Timeline for Showing The Laplace–Runge–Lenz vector (per unit mass) is constant
Current License: CC BY-SA 3.0
10 events
when toggle format | what | by | license | comment | |
---|---|---|---|---|---|
Oct 25, 2017 at 12:25 | comment | added | sammy gerbil | See Show that the Laplace-Runge-Lenz vector is conserved using poisson brackets | |
Jun 17, 2017 at 10:17 | comment | added | Theorem | Alright I got it thanks! and is there no way in which you don't use $\theta$-vectors? Seems like an overkill... | |
Jun 17, 2017 at 8:33 | comment | added | David Hammen | @Theorem - Use that to calculate $\vec H$ and then $\hat r \times \vec H$. Everything will cancel. | |
Jun 17, 2017 at 7:28 | comment | added | Theorem | @David $\dot{\hat{r}}=\dot{\theta}\hat{\theta}$ so $\dot{\vec{r}}=\dot{r}\hat{r}+r\dot{\theta}\hat{\theta}$ but what does that give me? | |
Jun 17, 2017 at 7:28 | comment | added | Theorem | @Qmechanic the maths there is over the top for me and it doesn't revole around the one per unit mass. | |
Jun 16, 2017 at 19:30 | comment | added | Qmechanic♦ | Related: physics.stackexchange.com/q/18088/2451 and links therein. | |
Jun 16, 2017 at 19:29 | history | edited | Qmechanic♦ |
edited tags
|
|
Jun 16, 2017 at 19:15 | history | edited | David Hammen |
edited tags
|
|
Jun 16, 2017 at 19:14 | comment | added | David Hammen | This looks like homework, so just a hint: Start with $\vec r = r \hat r$. What is it's time derivative? To answer that, you'll need to answer the auxiliary question, what is the time derivative of $\hat r$? | |
Jun 16, 2017 at 18:54 | history | asked | Theorem | CC BY-SA 3.0 |