# Difference between revisions of "Numerical Methods for Ordinary Differential Equations"

### Reference Materials

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\begin{document} \section{ Numerical Integration Methods }

Numerical integration is used to solve ODEs that cannot be solved analytically, generally through discretization of the ODE. Since the conception of the modern computer, numerical integration methods have become an essential tool in the physical sciences and beyond. Here we will describe two of many such methods, along with some sample code.

\subsection*{ The Euler Method }

The Euler Method is the simplest numerical integration method, and is most likely the only one you will need to use in C207. Here, we'll walk through how it works and show some examples of how to implement it. Imagine you have some ODE:

$$\frac{dy}{dx} = f(x,y)$$

with some initial condition $y(x_0) = y_0$. Now, let's say we want to determine the value of $y_1$ at some new value of $x_1$ that is close to $x_0$. We can estimate this by rearranging the ODE above into the following form:

$$\frac{y_{1} - y_{0}}{x_{1} - x_{0}} = f(x_0,y_0)$$

which we can write as:

$$y_{1} = y_{0} + (x_{1} - x_{0}) f(x_0,y_0) = y_{0} + h f(x_0,y_0)$$

where $(x_{1} - x_{0}) = h$ is called the "step size. We can generalize this equation with the following recursive relation:

$$y_{i+1} = y_{i} + h f(x_{i},y_{i})$$

where the step size is typically set as some constant value. As we will see, smaller step sizes produce more accurate integration results. More precisely, the error is on the order of $O(h)$ (i.e., reducing $h$ by a factor of two makes the Euler method twice as accurate).

\\[12pt] \\[12pt]

Now that we have a simple integration scheme, let's see how we'd execute this in python. Say our ODE is:

$$\frac{dy}{dx} = y$$

and our initial condition is $y(0) = 1$. We can solve this analytically, but let's see what we get using the Euler method for different values of $h$.

\begin{verbatim}

.import numpy as np .import matplotlib.pyplot as plt . .# plot analytic solution .plt.figure(figsize=(10,4)) .x_analytic = np.linspace(0,5,100) .y_analytic = np.exp(x_analytic) .plt.plot(x_analytic, y_analytic, 'k--', label='analytic solution') . .# define initial condition and values of h that will be used .x0 = 0 .y0 = 1 .h_values = np.array([0.1,0.5,1.0]) . .for h in h_values: . # define arrays that can be used to record x and y . x = np.zeros([100]) . x[0] = x0 . y = np.zeros([100]) . y[0] = y0 . # execute integration for current value of h . for i in range(1, len(y)): . x[i] = x[i-1] + h . dydx = y[i-1] . y[i] = y[i-1] + h*dydx . # plot curve for current value of h . plt.plot(np.trim_zeros(x, 'b'), np.trim_zeros(y, 'b'), label='h = '+str(h)) . .# remainder of plotting routine .plt.xlabel('x', fontsize=12) .plt.ylabel('y', fontsize=12) .plt.xlim([0,7]) .plt.ylim([0,100]) .plt.legend(loc=2, fontsize=12) .plt.tight_layout() .plt.show()

\end{verbatim}

\begin{center} \end{center}

As we can see, the curve obtained using the Euler method converges to the analytic solution as $h \rightarrow 0$. Therefore, you must be careful to use a value of $h$ small enough to produce realistic results when performing numerical integrations.

\\[12pt] \\[12pt]

Since this is an astrophysics course, let's conclude this section with a more relevant example. Let's calculate the trajectory of a relativistic electron in the presence of an electric field (see: Synchrotron radiation). In this case,

\subsection*{ The Runge-Kutta Method }

\section{ Monte Carlo Methods }

\subsection*{ Monte Carlo Sampling }

\subsection*{ Markov Chain Monte Carlo }

\end{document} <\latex>