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Commit bd2811f7 authored by Andrea Del Prete's avatar Andrea Del Prete
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Add example of Romeo walking

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exercizes/ex_4_conf.py 0 → 100644
View file @ bd2811f7
# -*- coding: utf-8 -*-
"""
Created on Thu Apr 18 09:47:07 2019
@author: student
"""
import numpy as np
import os
np.set_printoptions(precision=3, linewidth=200, suppress=True)
LINE_WIDTH = 60
# cost weights in the objective function:
# ---------------------------------------
alpha = 10**(2) # CoP error squared cost weight
beta = 0 # CoM position error squared cost weight
gamma = 10**(-1) # CoM velocity error squared cost weight
h = 0.58 # fixed CoM height (assuming walking on a flat terrain)
g = 9.81 # norm of the gravity vector
foot_step_0 = np.array([0.0, -0.096]) # initial foot step position in x-y
dt_mpc = 0.1 # sampling time interval
T_step = 1.2 # time needed for every step
step_length = 0.001 # fixed step length in the xz-plane
nb_steps = 4 # number of desired walking steps
#N_SIMULATION = 2000 # number of time steps simulated
dt = 0.002 # controller time step
DATA_FILE = 'romeo_walking_traj.npz'
lxp = 0.10 # foot length in positive x direction
lxn = 0.05 # foot length in negative x direction
lyp = 0.05 # foot length in positive y direction
lyn = 0.05 # foot length in negative y direction
lz = 0.0 # foot sole height with respect to ankle joint
mu = 0.3 # friction coefficient
fMin = 5.0 # minimum normal force
fMax = 1000.0 # maximum normal force
rf_frame_name = "RAnkleRoll" # right foot frame name
lf_frame_name = "LAnkleRoll" # left foot frame name
contactNormal = np.matrix([0., 0., 1.]).T # direction of the normal to the contact surface
w_com = 1.0 # weight of center of mass task
w_foot = 1e-1 # weight of the foot motion task
w_posture = 1e-4 # weight of joint posture task
w_forceRef = 1e-5 # weight of force regularization task
kp_contact = 10.0 # proportional gain of contact constraint
kp_foot = 10.0 # proportional gain of contact constraint
kp_com = 10.0 # proportional gain of center of mass task
kp_posture = 1.0 # proportional gain of joint posture task
PRINT_N = 500 # print every PRINT_N time steps
DISPLAY_N = 20 # update robot configuration in viwewer every DISPLAY_N time steps
CAMERA_TRANSFORM = [4.0, -0.2, 0.4, 0.5243823528289795, 0.518651008605957, 0.4620114266872406, 0.4925136864185333]
SPHERE_RADIUS = 0.03
REF_SPHERE_RADIUS = 0.03
COM_SPHERE_COLOR = (1, 0.5, 0, 0.5)
COM_REF_SPHERE_COLOR = (1, 0, 0, 0.5)
RF_SPHERE_COLOR = (0, 1, 0, 0.5)
RF_REF_SPHERE_COLOR = (0, 1, 0.5, 0.5)
LF_SPHERE_COLOR = (0, 0, 1, 0.5)
LF_REF_SPHERE_COLOR = (0.5, 0, 1, 0.5)
filename = str(os.path.dirname(os.path.abspath(__file__)))
path = filename + '/../models/romeo'
urdf = path + '/urdf/romeo.urdf'
srdf = path + '/srdf/romeo_collision.srdf'
