54bce9d7a0
Still needs a lot of explanation; mostly the implementation is there for now.
260 lines
6.4 KiB
Python
260 lines
6.4 KiB
Python
# -*- coding: utf-8 -*-
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"""
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Created on Thu May 28 20:23:57 2015
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@author: rlabbe
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"""
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from math import cos, sin, sqrt, atan2, tan
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import matplotlib.pyplot as plt
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import numpy as np
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from numpy import array, dot
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from numpy.linalg import pinv
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from numpy.random import randn
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from filterpy.common import plot_covariance_ellipse
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from filterpy.kalman import ExtendedKalmanFilter as EKF
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def print_x(x):
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print(x[0, 0], x[1, 0], np.degrees(x[2, 0]))
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def normalize_angle(x, index):
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if x[index] > np.pi:
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x[index] -= 2*np.pi
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if x[index] < -np.pi:
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x[index] = 2*np.pi
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def residual(a,b):
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y = a - b
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normalize_angle(y, 1)
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return y
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sigma_r = 0.1
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sigma_h = np.radians(1)
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sigma_steer = np.radians(1)
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#only partway through. predict is using old control and movement code. computation of m uses
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#old u.
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class RobotEKF(EKF):
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def __init__(self, dt, wheelbase):
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EKF.__init__(self, 3, 2, 2)
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self.dt = dt
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self.wheelbase = wheelbase
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def predict(self, u=0):
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self.x = self.move(self.x, u, self.dt)
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h = self.x[2, 0]
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v = u[0]
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steering_angle = u[1]
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dist = v*self.dt
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if abs(steering_angle) < 0.0001:
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# approximate straight line with huge radius
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r = 1.e-30
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b = dist / self.wheelbase * tan(steering_angle)
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r = self.wheelbase / tan(steering_angle) # radius
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sinh = sin(h)
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sinhb = sin(h + b)
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cosh = cos(h)
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coshb = cos(h + b)
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F = array([[1., 0., -r*cosh + r*coshb],
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[0., 1., -r*sinh + r*sinhb],
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[0., 0., 1.]])
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w = self.wheelbase
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F = array([[1., 0., (-w*cosh + w*coshb)/tan(steering_angle)],
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[0., 1., (-w*sinh + w*sinhb)/tan(steering_angle)],
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[0., 0., 1.]])
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print('F', F)
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V = array(
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[[-r*sinh + r*sinhb, 0],
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[r*cosh + r*coshb, 0],
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[0, 0]])
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t2 = tan(steering_angle)**2
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V = array([[0, w*sinh*(-t2-1)/t2 + w*sinhb*(-t2-1)/t2],
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[0, w*cosh*(-t2-1)/t2 - w*coshb*(-t2-1)/t2],
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[0,0]])
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t2 = tan(steering_angle)**2
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a = steering_angle
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d = v*dt
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it = dt*v*tan(a)/w + h
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V[0,0] = dt*cos(d/w*tan(a) + h)
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V[0,1] = (dt*v*(t2+1)*cos(it)/tan(a) -
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w*sinh*(-t2-1)/t2 +
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w*(-t2-1)*sin(it)/t2)
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print(dt*v*(t2+1)*cos(it)/tan(a))
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print(w*sinh*(-t2-1)/t2)
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print(w*(-t2-1)*sin(it)/t2)
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V[1,0] = dt*sin(it)
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V[1,1] = (d*(t2+1)*sin(it)/tan(a) + w*cosh/t2*(-t2-1) -
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w*(-t2-1)*cos(it)/t2)
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V[2,0] = dt/w*tan(a)
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V[2,1] = d/w*(t2+1)
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theta = h
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v01 = (dt*v*(tan(a)**2 + 1)*cos(dt*v*tan(a)/w + theta)/tan(a) -
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w*(-tan(a)**2 - 1)*sin(theta)/(tan(a)**2) +
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w*(-tan(a)**2 - 1)*sin(dt*v*tan(a)/w + theta)/(tan(a)**2))
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print(dt*v*(tan(a)**2 + 1)*cos(dt*v*tan(a)/w + theta)/tan(a))
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print(w*(-tan(a)**2 - 1)*sin(theta)/(tan(a)**2))
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print(w*(-tan(a)**2 - 1)*sin(dt*v*tan(a)/w + theta)/(tan(a)**2))
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'''v11 = (dt*v*(tan(a)**2 + 1)*sin(dt*v*tan(a)/w + theta)/tan(a) +
