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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.

Tuyển tập công trình Hội nghị Cơ điện tử toàn quốc lần thứ 6 169 Mã bài: 39 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 170 Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, Tran Quang Thuan VCM2012 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:   13211bc sinlsinlxx   (1)     42 3 213221bc cos 2 l sincoslsinlyy     (2)     42 3 2132 211bc sin 2 l coscosl coscoslzz     (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:   13211ca sinlsinlx   (4)     42 3 213221ca cos 2 l sincoslsinly     (5)     42 3 2132 211ca sin 2 l coscosl coscoslz     (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:   78172eh sinlsinlx   (7)   678162 3 eh sincoslsinl 2 l y   (8)   6781762eh coscoslcoscoslz   (9) 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  2  5  4  10  9  6  7  A nkle Pelvis Torso z h x h y h z a x a y a l 2 l 1 0 B 2 (x b ,y b ,z b ) K 1 B 2 B 1 C B K E C(x c ,y c ,z c ) Foot Hip Tuyển tập công trình Hội nghị Cơ điện tử toàn quốc lần thứ 6 171 Mã bài: 39 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: e43c21b ee4433cc2211bb com mmmmmmm xmxmxmxmxmxmxm x    (10) e43c21b ee4433cc2211bb com mmmmmmm ymymymymymymym y    (11) e43c21b ee4433cc2211bb com mmmmmmm zmzmzmzmzmzmzm z    (12) where (x b , y b , z b ) and (x e , y e , z e ) are coordinates of the ankle joints B 2 and E, (x 1 , y 1 , z 1 ) and (x 4 , y 4 , z 4 ) are coordinates of the knee joints B 1 and K 1 , (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 B 2 and E, m 1 and m 4 are the mass of knee joints B 1 and K 1 , 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: ccom xx  (13) ccom yy  (14) ccom zz  (15) 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 sinrx ca   (16) rrca rSsinry   (17) rDsinsin1rz p 2 r 2 ca   (18) [  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 mgz)zyx(m 2 1 L    (19) 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 SrC D SrC mg fz y x DSS D SrC 0rC D SrC rC0 m pp rr p r ca ca ca rp pp p rr r      (20) Multiplying the first row of the Eq. (20) by D/C r yields   rr r carca mgrS C D zrSyrDm     (21) Substituting Eqs. (16) and (17) into Eq. (21), the dynamics equation of inverted pendulum along y ca axis can be obtained as   caxcacacaca mgyzyyzm       (22) where r C D x   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   caycacacaca mgxzxxzm       (23) where p p y C D   is the torque around y axis. 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 ccaycaxca zykxkz  (24) where k x , k y , z c are constant. Second order derivative of Eq. (31) are caycaxca ykxkz         (25) x a y a z a  P  r  r  P r f P f r 0 p f 172 Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, Tran Quang Thuan VCM2012 Substituting Eqs. (24) and (25) into Eqs. (22) and (23), the equation of motion of 3D inverted pendulum under constraint can be expressed as   x c cacacaca c x ca c ca mz 1 yxyx z k y z g y    (26)   y c cacacaca c y ca c ca mz 1 yxyx z k x z g x    (27) 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    (28) y c ca c ca mz 1 x z g x    (29) 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 D’Alembert’s principle, ZMP of inverted pendulum under constraint can be expressed as ca c cazmp x g z xx   (30) ca c cazmp y g z yy   (31) 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 0.2 0.3 0.4 0.5 0.6 0.1 -0.1 t 1 t 2 t 3 t 4 t 5 t 6 t 7 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) x zmp reference t 2 t 3 t 4 t 5 t 6 t 7 x ZMP reference input [m] Fig. 4. x ZMP reference trajectory versus time. Foo 0 z c x a z a Mass point x c a x zmp Foo 0 z c y a z a Mass point y c a y zmp Tuyển tập công trình Hội nghị Cơ điện tử toàn quốc lần thứ 6 173 Mã bài: 39 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) y zmp reference t 1 t 2 t 3 t 4 t 5 t 6 t 7 t 8 y ZMP reference input [m] 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). cacax xx dt d u   and cacay yy dt d u   are defined as the time derivatives of the horizontal acceleration along x a and y a directions of the COM, x u and y u are introduced as inputs. Eqs. (30)~(31) can be rewritten in strictly proper form as follows:           , x x x g z 01x ,u 1 0 0 x x x 000 100 010 x x x t ca ca ca cd zmp x t ca ca ca t ca ca ca x xx x C Bx A x                                                                               . y y y g z 01y ,u 1 0 0 y y y 000 100 010 y y y t ca ca ca cd zmp y t ca ca ca t ca ca ca y yy               x C B xAx                                                            where zmp x is position of the ZMP along x a axis as output of the system (32), zmp y is position of the ZMP along y a axis as output of the system (33), ca x and ca y are positions of the COM with respect to x a and y a axes, and ca x  , ca x   , ca y  , ca y   are horizontal velocities and accelerations with respect to a x and a y 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 zmp x and zmp y are controlled to track the x and y ZMP reference trajectories, the COM trajectories can be obtained from state variables ca x and ca y . 