Presentation is loading. Please wait.

Presentation is loading. Please wait.

Constrained Dynamics. Spring 20062 A Bead on a Wire x f.

Similar presentations


Presentation on theme: "Constrained Dynamics. Spring 20062 A Bead on a Wire x f."— Presentation transcript:

1 Constrained Dynamics

2 Spring 20062 A Bead on a Wire x f

3 Spring 20063 A Bead on a Wire x f Zero rate-of- change ensures constant C!

4 Spring 20064 A Bead on a Wire x f

5 Spring 20065 A Bead on a Wire x f

6 Spring 20066 A Bead on a Wire x f However, one equation cannot solve two unknowns of f- hat!?

7 Spring 20067 A Bead on a Wire x f Constraint force does not produce work

8 Spring 20068 Constrained Dynamics General Recipe

9 Spring 20069 Constrained Dynamics

10 Spring 200610 About Constraint Force … Q q Constraint force Q-hat induced by Q to move q along legal velocity q-dot

11 Spring 200611 About Constraint Force … Q q Legal velocity q-dot is  to the hyperplane spanned by the gradients of all constraints. Hence, constraint force is a linear combination of all gradients.

12 Spring 200612 Numerical Concerns To account for numerical drift, we often apply numerical damping as follows:

13 Spring 200613 Ex: Bead in Recipe x Q

14 Spring 200614 Example: Double Pendulum l1l1 l2l2 p1p1 p2p2


Download ppt "Constrained Dynamics. Spring 20062 A Bead on a Wire x f."

Similar presentations


Ads by Google