In [48]:
# Double pendulum formula translated from the C code at
# http://www.physics.usyd.edu.au/~wheat/dpend_html/solve_dpend.c
from numpy import sin, cos, pi, array
import numpy as np
import matplotlib.pyplot as plt
import scipy.integrate as integrate
import matplotlib.animation as animation
In [49]:
import pickle
arquivo = open("../xyz", "r")
X = pickle.loads(arquivo.read())
print X.shape
joelho = X[0,:,:].T
trocanter = X[1,:,:].T
tibia = X[2,:,:].T
x_min = np.min(np.array([joelho[:, 0], trocanter[:, 0], tibia[:, 0]]))
x_max = np.max(np.array([joelho[:, 0], trocanter[:, 0], tibia[:, 0]]))
y_min = np.min(np.array([joelho[:, 1], trocanter[:, 1], tibia[:, 1]]))
y_max = np.max(np.array([joelho[:, 1], trocanter[:, 1], tibia[:, 1]]))
z_min = np.min(np.array([joelho[:, 2], trocanter[:, 2], tibia[:, 2]]))
z_max = np.max(np.array([joelho[:, 2], trocanter[:, 2], tibia[:, 2]]))
print joelho.shape
In [50]:
G = 9.8 # acceleration due to gravity, in m/s^2
L1 = 1.0 # length of pendulum 1 in m
L2 = 1.0 # length of pendulum 2 in m
M1 = 1.0 # mass of pendulum 1 in kg
M2 = 1.0 # mass of pendulum 2 in kg
In [51]:
def derivs(state, t):
dydx = np.zeros_like(state)
dydx[0] = state[1]
del_ = state[2]-state[0]
den1 = (M1+M2)*L1 - M2*L1*cos(del_)*cos(del_)
dydx[1] = (M2*L1*state[1]*state[1]*sin(del_)*cos(del_)
+ M2*G*sin(state[2])*cos(del_) + M2*L2*state[3]*state[3]*sin(del_)
- (M1+M2)*G*sin(state[0]))/den1
dydx[2] = state[3]
den2 = (L2/L1)*den1
dydx[3] = (-M2*L2*state[3]*state[3]*sin(del_)*cos(del_)
+ (M1+M2)*G*sin(state[0])*cos(del_)
- (M1+M2)*L1*state[1]*state[1]*sin(del_)
- (M1+M2)*G*sin(state[2]))/den2
return dydx
In [52]:
# create a time array from 0..100 sampled at 0.05 second steps
dt = 0.05
t = np.arange(0.0, 20, dt)
# th1 and th2 are the initial angles (degrees)
# w10 and w20 are the initial angular velocities (degrees per second)
th1 = 120.0
w1 = 0.0
th2 = -10.0
w2 = 0.0
rad = pi/180
In [53]:
# initial state
state = np.array([th1, w1, th2, w2])*pi/180.
# integrate your ODE using scipy.integrate.
y = integrate.odeint(derivs, state, t)
x1 = L1*sin(y[:,0])
y1 = -L1*cos(y[:,0])
x2 = L2*sin(y[:,2]) + x1
y2 = -L2*cos(y[:,2]) + y1
fig = plt.figure()
ax = fig.add_subplot(111, autoscale_on=False, xlim=(x_min, x_max), ylim=(z_min, z_max))
ax.grid()
line, = ax.plot([], [], 'o-', lw=2)
time_template = 'time = %.1fs'
time_text = ax.text(0.05, 0.9, '', transform=ax.transAxes)
In [ ]:
def init():
line.set_data([], [])
time_text.set_text('')
return line, time_text
def animate(i):
thisx = [trocanter[i, 0], joelho[i, 0], tibia[i, 0]]
thisy = [trocanter[i, 2], joelho[i, 1], tibia[i, 2]]
line.set_data(thisx, thisy)
return line, time_text
ani = animation.FuncAnimation(fig, animate, np.arange(1, 66),
interval=25, blit=False, init_func=init)
#ani.save('double_pendulum.mp4', fps=15)
plt.show()
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