\ No newline at end of file
exercizes/ex_4_plan_LIPM_romeo.py 0 → 100644
View file @ bd2811f7
# LMPC_walking is a python software implementation of some of the linear MPC
# algorithms based presented in:
# https://groups.csail.mit.edu/robotics-center/public_papers/Wieber15.pdf
# Copyright (C) 2019 @ahmad gazar
# LMPC_walking is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
# LMPC_walking is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
# You should have received a copy of the GNU General Public License
# along with this program. If not, see <https://www.gnu.org/licenses/>.
# headers:
# -------
import numpy as np
from quadprog import solve_qp
import LMPC_walking.second_order.reference_trajectories as reference_trajectories
import LMPC_walking.second_order.motion_model as motion_model
import LMPC_walking.second_order.cost_function as cost_function
import LMPC_walking.second_order.constraints as constraints
import LMPC_walking.second_order.plot_utils as plot_utils
from LMPC_walking.second_order.motion_model import discrete_LIP_dynamics
import matplotlib.pyplot as plt
import ex_4_conf as conf
# Inverted pendulum parameters:
# ----------------------------
foot_length = conf.lxn + conf.lxp # foot size in the x-direction
foot_width = conf.lyn + conf.lyp # foot size in the y-direciton
nb_steps_per_T = int(round(conf.T_step/conf.dt_mpc))
# walking parameters:
# ------------------
N = conf.nb_steps * nb_steps_per_T # number of desired walking intervals
# CoM initial state: [x_0, xdot_0].T
# [y_0, ydot_0].T
# ----------------------------------
x_0 = np.array([conf.foot_step_0[0], 0.0])
y_0 = np.array([conf.foot_step_0[1], 0.0])
step_width = 2*np.absolute(y_0[0])
# compute CoP reference trajectory:
# --------------------------------
desiredFoot_steps = reference_trajectories.manual_foot_placement(conf.foot_step_0,
conf.step_length, conf.nb_steps)
desiredFoot_steps[1:,0] -= conf.step_length
desired_Z_ref = reference_trajectories.create_CoP_trajectory(conf.nb_steps,
desiredFoot_steps, N, nb_steps_per_T)
# used in case you want to have terminal constraints
# -------------------------------------------------
x_terminal = np.array([desired_Z_ref[N-1, 0], 0.0]) # CoM terminal constraint in x : [x, xdot].T
y_terminal = np.array([desired_Z_ref[N-1, 1], 0.0]) # CoM terminal constraint in y : [y, ydot].T
nb_terminal_constraints = 4
terminal_index = N-1
# construct your preview system: 'Go pokemon !'
# --------------------------------------------
[P_ps, P_vs, P_pu, P_vu] = motion_model.compute_recursive_matrices(conf.dt_mpc, conf.g,
conf.h, N)
[Q, p_k] = cost_function.compute_objective_terms(conf.alpha, conf.beta, conf.gamma,
conf.T_step, nb_steps_per_T, N, conf.step_length, step_width,
P_ps, P_pu, P_vs, P_vu, x_0, y_0, desired_Z_ref)
[A_zmp, b_zmp] = constraints.add_ZMP_constraints(N, foot_length, foot_width,
desired_Z_ref, x_0, y_0)
# used in case you want to add both terminal add_ZMP_constraints
# --------------------------------------------------------------
[A_terminal, b_terminal] = constraints.add_terminal_constraints(N,
terminal_index, x_0, y_0, x_terminal,
y_terminal, P_ps, P_vs, P_pu, P_vu)
A = np.concatenate((A_terminal, A_zmp), axis = 0)
b = np.concatenate((b_terminal, b_zmp), axis = 0)
# call quadprog solver:
# --------------------
U = solve_qp(Q, -p_k, A.T, b, nb_terminal_constraints)[0] # uncomment to solve with 4 equality terminal constraints
#U = solve_qp(Q, -p_k, A_zmp.T, b_zmp)[0] # solve only with only CoP inequality constraints
Z_x_total = U[0:N]
Z_y_total = U[N:2*N]
# Trajectory optimization: (based on the initial state x_hat_0, y_hat_0)
# -------------------------------------------------------------------------
[X_total, Y_total] = motion_model.compute_recursive_dynamics(P_ps, P_vs, P_pu,
P_vu, N, x_0,
y_0, U)
X_total = np.vstack((x_0, X_total))
Y_total = np.vstack((y_0, Y_total))
# ------------------------------------------------------------------------------
# visualize your open-loop trajectory:
# ------------------------------------------------------------------------------
time = np.arange(0, round(N*conf.dt_mpc, 2), conf.dt_mpc)
min_admissible_CoP = desired_Z_ref - np.tile([foot_length/2, foot_width/2],
(N,1))
max_admissible_cop = desired_Z_ref + np.tile([foot_length/2, foot_width/2],
(N,1))
