Euler's Method is a numerical technique applied in the realm of initial value problems for ordinary differential equations (ODEs). The simplicity of this method makes it a popular choice in cases where the differential equation lacks a closed-form solution. The method might not always provide the most accurate result, but it offers a good trade-off between simplicity and accuracy.
Consider an initial value problem (IVP) represented as:
This IVP can be solved by Euler's method, where the method employs the following approximation:
where:
-
$u_{n+1}$ is the approximate value of$u$ at$t = t_n + h$ , -
$u_n$ is the approximate value of$u$ at$t = t_n$ , -
$h$ is the step size, -
$f(t_n, u_n)$ is the derivative of$u$ at$t = t_n$ .
Let's start with the Taylor series:
We may alternatively rewrite the above equation as follows:
Which is roughly equivalent to:
- Start with initial conditions
$t_0$ and$u_0$ . - Calculate
$u_{n+1}$ using the formula:$u_{n+1} = u_n + h*f(t_n, u_n)$ . - Repeat the above step for a given number of steps or until the final value of
$t$ is reached.
Let's choose the step value:
We start at
Now that we know
- Euler's method is easy to implement and serves as a foundational technique for introducing numerical solution methods for ODEs.
- It can provide reasonable approximations for well-behaved functions when the step size is sufficiently small.
- The simplicity of the method makes it computationally inexpensive for basic problems and suitable for initial experimentation.
- Accuracy is limited, as the method can introduce significant errors if the step size is too large or if the function has rapid changes.
- The cumulative error from each step can grow significantly, making the method unsuitable for long-time integration.
- Stability is an issue, as Euler's method may fail to converge or produce reliable results for stiff or oscillatory ODEs.
- The method lacks the ability to adapt step sizes dynamically, which can lead to inefficiencies or inaccuracies in varying conditions.