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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
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Jun 16, 2017 at 19:15 history edited David Hammen
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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