# time vs CoP and CoM in x: 'A.K.A run rabbit run !'
# -------------------------------------------------
#plot_utils.plot_x(time, N, min_admissible_CoP,
# max_admissible_cop, Z_x_total, X_total, desired_Z_ref)
#
## time VS CoP and CoM in y: 'A.K.A what goes up must go down'
## ----------------------------------------------------------
#plot_utils.plot_y(time, N, min_admissible_CoP,
# max_admissible_cop, Z_y_total, Y_total, desired_Z_ref)
#
## plot CoP, CoM in x Vs Cop, CoM in y:
## -----------------------------------
#plot_utils.plot_xy(time, N, foot_length, foot_width,
# desired_Z_ref, Z_x_total, Z_y_total, X_total, Y_total)
dt_ctrl = conf.dt
N_ctrl = int((N*conf.dt_mpc)/dt_ctrl)
(A,B) = discrete_LIP_dynamics(dt_ctrl, conf.g, conf.h)
com = np.empty((3,N_ctrl+1))*np.nan
dcom = np.zeros((3,N_ctrl+1))
ddcom = np.zeros((3,N_ctrl+1))
cop = np.empty((2,N_ctrl+1))*np.nan
#foot_steps = np.empty((2,N_ctrl+1))*np.nan
contact_phase = (N_ctrl+1)*['right']
com[2,:] = conf.h
N_inner = int(N_ctrl/N)
for i in range(N):
com[0,i*N_inner] = X_total[i,0]
com[1,i*N_inner] = Y_total[i,0]
dcom[0,i*N_inner] = X_total[i,1]
dcom[1,i*N_inner] = Y_total[i,1]
if(i>0):
if np.linalg.norm(desired_Z_ref[i,:] - desired_Z_ref[i-1,:]) < 1e-10:
contact_phase[i*N_inner] = contact_phase[i*N_inner-1]
else:
if contact_phase[(i-1)*N_inner]=='right':
contact_phase[i*N_inner] = 'left'
elif contact_phase[(i-1)*N_inner]=='left':
contact_phase[i*N_inner] = 'right'
for j in range(N_inner):
ii = i*N_inner + j
(A,B) = discrete_LIP_dynamics((j+1)*dt_ctrl, conf.g, conf.h)
# foot_steps[:,ii] = desired_Z_ref[i,:].T
cop[0,ii] = Z_x_total[i]
cop[1,ii] = Z_y_total[i]
x_next = A.dot(X_total[i,:]) + B.dot(cop[0,ii])
y_next = A.dot(Y_total[i,:]) + B.dot(cop[1,ii])
com[0,ii+1] = x_next[0]
com[1,ii+1] = y_next[0]
dcom[0,ii+1] = x_next[1]
dcom[1,ii+1] = y_next[1]
ddcom[:2,ii] = conf.g/conf.h * (com[:2,ii] - cop[:,ii])
if(j>0): contact_phase[ii] = contact_phase[ii-1]
# Generate foot trajectories using polynomials with following constraints:
# x(0)=x0, x(T)=x1, dx(0)=dx(T)=0
# x(t) = a + b t + c t^2 + d t^3
# x(0) = a = x0
# dx(0) = b = 0
# dx(T) = 2 c T + 3 d T^2 = 0 => c = -3 d T^2 / (2 T) = -(3/2) d T
# x(T) = x0 + c T^2 + d T^3 = x1
# x0 -(3/2) d T^3 + d T^3 = x1
# -0.5 d T^3 = x1 - x0
# d = 2 (x0-x1) / T^3
# c = -(3/2) T 2 (x0-x1) / (T^3) = 3 (x1-x0) / T^2
def compute_polynomial_traj(x0, x1, T, dt):
a = x0
b = np.zeros_like(x0)
c = 3*(x1-x0) / (T**2)
d = 2*(x0-x1) / (T**3)
N = int(T/dt)
n = x0.shape[0]
x = np.zeros((n,N))
dx = np.zeros((n,N))
ddx = np.zeros((n,N))
for i in range(N):
t = i*dt
x[:,i] = a + b*t + c*t**2 + d*t**3
dx[:,i] = b + 2*c*t + 3*d*t**2
ddx[:,i] = 2*c + 6*d*t
return x, dx, ddx
foot_steps = desiredFoot_steps[::2,:]
#x = np.zeros((3,N_ctrl+1))
#dx = np.zeros((3,N_ctrl+1))
#ddx = np.zeros((3,N_ctrl+1))
#N_step = int(step_time/dt_ctrl)
#for s in range(foot_steps.shape[0]):
# x[0, s*2*N_step :s*2*N_step+N_step] = foot_steps[s,0]
# x[1, s*2*N_step :s*2*N_step+N_step] = foot_steps[s,1]
# x[:2, s*2*N_step+N_step:(s+1)*2*N_step] = compute_polynomial_traj(foot_steps[s,:], foot_steps[s+1,:],
# step_time, dt)
#np.savez('3_step_walking_traj', x=X_total, y=Y_total, z=desired_Z_ref)
np.savez(conf.DATA_FILE, com=com, dcom=dcom, ddcom=ddcom,
contact_phase=contact_phase, foot_steps=foot_steps)
