Runge Kutta 4和python中的摆锤模拟 [英] Runge Kutta 4 and pendulum simulation in python

问题描述

我正在尝试制作一个使用runge kutta 4绘制摆幅的python程序.我拥有的方程是角加速度= -(m*g*r/I) * np.sin(y).

I am trying to make a python program which plot pendulum swings using runge kutta 4. The equation I have is angular accelartion = -(m*g*r/I) * np.sin(y).

请找到我的代码.我是python的新手.

Please find my code. I am quite new to python.

import numpy as np 
import matplotlib.pyplot as plt 
m = 3.0
g = 9.8
r = 2.0
I = 12.0
h = 0.0025 
l=2.0
cycle = 10.0
t = np.arange(0, cycle, h)
n = (int)((cycle)/h)  
initial_angle = 90.0
y=np.zeros(n)
v=np.zeros(n)
def accel(theta):
  return -(m*g*r/I)*np.sin(theta)
y[0] = np.radians(initial_angle) 
v[0] = np.radians(0.0)
for i in range(0, n-1): 
    k1y = h*v[i]
    k1v = h*accel(y[i])
    k2y = h*(v[i]+0.5*k1v)
    k2v = h*accel(y[i]+0.5*k1y)
    k3y = h*(v[i]+0.5*k2v)
    k3v = h*accel(y[i]+0.5*k2y)
    k4y = h*(v[i]+k3v)
    k4v = h*accel(y[i]+k3y)
    y[i+1] = y[i] + (k1y + 2 * k2y + 2 * k3y + k4y) / 6.0 
    v[i+1] = v[i] + (k1v + 2 * k2v + 2 * k3v + k4v) / 6.0

plt.plot(t, y)
plt.title('Pendulum Motion:')
plt.xlabel('time (s)')
plt.ylabel('angle (rad)')
plt.grid(True)
plt.show()

我现在更新了代码.我正正弦. 谢谢.

I have updated code now. I am getting sine way. Thank you..

推荐答案

您已经应用了RK4步骤，就好像在求解一阶方程式一样.您需要将二阶方程转换为一阶系统，然后求解该耦合系统.

You have applied the RK4 steps as if you were solving a first order equation. You need to transform the second order equation into a first order system and then solve that coupled system.

v = dy/dt
acceleration = dv/dt

所以RK4的每个步骤都有两个组成部分

so that each step in RK4 has two components

k1y = h*v
k1v = h*accel(y)

k2y = h*(v+0.5*k1v)
k2v = h*accel(y+0.5*k1y)

等

完整的代码给出了一个很好的正弦波

The complete code gives then a nice sine wave

import numpy as np 
import matplotlib.pyplot as plt 
m = 3.0
g = 9.8
r = 2.0
I = 12.0
h = 0.0025 
l=2.0
cycle = 10.0
t = np.arange(0, cycle, h)
# step height h 
n = len(t) 
initial_angle = 90.0
y=np.zeros(n)
v=np.zeros(n)
def accel(theta): return -(m*g*r/I)*np.sin(theta)
y[0] = np.radians(initial_angle) 
v[0] = np.radians(0.0)

for i in range(0, n-1): 
    k1y = h*v[i]
    k1v = h*accel(y[i])

    k2y = h*(v[i]+0.5*k1v)
    k2v = h*accel(y[i]+0.5*k1y)

    k3y = h*(v[i]+0.5*k2v)
    k3v = h*accel(y[i]+0.5*k2y)

    k4y = h*(v[i]+k3v)
    k4v = h*accel(y[i]+k3y)

    # Update next value of y 
    y[i+1] = y[i] + (k1y + 2 * k2y + 2 * k3y + k4y) / 6.0 
    v[i+1] = v[i] + (k1v + 2 * k2v + 2 * k3v + k4v) / 6.0

plt.plot(t, y)
plt.title('Pendulum Motion:')
plt.xlabel('time (s)')
plt.ylabel('angle (rad)')
plt.grid(True)
plt.show()

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