Lecture 12: Time Transfer Property
published: May 31, 2010, recorded: September 2007, views: 2788
released under terms of: Creative Commons Attribution Non-Commercial (CC-BY-NC)
Report a problem or upload filesIf you have found a problem with this lecture or would like to send us extra material, articles, exercises, etc., please use our ticket system to describe your request and upload the data.
Enter your e-mail into the 'Cc' field, and we will keep you updated with your request's status.
So here's what it tells you. It says that to get this state at time Tau plus T from the state at time Tau – first of all they're linearly related. That alone is – well, it's not unexpected, but they're linearly related. They're related by an end-by-end matrix that maps one to the other. And that matrix is simply E to the TA. So E to the TA is a time propagator. It propagates X dot equals AX forward T seconds in time. If T is negative it actually runs time backwards, and reconstructs what the state was some seconds ago. ...
See the whole transcript at Introduction to Linear Dynamical Systems - Lecture 12
Link this pageWould you like to put a link to this lecture on your homepage?
Go ahead! Copy the HTML snippet !