time_ctrl = np.arange(0, round(N_ctrl*dt_ctrl, 2), dt_ctrl)
for i in range(2):
plt.figure()
plt.plot(time_ctrl, cop[i,:-1], label='CoP')
# plt.plot(time_ctrl, foot_steps[i,:-1], label='Foot step')
plt.plot(time_ctrl, com[i,:-1], 'g', label='CoM')
if i==0: plt.plot(time, X_total[:-1,0], ':', label='CoM TO')
else: plt.plot(time, Y_total[:-1,0], ':', label='CoM TO')
plt.legend()
for i in range(2):
plt.figure()
plt.plot(time_ctrl, dcom[i,:-1], label='CoM vel')
vel_fd = (com[i,1:] - com[i,:-1]) / dt_ctrl
plt.plot(time_ctrl, vel_fd, ':', label='CoM vel fin-diff')
plt.legend()
for i in range(2):
plt.figure()
plt.plot(time_ctrl, ddcom[i,:-1], label='CoM acc')
acc_fd = (dcom[i,1:] - dcom[i,:-1]) / dt_ctrl
plt.plot(time_ctrl, acc_fd, ':', label='CoM acc fin-diff')
plt.legend()
#plot_utils.plot_xy(time_ctrl, N_ctrl, foot_length, foot_width,
# foot_steps.T, cop[0,:], cop[1,:],
# com[0,:].reshape((N_ctrl+1,1)),
# com[1,:].reshape((N_ctrl+1,1)))
#plt.plot( X_total[:,0], Y_total[:,0], 'r* ', markersize=15,)
exercizes/ex_4_walking.py 0 → 100644
View file @ bd2811f7
import numpy as np
import numpy.matlib as matlib
from numpy import nan
from numpy.linalg import norm as norm
import matplotlib.pyplot as plt
import plot_utils as plut
import time
import ex_4_conf as conf
from tsid_biped import TsidBiped
print "".center(conf.LINE_WIDTH,'#')
print " Test Walking ".center(conf.LINE_WIDTH, '#')
print "".center(conf.LINE_WIDTH,'#'), '\n'
data = np.load(conf.DATA_FILE)
tsid = TsidBiped(conf)
N = data['com'].shape[1]
com_pos = matlib.empty((3, N))*nan
com_vel = matlib.empty((3, N))*nan
com_acc = matlib.empty((3, N))*nan
f_RF = matlib.zeros((6, N))
f_LF = matlib.zeros((6, N))
cop_RF = matlib.zeros((2, N))
cop_LF = matlib.zeros((2, N))
foot_steps = np.asmatrix(data['foot_steps'])
contact_phase = data['contact_phase']
com_pos_ref = np.asmatrix(data['com'])
com_vel_ref = np.asmatrix(data['dcom'])
com_acc_ref = np.asmatrix(data['ddcom'])*1.0
com_acc_des = matlib.empty((3, N))*nan # acc_des = acc_ref - Kp*pos_err - Kd*vel_err
x_rf = tsid.get_placement_RF().translation
offset = matlib.zeros((3,1))
offset[:2,0] = x_rf[:2,0] - foot_steps[0,:].T #tsid.robot.com(tsid.formulation.data())
for i in range(N):
com_pos_ref[:,i] += offset
# foot_steps[:,i] += offset[:2,0]
sampleCom = tsid.trajCom.computeNext()
t = 0.0
q, v = tsid.q, tsid.v
for i in range(-2000, N):
time_start = time.time()
if i==0:
print "Starting to walk (remove contact left foot)"
tsid.remove_contact_LF()
elif i>0:
if contact_phase[i] != contact_phase[i-1]:
print "Changing contact phase from %s to %s"%(contact_phase[i-1], contact_phase[i])
if contact_phase[i] == 'left':
tsid.add_contact_LF()
tsid.remove_contact_RF()
else:
tsid.add_contact_RF()
tsid.remove_contact_LF()
if i<0:
sampleCom.pos(com_pos_ref[:,0])
else:
sampleCom.pos(com_pos_ref[:,i])
sampleCom.vel(com_vel_ref[:,i])
sampleCom.acc(com_acc_ref[:,i])
tsid.comTask.setReference(sampleCom)
tsid.rightFootTask.setReference(tsid.trajRF.computeNext())
tsid.leftFootTask.setReference(tsid.trajLF.computeNext())
HQPData = tsid.formulation.computeProblemData(t, q, v)
sol = tsid.solver.solve(HQPData)
if(sol.status!=0):
print "QP problem could not be solved! Error code:", sol.status
break
if norm(v,2)>20.0:
print "Time %.3f Velocities are too high, stop everything!"%(t), norm(v)
