Worksheets/Eulers Method Circuits: Difference between revisions
From charlesreid1
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=Content= | |||
==Introduction== | |||
Today we will be using a spreadsheet program to implement Euler’s Method and solve a differential equation. Euler’s Method ties together the concepts of numerical integration and differential equations. We will implement Euler’s Method to solve for the current in the following circuit: | |||
This circuit is described in Example 4 of Section 9.5 of the Stewart Calculus textbook. | |||
==Euler's Method== | |||
We can use Euler’s Method to solve a differential equation of the general form: | |||
<math> | |||
\frac{dy}{dt} = F(t,y) | |||
</math> | |||
We start by chopping up the time domain into a set of steps of size <math>\Delta</math>. We will evaluate the solution, and the right‐hand side of the equation, at each timestep. | |||
Start by turning the derivative on the left‐hand side into a finite difference quotient: | |||
<math> | |||
\frac{dy}{dt} \approx \frac{\Delta y}{\Delta t} | |||
</math> | |||
Next, using the fact that <math>\Delta y = y(t+\Delta t)-y(t)</math>, we can write a relationship between the solution at a given time step <math>t_i</math>, denoted <math>y_i = y(t_i)</math>, and the solution at the next timestep <math>t_{i+1} = t_i + \Delta t</math>, denoted <math>y_{i+1}</math>: | |||
<math> | |||
y_{i+1} = y_i + \Delta t \left( F(t,y) \right) | |||
</math> | |||
Revision as of 17:45, 8 May 2016
Background
Setup of basic equation describing a simple inductor circuit - how does an inductor work, what is an inductor used for, how can we model the inductor
Inductor coil in electrical circuit: solving the differential equation for current
Setting up the use of Simpson's Rule to implement Euler's Method and integrate Right Hand side, with Delta x instead of Delta t.
Electrical circuit
Solving a differential equation
Different right-hand sides, different time steps
Content
Introduction
Today we will be using a spreadsheet program to implement Euler’s Method and solve a differential equation. Euler’s Method ties together the concepts of numerical integration and differential equations. We will implement Euler’s Method to solve for the current in the following circuit:
This circuit is described in Example 4 of Section 9.5 of the Stewart Calculus textbook.
Euler's Method
We can use Euler’s Method to solve a differential equation of the general form:
$ \frac{dy}{dt} = F(t,y) $
We start by chopping up the time domain into a set of steps of size $ \Delta $. We will evaluate the solution, and the right‐hand side of the equation, at each timestep.
Start by turning the derivative on the left‐hand side into a finite difference quotient:
$ \frac{dy}{dt} \approx \frac{\Delta y}{\Delta t} $
Next, using the fact that $ \Delta y = y(t+\Delta t)-y(t) $, we can write a relationship between the solution at a given time step $ t_i $, denoted $ y_i = y(t_i) $, and the solution at the next timestep $ t_{i+1} = t_i + \Delta t $, denoted $ y_{i+1} $:
$ y_{i+1} = y_i + \Delta t \left( F(t,y) \right) $