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:       tytrte  (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) 174 Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, Tran Quang Thuan VCM2012 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:       xC      tytrte (36) From the time derivative of the first row of Eq. (34) and Eq. (36) the augmented system is obtained as follows:   w 0e0edt d 1n aa a BX X Bx C 0Ax                                 (37) where uw   is defined as a new input signal. A scalar cost function of the quadratic form is chosen as      0 2 cc dtwRJ ac T a XQX (38) where     1n1n ecn1 1nnn Q            0 00 Q c is 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 eKuw c2  xKXK 1cac   (39) where   c T 1cc PBKK 1 cc2 RK   and P c   n+1n+1 is solution of the following Ricatti equation with symmetric positive definite matrix. 0R 1 c   cc T aacacc T a QPBBPAPPA (40) When the initial conditions are u c (0) = 0 and x(0) = 0, Eq. (39) yields         t 0 c2 dtteKttu xK 1c (41) 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: 42   and 69   . - The feet of the biped robot are always parallel with floor: 513      . - The walking of the biped robot is divided into 3 phase: Two legs supported, right leg supported and Tuyển tập công trình Hội nghị Cơ điện tử toàn quốc lần thứ 6 175 Mã bài: 39 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:                21 22 2 2 1 1 3 ll2 khll cosk  (42) The ankle joint angle   k 2  can be obtained from Eq. (43). The angle   k 1  can be obtained from Eq. (44).           kh/2/lkysinAOBk 3ca 1 2    (43)                               1 2 2 2 1 2 1ca1 11 lkh2 llkh cos kh kx sinDOBk  (44) where       kylkr 4 l kh ca3 2 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 h  with the origin that is taken at the middle of pelvis link is defined. During the swing of this leg, the coordinate eh y of the foot of swing leg is constant.   k'r 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 h  as follows.         kz 2 l kykxk'r 2 eh 2 3 eh 2 eh 2         (45) where (x eh (k),y eh (k),z eh (k)) is coordinate of the ankle of swing leg in the coordinate h  at k th sample time. The hip angle   k 6  of the swing leg is obtained based on the right triangle KEF as                  k'r 2/lky sinEKFk 3eh 1 6  (46) The minus sign in (46) means counterclockwise. The hip angle   k 7  is equal to the angle between link l 2 and KG line. It is can be expressed as                                2 2 1 2 2 2 1 eh 1 17 lk'r2 llk'r cos k'r kx sin EKKGKEk  (47) Using the cosin’s law, the angle of knee of swing leg can be obtained as                21 22 2 2 1 1 18 ll2 k'rll cosEKKk  . (48) 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. l 3 /2 COM r  r  P x a y a z a z c  3 0 C B l 1 l 2 h  D  2 A  1 B 1 F E G H K y h x h z h C l 1 l 2 r' ( x ca , y ca , z ca )  6  8  7 l 3 /2 K 1 176 Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, Tran Quang Thuan VCM2012 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 I2C communication Motor Motor Motor Potentiomate r Potentiomate r Potentiomate r Motor Motor Potentiomate r Potentiomate r Motor Motor Potentiomate r Potentiomate r Motor Motor Potentiomate r Potentiomate r Motor Potentiomate r Slave unit 1 PIC 18 F4 431 Slave unit 2 PIC 18 F4 431 Slave unit 3 PIC 18 F4 431 Hip joint Ankle joint Hip joint Ankle joint Hip joint Ankle joint Knee joint Hip joint Ankle joint Knee joint Servo controller of right knee joint  3 Servo controller of right hip joint  5 Servo controller of right ankle joint  1 Servo controller of right hip joint  4 Servo controller of left hip joint  6 Servo controller of right ankle joint  2 Servo controller of left ankle joint  9 Servo controller of left hip joint  7 Servo controller of left ankle joint  10 Servo controller of left knee joint  8 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 Parameters Values Units 1 l 0.28 [m] 2 l 0.28 [m] 3 l 0.2 [m] a 0.18 [m] b 0.24 [m] c z 0.5 [m] 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 Tuyển tập công trình Hội nghị Cơ điện tử toàn quốc lần thứ 6 177 Mã bài: 39 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 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 ZMP reference input,ZMP output, Position of COM [m] Time [sec] ZMP reference input Position of COM ZMP output a) x ZMP reference, output and COM 0 10 20 30 40 50 60 70 80 -0.1 -0.05 0 0.05 0.1 0.15 ZMP reference input,ZMP output, Position of COM [m] 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 2 x 10 -4 Time (sec) Control signal u a) Control signal u of y ZMP 0 10 20 30 40 50 60 70 80 -5 -4 -3 -2 -1 0 1 2 3 4 5 x 10 -4 Time (sec) Control signal ux b) Control signal u of x ZMP Fig. 15 Control signal input. 