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w*(-tan(a)**2 - 1)*cos(theta)/tan(a)**2 -
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w*(-tan(a)**2 - 1)*cos(dt*v*tan(a)/w + theta)/tan(a)**2)
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print(dt*v*(tan(a)**2 + 1)*sin(dt*v*tan(a)/w + theta)/tan(a))
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print(w*(-tan(a)**2 - 1)*cos(theta)/tan(a)**2)
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print(w*(-tan(a)**2 - 1)*cos(dt*v*tan(a)/w + theta)/tan(a)**2)
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print(v11)
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print(V[1,1])
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1/0
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V[1,1] = v11'''
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print(V)
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# covariance of motion noise in control space
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M = array([[0.1*v**2, 0],
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[0, sigma_steer**2]])
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fpf = dot(F, self.P).dot(F.T)
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Q = dot(V, M).dot(V.T)
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print('FPF', fpf)
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print('V', V)
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print('Q', Q)
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print()
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self.P = dot(F, self.P).dot(F.T) + dot(V, M).dot(V.T)
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def move(self, x, u, dt):
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h = x[2, 0]
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v = u[0]
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steering_angle = u[1]
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dist = v*dt
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if abs(steering_angle) < 0.0001:
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# approximate straight line with huge radius
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r = 1.e-30
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b = dist / self.wheelbase * tan(steering_angle)
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r = self.wheelbase / tan(steering_angle) # radius
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sinh = sin(h)
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sinhb = sin(h + b)
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cosh = cos(h)
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coshb = cos(h + b)
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return x + array([[-r*sinh + r*sinhb],
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[r*cosh - r*coshb],
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[b]])
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def H_of(x, p):
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""" compute Jacobian of H matrix where h(x) computes the range and
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bearing to a landmark for state x """
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px = p[0]
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py = p[1]
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hyp = (px - x[0, 0])**2 + (py - x[1, 0])**2
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dist = np.sqrt(hyp)
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H = array(
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[[-(px - x[0, 0]) / dist, -(py - x[1, 0]) / dist, 0],
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[ (py - x[1, 0]) / hyp, -(px - x[0, 0]) / hyp, -1]])
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return H
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def Hx(x, p):
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""" takes a state variable and returns the measurement that would
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correspond to that state.
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"""
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px = p[0]
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py = p[1]
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dist = np.sqrt((px - x[0, 0])**2 + (py - x[1, 0])**2)
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Hx = array([[dist],
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[atan2(py - x[1, 0], px - x[0, 0]) - x[2, 0]]])
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return Hx
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dt = 1.0
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ekf = RobotEKF(dt, wheelbase=0.5)
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#np.random.seed(1234)
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m = array([[5, 10],
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[10, 5],
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[15, 15]])
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ekf.x = array([[2, 6, .3]]).T
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u = array([.5, .01])
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ekf.P = np.diag([1., 1., 1.])
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ekf.R = np.diag([sigma_r**2, sigma_h**2])
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c = [0, 1, 2]
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xp = ekf.x.copy()
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plt.scatter(m[:, 0], m[:, 1])
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for i in range(300):
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xp = ekf.move(xp, u, dt/10.) # simulate robot
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plt.plot(xp[0], xp[1], ',', color='g')
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if i % 10 == 0:
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ekf.predict(u=u)
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plot_covariance_ellipse((ekf.x[0,0], ekf.x[1,0]), ekf.P[0:2, 0:2], std=2,
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facecolor='b', alpha=0.3)
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for lmark in m:
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d = sqrt((lmark[0] - xp[0, 0])**2 + (lmark[1] - xp[1, 0])**2) + randn()*sigma_r
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a = atan2(lmark[1] - xp[1, 0], lmark[0] - xp[0, 0]) - xp[2, 0] + randn()*sigma_h
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z = np.array([[d], [a]])
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ekf.update(z, HJacobian=H_of, Hx=Hx, residual=residual,
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args=(lmark), hx_args=(lmark))
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plot_covariance_ellipse((ekf.x[0,0], ekf.x[1,0]), ekf.P[0:2, 0:2], std=10,
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facecolor='g', alpha=0.3)
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#plt.plot(ekf.x[0], ekf.x[1], 'x', color='r')
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plt.axis('equal')
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plt.show()
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