Timeline for What is canonical momentum in rigid body systems?
Current License: CC BY-SA 4.0
5 events
| when toggle format | what | by | license | comment | |
|---|---|---|---|---|---|
| Dec 22, 2019 at 13:24 | answer | added | Arnold Neumaier | timeline score: 1 | |
| Dec 20, 2019 at 20:52 | comment | added | Joshua Tilley | @Qmechanic, not sure what you mean. Can you address my argument? | |
| Dec 20, 2019 at 17:27 | comment | added | Manvendra Somvanshi | I think you will have to consider two new Hamiltonian variables $\theta_i$ and $l_i$ and the Poisson brackets should be written in terms of these variables. Here $l_i$ will be the canonical momentum $\frac{\partial L}{\partial \dot{\theta}}$. | |
| Dec 20, 2019 at 16:57 | comment | added | Qmechanic♦ | Well, that's just different Poisson structures. | |
| Dec 20, 2019 at 16:11 | history | asked | Joshua Tilley | CC BY-SA 4.0 |