lower links via one DOF rotating joints those are called knee joints which can rotate on sagittal plane The lower links of legs are connected with feet via two DOF of ankle joints The ankle joints can rotate the feet in angle 1 (for right leg) and 10

(for left leg) on the sigattal plane, and in angle  2

for left leg and  9 for right leg on the in frontal plane The rotating joints are considered to be friction-free and each one is driven by one DC motor

2.1 Kinematics model of biped robot

It is assumed that the soles of robot do not slip In the world coordinate system w which the origin is set on the ground, the coordinate of the center of the pelvis link and the ankle of swing leg can be expressed as follows:

3 1

2 1 1 b

c x l sin l sin

2 4

3

2 1 3 2 2 1 b c cos 2 l

sin cos

l sin l y y

(2)

2 1 3 2

2 1 1 b c

sin 2

l cos cos

l

cos cos l z z

(3)

In choosing Cartesian coordinate a which the origin is taken on the ankle, position of the center

of the pelvis link is expressed as follows:

3 1

2 1 1

ca l sin l sin

3

2 1 3 2 2 1 ca

cos 2 l

sin cos

l sin l y

(5)

3 2 1 3 2

2 1 1 ca

sin 2

l cos cos

l

cos cos l z

(6)

where, x ca , y ca , z ca are position of the center of the

pelvis link in a Similarly, position of the ankle joint of swing leg

is expressed in the coordinate system h which the origin is taken on the center of pelvis link as:

8 7

1 7 2

8 76

1 6 2 3

eh l sin l cos sin 2

l

8 76 1

7 6 2

eh l cos cos l cos cos

It is assumed that the center of mass of each link is concentrated on the tip of the link and the initial

z

x

y

Knee

a

b

3

8

1

5

10

6

7

Ankle

Pelvis Torso

z h x h

y h

z a

x a

y a

l2

l 1

0

B 2(x b ,y b ,z b )

K1

B2

B1

C

B

K

E

C(x c ,y c ,z c )

Foot

Hip

Trang 3

position is located at the origin of the w This

means that x b = 0 and y b = 0

The COM of the robot can be obtained as follows:

e 4 3 c 2 1 b

e e 4 4 3 3 c c 2 2 1

1

b

b

com

m m m m m m m

x m x m x m x m x m x

m

x

m

x

e 4 3 c 2 1 b

e e 4 4 3 3 c c 2 2 1

1

b

b

com

m m m m m m m

y m y m y m y m y m y

m

y

m

y

e 4 3 c 2 1 b

e e 4 4 3 3 c c 2 2 1

1

b

b

com

m m m m m m m

z m z m z m z m z m z

m

z

m

z

where (x b , y b , z b ) and (x e , y e , z e) are coordinates of

the ankle joints B2 and E, (x 1 , y 1 , z 1 ) and (x 4 , y 4 , z 4)

are coordinates of the knee joints B1 and K1, (x 2,

y 2 , z 2 ) and (x 3 , y 3 , z 3) are coordinate of the hip

joints B and K, (x c , y c , z c) is coordinate of the

center of pelvis link C, m b and m e are the mass of

ankle joints B2 and E, m 1 and m 4 are the mass of

knee joints B1 and K1, m 2 and m 3 are the mass of

hip joints B and K, and m c is the mass of the center

of pelvis link C

If the mass of links of legs is negligible compared

with mass of the trunk, Eqs (1)~(3) can be

rewritten as follows:

c

com x

c

c

It means that the COM is concentrated on the

center of the pelvis link

In this paper, Eqs (13)~(15) are used

2.2 Dynamic model of biped robot

When the biped robot is supported by one leg, the

dynamics of the robot can be approximated by a

simple 3D inverted pendulum whose leg is the foot

of biped robot and head is COM of biped robot as

shown in Fig 2

Fig 2 Three dimension inverted pendulum

The length of inverted pendulum r is able to be

expanded or contracted The position of the mass

point p = [x ca , y ca , z ca]T can be uniquely specified

by a set of state variable q = [ r ,  p , r]T as follows

[1]:

p rS p sin r

r r

rD sin

sin 1 r

[r ,  p , f]T is defined as actuator torques and force associated with the variables [r ,  p , r]T The Lagrangian of the 3D inverted pendulum is

ca 2

ca 2 ca 2

ca y z ) mgz x

( m 2

1

where m is the total mass of the biped robot, g is

the gravity acceleration

Based on the Largange’s equation, the dynamics

of 3D inverted pendulum can be obtained in the Cartesian coordinate as follows:

D D

S

rC D

S rC

mg f z y x

D S

S rC 0 rC

D S rC rC 0

r r

p r

ca ca ca

r p

p p p

r r r

Multiplying the first row of the Eq (20) by D/C r

yields

r ca r

C

D z

rS y rD

Substituting Eqs (16) and (17) into Eq (21), the

dynamics equation of inverted pendulum along y ca

axis can be obtained as

where

r C

D

  is the torque around x axis

Using similar procedure, the dynamics equation of

inverted pendulum along x ca axis can be derived from the second row of the Eq (20) as

z ca x ca x ca z cay mgx ca

p y C

D

The motions of the point mass of inverted pendulum are assumed to be constrained on the

plane whose normal vector is [k x , k y , -1]T and z intersection is z c The equation of the plane can be expressed as

c ca y ca x

ca k x k y z

where k x , k y , z c are constant

Second order derivative of Eq (31) are

ca y ca x

x a

 P  r

 r

 P

r

f P

f r

0

p

f

Trang 4

Substituting Eqs (24) and (25) into Eqs (22) and

(23), the equation of motion of 3D inverted

pendulum under constraint can be expressed as

c ca ca ca ca c

x ca

c

ca

mz

1 y

x y x z

k y

z

g

c ca ca ca ca c

y ca

c

ca

mz

1 y

x y x z

k

x

z

g

It is assumed that the biped robot walks on the flat

floor and horizontal plane In this case, k x and k y

are set to zero It means that the mass point of

inverted pendulum moves on a horizontal plane

with the height z ca = z c Eqs (26) and (27) can be

rewritten as

x c ca

c

ca

mz

1 y

z

g

y c ca

c

ca

mz

1 x

z

g

When inverted pendulum moves on the horizontal

plane, the dynamic equation along the x ca axis and

y ca axis are independent and linear differential

equations[1]

(x zmp , y zmp) is defined as location of ZMP on the

floor as shown in Fig 3

ZMP is such a point where the net support torque

from floor about x ca axis and y ca axis is zero From

pendulum under constraint can be expressed as

ca c

ca

g

z

x

ca c

ca

g

z

y

Fig 3 ZMP of inverted pendulum

Eq (30) shows that position of ZMP along x ca axis

is linear differential equation and it depends only

on the position of mass point along x ca axis

Similarly, position of ZMP along y ca axis do not

depend on x ca but only on y ca axis

3 WALKING PATTERN GENERATION

The objective of controlling the biped robot is to realize a stable walking or running The stable walking or running of the biped robot depends on

a walking pattern The walking pattern generation

is used to generate a trajectory for the COM of the biped robot For the stable walking or running of the biped robot, the walking pattern should satisfy the condition that the ZMP of the biped robot always exists inside the stable region Since position of the COM of the biped robot has the close relationship with the position of the ZMP as shown in Eqs (25)~(26), a trajectory of the COM can be obtained from the trajectory of the ZMP Based on a sequence of the desired footprint and the period time of each step of the biped robot, a reference trajectory of the ZMP can be specified Fig 3 illustrates the footprint and the zigzag reference trajectory of the ZMP to guarantee a stable gait

Left foot

Right foot

ZMP reference trajectory

y [m]

x [m]

0.1

0.1

-0.1

t 1

t 8

Fig 3 Footprint and reference trajectory of the

ZMP

The x and y ZMP trajectories versus times

corresponding to the zigzag reference trajectory of the ZMP in Fig 3 can be obtained as shown in Figs 4 and 5

0 10 20 30 40 50 60 70 80 -0.1

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7

Time (sec)

t 2

t 3

t 4

t 5

t 6

t 7

Fig 4 x ZMP reference trajectory versus time

Foo

0

z c

x a

z a Mass

point

x ca

x zmp

Foo

0

z c

y a

z a

Mass point

y ca y zmp

Trang 5

0 10 20 30 40 50 60 70 80

-0.1

-0.08

-0.06

-0.04

-0.02

0

0.02

0.04

0.06

0.08

0.1

Time (sec)

t 1

t 2 t 3 t 4 t 5 t 6 t 7

t 8

Fig 5 y ZMP reference trajectory versus time

3.1 Walking pattern generation based on

optimal tracking control of the ZMP

When the biped robot is modeled as the 3D

inverted pendulum which is moved on the

horizontal plane, the ZMP’s position of the biped

robot is expressed by linear independent equations

along x a and y a directions which are shown as Eqs

(30)~(31)

ca ca

dt

d

dt

d

defined as the time derivatives of the horizontal

acceleration along x a and y a directions of the

COM, uxand u y are introduced as inputs Eqs

(30)~(31) can be rewritten in strictly proper form

as follows:

 

 

 

, x x x g

z 0

1

x

, u 1 0 0 x x x 0 0

0

1 0

0

0 1

0

x

x

x

t ca ca

ca cd zmp

x

t ca ca ca

t

ca

ca

ca

x

x x

x C

B x

A

x

 

 







 

y y y g

z 0

1

y

, u 1 0 0

y y y

0 0

0

1 0

0

0 1

0

y

y

y

t ca ca

ca cd zmp

y

t ca ca ca

t

ca

ca

ca

y

y y

 

 

 

 





 



x C

B x

A

x

where x zmp is position of the ZMP along x a axis as output of the system (32), y zmp is position of the

ZMP along y a axis as output of the system (33),

ca

x and ycaare positions of the COM with respect

to x a and y a axes, andxca, xca, yca, yca are horizontal velocities and accelerations with respect

to xa and ya directions, respectively

The systems (32) and (33) can be generalized

as a linear time invariant system as follows:

Cx

B Ax x

y

u

(34)

where x   n1 is state vector of system, u c   is

input signal, y   is output, A   nn , B   n1 and C   1n

Instead of solving differential Eqs (30)~(31), the position of the COM can be obtained by constructing a controller to track the ZMP as the outputs of Eqs (32)~(33) When x zmp and y zmp are controlled to track the x and y ZMP reference

trajectories, the COM trajectories can be obtained from state variablesxcaandyca According to this pattern, the walking or running of the biped robot are stable

3.2 Continuous Time Controller Design for ZMP Tracking Control

The system (34) is assumed to be controllable and observable The objective designing this controller

is to stabilize the closed loop system and to track the output of the system to the reference input

An error signal between the reference input r(t)

and the output of the system is defined as follows:

e   (35) The objective of the control system is to regulate

the error signal e(t) equal to zero when time goes

to infinity

As shown in Figs 4 and 5, the x and y ZMP

reference trajectories include segments as a ramp function and segments as a step function and have singular points To control the output of the ZMP tracking control systems to track the ramp

segments of the x and y ZMP reference

trajectories, the designed controller should satisfy the internal model principle This means that the reference input should be assumed to be a ramp signal input However, when the outputs of the ZMP tracking control systems track the ZMP

(32)

(33)

Trang 6

reference trajectories, an overshoot occurs at

singular points of the ZMP reference input because

at these points the time derivative of the ZMP

reference input does not exist Moreover, the

singular points of the ZMP reference trajectories

are very important points The overshoot at these

points makes the ZMP of the biped robot to move

outside the stable region if the maximum value of

the overshoot is larger than the chosen value of

stability margin In this case, the biped robot

becomes unstable When the outputs of the ZMP

tracking control systems are controlled to track the

step reference inputs, the errors between the

outputs of the ZMP systems and the ramp

segments of the ZMP reference inputs are

constant Because the ramp segments of the ZMP

reference trajectories are segments that the biped

robot changes its ZMP in two leg supported phase,

the errors mean that the outputs of the ZMP

systems are delayed by time compared with the

ZMP reference trajectories However, the walking

pattern generation is generated in offline process

so that the errors at the ramp segments of the ZMP

reference trajectory are not important The

reference signal is assumed to be a step function in

this paper

The first order and second order derivatives of the

error signal are expressed as follows:

tr ty t  

From the time derivative of the first row of Eq

(34) and Eq (36) the augmented system is

obtained as follows:

w 0 e 0 e

dt

a a

X

B x C

0 A

x

(37)

where wu is defined as a new input signal

A scalar cost function of the quadratic form is

chosen as

0

2 c

ec n 1

1 n n n

Q

0

0 0

symmetric semi-positive definite matrix, R c  

and Q ec   are positive scalar

The control signal w that minimizes the cost

function (38) of the system (37) can be obtained as

e K u

w    KcXaK1cx c (39)

1c

 n+1n+1 is solution of the following Ricatti equation with symmetric positive definite matrix

0

a a c a c c T

a P P A P B B P Q

When the initial conditions are u c (0) = 0 and

x(0) = 0, Eq (39) yields

t

0

c e t dt K

t t

Block diagram of the closed loop optimal tracking control system is shown as follows:

Fig 6 Block diagram of the closed loop optimal

tracking control system

4 Walking Control

Based on the stable walking pattern generation discussed in previous section, a continuous time trajectory of the COM of the biped robot is generated by the ZMP tracking control system The continuous time trajectory of the COM of the

biped robot is sampled with sampling time T c and

is stored into micro-controller The ZMP reference trajectory of the ZMP system is chosen to satisfy the stable condition of the biped robot The control objective for the stable walking of the biped robot

is to track the center of the pelvis link to the COM trajectory The inverse kinematics of the biped robot is solved to obtain the angle of each joint of the biped robot The walking control of the biped robot is performed based on the solutions of the inverse kinematics which is solved by the solid

geometry method

Solving the inverse kinematics problems directly from kinematics models is complex An inverse kinematics based on the solid geometry method is presented in this section During the walking of the biped robot, the following assumptions are supposed

- Trunk of the biped robot is always kept on the sagittal plane:  2  4 and 9  6

- The feet of the biped robot are always parallel with floor:  3 1 5

- The walking of the biped robot is divided into 3 phase: Two legs supported, right leg supported and

Trang 7

left leg supported

- The origin of the 3D inverted pendulum is

located at the ankle of supported leg

4.2 Inverse kinematics of biped robot in one leg

supported

When the biped robot is supported by right leg,

left leg swings A coordinate system  a that takes

the origin at the ankle of supported leg is defined

Since the trunk of robot is always kept on the

sagittal plane, the pelvis link is always on the

horizontal plane as shown in Fig 7

The knee joint angle of the biped robot is gotten as

follows:

2 1

2 2 2 2 1 1 3

l l 2 k h l l cos

The ankle joint angle  2 k can be obtained from

Eq (43) The angle  1 k can be obtained from Eq

(44)

 

 

  





1

2 2 2 1 2 1 ca

1 1

1

l k h

l l k h cos k h

k x sin

DOB

k

where   r  k l y  k

4

l

k

2

3  

Fig 7 Inverted pendulum and supported leg

4.1 Inverse kinematics of swing leg

When the biped robot is supported by right leg,

left leg is swung as shown in Fig 8

Fig 8 Swing leg of biped robot

A coordinate system  hwith the origin that is taken at the middle of pelvis link is defined During the swing of this leg, the coordinate y of eh

the foot of swing leg is constant r ' k is defined

as the distance between foot and hip joint of swing

leg at k th sample time It is expressed in the coordinate system has follows

      z  k

2

l k y k x k '

2 3 eh 2

eh 2

where (x eh (k),y eh (k),z eh (k)) is coordinate of the

ankle of swing leg in the coordinateh at k th

sample time

The hip angle  6 k of the swing leg is obtained

based on the right triangle KEF as

  



k ' r 2 / l k y sin EKF

6

The minus sign in (46) means counterclockwise The hip angle  7 k is equal to the angle between

link l 2 and KG line It is can be expressed as

 

 

 

 

  





2

2 2 2 1 eh

1

1 7

l k ' r 2

l l k ' r cos k

' r k x sin

EKK GKE

k

(47)

Using the cosin’s law, the angle of knee of swing leg can be obtained as

          

2

2 2 2 1 1

8

l 2 k ' r l l cos E

KK

When robot is supported by two legs, the inverse kinematics is calculated by similar proceduce of one leg supported

5 Simulation And Experimental Results

The walking control method proposed in previous section is implemented in the CIMEC-1 biped robot developed for this paper as shown in Fig 9

l3/2 COM

r

 r

 P

x a

y a

z a

z c

 3

0

C

B

l1

l2

h 

D

 2

A

 1

B 1

F

E

G

H

x h

z h

C

l 1

l 2 r'

(x ca ,y ca ,z ca)

 7

l 3 /2

K 1

Trang 8

Fig 9 HUTECH-1 biped robot

A simple hardware configuration using three

PIC18F4431 and one dsPIC30F6014 for the

CIMEC-1 biped robot is shown in Fig 10

Master unit dsPIC 30F6014

Motor

Potentiomate

r

Potentiomate

r Potentiomate

r

r Potentiomate

r

r Potentiomate

r

r Potentiomate

r

r

Slave unit 1 PIC 18F4431

Slave unit 2 PIC 18F4431

Slave unit 3 PIC 18F4431

Hip joint

Ankle joint

Hip joint

Ankle joint

Knee joint

Knee joint

Fig 10 Hardware configuration of the

CIMEC-1 biped robot

dsPIC30F6014 is used as a master unit, and

PIC18F4431 is used as slave units The master unit

and the slave units communicate each other via

I2C communication The master unit is used to

solve the inverse kinematics problem based on the

trajectory of the center of the pelvis of the biped

robot and the trajectory of the ankle of the

swinging leg which are contained in its memory It

can also communicate personal computer via

RS-232 communication The angles at the k th sample

time obtained from the inverse kinematics are sent

to the slave units as reference signals

The block diagram of proposed controller for biped robot is shown in Fig 11

Fig 11 Block diagram of proposed controller

To demonstrate the walking performance of the biped robot based on the ZMP walking pattern generation combined with the inverse kinematics, the simulation results for walking on the flat floor