break
tau = tsid.formulation.getActuatorForces(sol)
dv = tsid.formulation.getAccelerations(sol)
if i>=0:
com_pos[:,i] = tsid.robot.com(tsid.formulation.data())
com_vel[:,i] = tsid.robot.com_vel(tsid.formulation.data())
com_acc[:,i] = tsid.comTask.getAcceleration(dv)
com_acc_des[:,i] = tsid.comTask.getDesiredAcceleration
if tsid.formulation.checkContact(tsid.contactRF.name, sol):
T_RF = tsid.contactRF.getForceGeneratorMatrix
f_RF[:,i] = T_RF * tsid.formulation.getContactForce(tsid.contactRF.name, sol)
if(f_RF[2,i]>1e-3):
cop_RF[0,i] = f_RF[4,i] / f_RF[2,i]
cop_RF[1,i] = -f_RF[3,i] / f_RF[2,i]
if tsid.formulation.checkContact(tsid.contactLF.name, sol):
T_LF = tsid.contactRF.getForceGeneratorMatrix
f_LF[:,i] = T_LF * tsid.formulation.getContactForce(tsid.contactLF.name, sol)
if(f_LF[2,i]>1e-3):
cop_LF[0,i] = f_LF[4,i] / f_LF[2,i]
cop_LF[1,i] = -f_LF[3,i] / f_LF[2,i]
if i%conf.PRINT_N == 0:
print "Time %.3f"%(t)
if tsid.formulation.checkContact(tsid.contactRF.name, sol):
print "\tnormal force %s: %.1f"%(tsid.contactRF.name.ljust(20,'.'), f_RF[2,i])
if tsid.formulation.checkContact(tsid.contactLF.name, sol):
print "\tnormal force %s: %.1f"%(tsid.contactLF.name.ljust(20,'.'), f_LF[2,i])
print "\ttracking err %s: %.3f"%(tsid.comTask.name.ljust(20,'.'), norm(tsid.comTask.position_error, 2))
print "\t||v||: %.3f\t ||dv||: %.3f"%(norm(v, 2), norm(dv))
q, v = tsid.integrate_dv(q, v, dv, conf.dt)
t += conf.dt
if i%conf.DISPLAY_N == 0: tsid.robot_display.display(q)
time_spent = time.time() - time_start
if(time_spent < conf.dt): time.sleep(conf.dt-time_spent)
# PLOT STUFF
time = np.arange(0.0, N*conf.dt, conf.dt)
(f, ax) = plut.create_empty_figure(3,1)
for i in range(3):
ax[i].plot(time, com_pos[i,:].A1, label='CoM '+str(i))
ax[i].plot(time, com_pos_ref[i,:].A1, 'r:', label='CoM Ref '+str(i))
ax[i].set_xlabel('Time [s]')
ax[i].set_ylabel('CoM [m]')
leg = ax[i].legend()
leg.get_frame().set_alpha(0.5)
(f, ax) = plut.create_empty_figure(3,1)
for i in range(3):
ax[i].plot(time, com_vel[i,:].A1, label='CoM Vel '+str(i))
ax[i].plot(time, com_vel_ref[i,:].A1, 'r:', label='CoM Vel Ref '+str(i))
ax[i].set_xlabel('Time [s]')
ax[i].set_ylabel('CoM Vel [m/s]')
leg = ax[i].legend()
leg.get_frame().set_alpha(0.5)
(f, ax) = plut.create_empty_figure(3,1)
for i in range(3):
ax[i].plot(time, com_acc[i,:].A1, label='CoM Acc '+str(i))
ax[i].plot(time, com_acc_ref[i,:].A1, 'r:', label='CoM Acc Ref '+str(i))
ax[i].plot(time, com_acc_des[i,:].A1, 'g--', label='CoM Acc Des '+str(i))
ax[i].set_xlabel('Time [s]')
ax[i].set_ylabel('CoM Acc [m/s^2]')
leg = ax[i].legend()
leg.get_frame().set_alpha(0.5)
(f, ax) = plut.create_empty_figure(2,1)
for i in range(2):
ax[i].plot(time, cop_LF[i,:].A1, label='CoP LF '+str(i))
ax[i].plot(time, cop_RF[i,:].A1, label='CoP RF '+str(i))
ax[i].set_xlabel('Time [s]')
ax[i].set_ylabel('CoP [m]')
leg = ax[i].legend()
leg.get_frame().set_alpha(0.5)
(f, ax) = plut.create_empty_figure(3,2)
ax = ax.reshape((6))
for i in range(6):
ax[i].plot(time, f_LF[i,:].A1, label='Force LF '+str(i))
ax[i].plot(time, f_RF[i,:].A1, label='Force RF '+str(i))
ax[i].set_xlabel('Time [s]')
ax[i].set_ylabel('Force [N/Nm]')
leg = ax[i].legend()
leg.get_frame().set_alpha(0.5)
plt.show()
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