0 10 20 30 40 50 60 70 80 -2 0 2 4 6 8 10 x 10 -3 Tracking error [m] Time [sec] a) x tracking error. 0 20 40 60 80 -0.025 -0.02 -0.015 -0.01 -0.005 0 0.005 0.01 0.015 0.02 0.025 Tracking error [m] Time [sec] b) y tracking error. Fig. 16 Tracking error. 0 10 20 30 40 50 60 70 80 10 15 20 25 30 35 40 45 50 55 Time (sec) Ankle joint angle  1 (deg) Experiment Result Simulation result Fig. 17 The ankle joint angle 1  . 0 10 20 30 40 50 60 70 80 -15 -10 -5 0 5 10 15 20 Time (sec) Ankle joint angle  2 (deg) Experiment result Simulation result Fig. 18 The ankle joint angle 2  . 0 10 20 30 40 50 60 70 80 40 45 50 55 60 65 70 75 80 85 90 95 Time (sec) Knee joint angle  3 (deg) Experiment result Simulation result Fig. 19 The knee joint angle 3  . [m] [m] [m] [m] 178 Tran Dinh Huy, Nguyen Thanh Phuong, Ho Dac Loc, Tran Quang Thuan VCM2012 -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) y (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 Pendulum Mode: A simple modeling for a biped walking pattern generation”, Proc. of IEEE/RSJ International conference on Intelligent Robots and Systems, pp. 239~246, 2001. [2] C. Zhu and A. Kawamara, “Walking Principle Analysis for Biped Robot with ZMP Concept, Friction Constraint, and Inverted Pendulum Model”, Proc. of IEEE/RSJ International conference on Intelligent Robots and Systems, pp. 364~369, 2003. [3] S. K. Agrawal, and A. Fattah, “Motion Control of a Novel Planar Biped with Nearly Linear Dynamics”, IEEE/ASME Transaction on Mechatronics, Vol. 11, No. 2, pp. 162~168, 2006. [4] J. H. Part, “Impedance Control for Biped Robot Locomotion”, IEEE Transaction on Robotics and Automation, Vol. 17, No. 3, pp. 870~882, 2001. [5] Q. Huang and Y. Nakamura, “Sensor Reflex Control for Humanoid Walking”, IEEE Transaction on Robotics, Vol. 21, No. 5, pp. 977~984, 2005. [6] B. C. Kou, “Digital Control Systems”, International Edition, 1992. [7] D. Li, D. Zhou, Z. Hu, and H. Hu, “Optimal Priview Control Applied to Terrain Following Flight”, Proc. of IEEE Conference on Decision and Control, pp. 211~216, 2001. [8] D. Plestan, J. W. Grizzle, E. R. Westervelt and G. Abba, “Stable Walking of A 7-DOF Biped Robot”, IEEE Transaction on Robotics and Automation, Vol. 19, No. 4, pp. 653-668, 2003. [9] F. L. Lewis, C. T. Abdallah and D.M. Dawson, “Control of Robot Manipulator”, Prentice Hall International Edition, 1993. [10] G. F. Franklin, J. D. Powell and A. E. Naeini, “Feedback Control of Dynamic System”, Prentice Hall Upper Saddle River, New Jersey 07458. [11] G. A. Bekey, “Autonomous Robots From Biological Inspiration to Implementation and Control”, The MIT Press 2005. [12] H. K. Lum, M. Zribi and Y. C. Soh, “Planning and Control of a Biped Robot”, International Journal of Engineering Science ELSEVIER, Vol. 37, pp. 1319~1349, 1999. [13] H. Hirukawa, S. Kajita, F. Kanehiro, K. Kaneko and T. Isozumi, “The Human-size Humanoid Robot That Can Walk, Lie Down and Get Up”, International Journal of Robotics Research Vol. 24, No. 9, pp. 755~769, 2005. [14] K. Mitobe, G. Capi and Y. Nasu, “A New Control Method for Walking Robots Based on Angular Momentum”, Journal of Mechatronics ELSEVIER, Vol. 14, pp. 164~165, 2004. [15] K. Harada, S. Kajita, K. Kaneko and H. Hirukawa, “Walking Motion for Pushing Manipulation by a Humanoid Robot”, Journal of the Robotics Society of Japan, Vol. 22, No. 3, pp. 392–399, 2004. Tran Dinh Huy received the B.E. and M.E. degrees in mechanical 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, 2003, and PhD degree in mechatronics in 2008 from Pukyong National University, Korea respectively. He is currently a Lecturer in the Department of [...]... Mechanical – Electrical - Electronic,HUTECH university His research interests include robotics, renewable energy and motion control Ho Dac Loc received the B.E., PhD and Dr.Sc degrees in electrical engineering from Russia, in 1991, 1994 and 2002, respectively He is currently a rector of HUTECH university His research interests include robotics and industrial automatic control 179 Tran Quang Thuan received... B.E and M.E degrees in electrical electronic engineering from HoChiMinh City University of Technology in 1998 and 2006, respectively He is currently a Lecturer, of Faculty of Electronics Engineering, Posts and Telecommunications Institute of Technology branch Hochiminh city and a PhD student of Vietnam Research Institute of Electronics, Informetics and Automation His research interests include robotics... Telecommunications Institute of Technology branch Hochiminh city and a PhD student of Vietnam Research Institute of Electronics, Informetics and Automation His research interests include robotics and motion control Mã bài: 39 . 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. 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. 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

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