of the biped robot using Matlab are shown Fig

10 shows one step walking pattern of the biped robot on the flat floor

The period of step is 10 sec That is, changing time

of supported leg is 5 sec and moving time of swing leg is 5 sec The length of step is 20 cm During the moving of the biped robot, the height of the center of pelvis link is constant In the swing phase, the ZMP is located at the center of the supported foot When two legs of the biped robot are contacted to the ground, the ZMP moves from current supported leg to geometry center of the new supported foot The parameter values of the biped robot used in the simulation are given in Table 5.1

Table 5.1 Numerical values used in simulation

1

2

3

c

The footprint and ZMP desired trajectory are shown in Fig 13

Desired ZMP Trajectory

x ZMP Trajectory

y ZMP Trajectory

y ZMP servo system

x ZMP servo system x COM

y COM

Desired trajectory of swing leg

Biped robot

angle joints

 i

Inverse kinematics

of the biped robot

Swing phase Changing supported leg

Fig 12 One step walking pattern

ZMP servo system

Trang 9

ZMP desired trajectory Left foot

Right foot

Fig 13 Footprint and desired trajectory of ZMP

The simulation results are shown in Figs 14~20

Fig 14 presents x, y ZMP reference, output and

coordinate of COM with respect to time Figs

15~16 show control signals and tracking errors

Figs 17 ~19 show joints’ angle of one leg of the

robot, the joints’ angle of opposite side leg are

similar Fig 20 presents movement of the center of

pelvis link in the world coordinate system

-0.1

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

Time [sec]

ZMP reference input Position of COM ZMP output

a) x ZMP reference, output and COM

-0.1

-0.05

0

0.05

0.1

0.15

Time [sec]

ZMP reference input Position of COM ZMP output

a) y ZMP reference, output and COM

Fig 14 x, y ZMP reference, output and COM

0 10 20 30 40 50 60 70 80

-2

-1.5

-1

-0.5

0

0.5

1

1.5

2x 10

-4

Time (sec)

a) Control signal u of y ZMP

-5

-4

-3

-2

-1

0

1

2

3

4

-4

Time (sec)

b) Control signal u of x ZMP Fig 15 Control signal input

-2 0 2 4 6 8

-3

Time [sec]

a) x tracking error

-0.025 -0.02 -0.015 -0.01 -0.005 0 0.005 0.01 0.015 0.02 0.025

Time [sec]

b) y tracking error

Fig 16 Tracking error

10 15 20 25 30 35 40 45 50 55

Time (sec)

1

Experiment Result Simulation result

Fig 17 The ankle joint angle 1

-15 -10 -5 0 5 10 15 20

Time (sec)

2

Experiment result Simulation result

Fig 18 The ankle joint angle 2

40 45 50 55 60 65 70 75 80 85 90 95

Time (sec)

Experiment result Simulation result

Fig 19 The knee joint angle 3

Trang 10

-0.1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7

-0.1

-0.05

0

0.05

0.1

x (m)

Fig 20 Coordinate of center of pelvis link

5 Conclusion

In this paper, a 10 DOF biped robot is developed

The kinematic and dynamic models of the biped

robot are proposed An continuous time optimal

tracking controller is designed to generate the

trajectory of the COM for its stable walking The

walking control of the biped robot is performed

based on the solutions of the inverse kinematics

which is solved by the solid geometry method A

simple hardware configuration is constructed to

control the biped robot The simulation and

experimental results are shown to prove

effectiveness of the proposed controller

REFERENCES

[1] S Kajita, F Kanehiro, K Kaneko, K, Yokoi

and H Hirukawa, “The 3D Linear Inverted

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Tran Dinh Huy received the B.E and

engineering from HoChiMinh City University of Technology in 1995 and

1998, respectively He is currently a PhD student of Open University Malaysia His research interests include robotics and motion control

Nguyen Thanh Phuong received

the B.E., M.E degrees in electrical engineering from HoChiMinh City University of Technology, in 1998,

mechatronics in 2008 from Pukyong National University, Korea respectively He is currently a Lecturer in the Department of

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