Week5: upto c)
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week5/ex1.py
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week5/ex1.py
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#!/usr/bin/env python3
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"""Ordinary Differential Equations"""
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import numpy as np
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def mk_phi_euler(f):
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""" Return a Phi computed for the Euler Method. """
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def phi_euler(x, y, h):
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return f(x[-1], y[-1])
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return phi_euler
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def mk_phi_euler_mod(f):
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""" Return a Phi computed for the Modified Euler (Collatz) Method. """
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def phi_euler_mod(x, y, h):
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return f(x[-1] + 0.5*h, y[-1] + 0.5*h*f(x[-1], y[-1]))
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return phi_euler_mod
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def mk_phi_heun(f):
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""" Return a Phi computed for the Heun Method. """
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def phi_heun(x, y, h):
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return (f(x[-1], y[-1]) + f(x[-1] + h, y[-1] + h * f(x[-1], y[-1])))/2
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return phi_heun
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def mk_phi_rk4(f):
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""" Return a Phi computed for the 4th order Runge-Kutta Method. """
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def phi_rk4(x, y, h):
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k1 = f(x[-1], y[-1])
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k2 = f(x[-1] + 0.5*h, y[-1] + 0.5*k1)
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k3 = f(x[-1] + 0.5*h, y[-1] + 0.5*h*k2)
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k4 = f(x[-1] + h, y[-1] + h*k3)
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return (k1 + 2*k2 + 2*k3 + k4)/6
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return phi_rk4
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def integrator(x, y_0, phi):
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x = np.asarray(x)
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if isinstance(y_0, (list,np.ndarray)):
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y_0 = np.asarray(y_0)
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else:
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y_0 = np.array([ y_0 ])
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N = len(x)
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M = len(y_0)
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y = np.zeros((N,M), dtype=np.float64)
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y[0] = y_0
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h = x[1]-x[0]
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for i, x_i in enumerate(x):
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# Skip the first iteration
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if not i:
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continue
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y[i] = y[i-1] + h*phi(x[:i], y[:i], h)
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return y
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def test_integrator():
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np.random.seed(0)
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def ODEF(x, y):
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return y - x**2 + 1
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def ODEF_sol(x):
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return (x+1)**2 - 0.5*np.exp(x)
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test_func = ODEF
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exact_sol = ODEF_sol
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N = 2e1
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M = 1
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# Domain on which to do the integration
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x = np.linspace(0, 1, N)
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# Generate Initial Value
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y_0 = 0.5
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schemes = [
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["Euler", mk_phi_euler],
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["Collatz", mk_phi_euler_mod],
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["Heun", mk_phi_heun],
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["RK4", mk_phi_rk4],
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]
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# Show Plot
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from matplotlib import pyplot
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pyplot.subplots()
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for name, func in schemes:
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pyplot.plot(x, integrator(x, y_0, func(test_func)), '--o', label=name)
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pyplot.plot(x, exact_sol(x), '-', label="Exact Solution")
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pyplot.xlabel("x")
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pyplot.ylabel("y")
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pyplot.legend()
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pyplot.show()
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if __name__ == "__main__":
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test_integrator()
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