Difference between revisions of "Matlab Primer"

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(Step 1: Make the model first order)
(Step 1: Make the model first order)
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Now we have two equations:
 
Now we have two equations:
  
<math> \dot\theta_0 = \theta_1,
+
<math> \begin{align} \dot\theta_0 & = \theta_1,
  \dot\theta_1 = - \frac{g}{\ell} \sin\theta_0 </math>
+
  \dot\theta_1 & = - \frac{g}{\ell} \sin\theta_0 \end{align} </math>

Revision as of 18:30, 3 November 2012

Today's lecture will be on MATLAB and PENDULA (plural of PENDULUM). Your next lab assignment motivated the topic.

My name is Sean Carver; I am a research scientist in Mechanical Engineering. I have been programming in MATLAB for almost 20 years and programming computers for almost 30 years.

This class is about MATLAB, not about deriving equations. So I am just going to give you the equations for the PENDULUM. There is still a lot to do to get it into MATLAB.

Pendulum on a movable support

This example comes from Wikipedia (copied legally). Consider a pendulum of mass m and length , which is attached to a support with mass M which can move along a line in the x-direction. Let x be the coordinate along the line of the support, and let us denote the position of the pendulum by the angle θ from the vertical.

Sketch of the situation with definition of the coordinates (click to enlarge)
\ddot\theta + \frac{\ddot x}{\ell} \cos\theta + \frac{g}{\ell} \sin\theta = 0.\,

See http://en.wikipedia.org/w/index.php?title=Lagrangian_mechanics&oldid=516894618 for a full derivation.

Your homework and class exercise for today is to implement this model.

Pendulum on a fixed support

Together we are going to implement a simpler model with support fixed and unmovable. You can see what the equations for this are easily. Just plug in

\ddot x = \dot x = x = 0

The second term drops out:

\ddot\theta + \frac{g}{\ell} \sin\theta = 0.\,

Step 1: Make the model first order

Define new variables

\begin{align}
\theta_0 & = \theta, \\
 \theta_1 & = \dot\theta \end{align}

Now we have two equations:

 \begin{align} \dot\theta_0 & = \theta_1,
 \dot\theta_1 & = - \frac{g}{\ell} \sin\theta_0 \end{align}