- #1

alexjean

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## Homework Statement

I am trying to show that as the alpha particle is being scattered, the angular momentum magnitude at point M is [itex]m r^2 \frac{d \phi}{dt}[/itex].

Diagram:

## Homework Equations

Linear Momentum: ##\vec L = \vec r \times \vec p ##

Repulsive Coulomb Force: ##\vec F = \frac{k 2Ze^2}{r^2} \frac{\vec r}{r}##

## The Attempt at a Solution

As the alpha particle approaches the nucleus, the repulsive force begins acting on it. Changing it's velocity:

##\vec v_M = \int_{t_{-\infty}}^{t_{M}} \frac{\vec F(\phi)}{m} t \, dt + \vec v_0 ##

If I could solve that integral, I would know the velocity for any angle ##\phi##. Allowing me to solve for angular momentum in terms of ##\vec r##. However, that integral is a mess. I would need to get time, ##t## in terms of ##\phi##. I've attempted that below, but it doesn't look promising:

##t = \frac{\Delta \vec r}{\vec v} ##

## t = \int \frac{1}{\vec v} \, d\vec r ##,

## t_M = \int_{<-\infty,0>}^{\vec r_M} \frac{1}{\vec v} \, d\vec r ##

## \frac{dt}{d\vec r} = \frac{1}{\vec v} ##

Substituting into the original integral:

## \vec v_M = \int_{<-\infty,0>}^{\vec r_M} \frac{\vec F(\phi)}{m} (\int_{<-\infty,0>}^{\vec r_M} \frac{1}{\vec v} \, d\vec r) \frac{1}{\vec v} \, d\vec r + \vec v_0 ##

Most derivations of this I've found online seem to glaze over the determination of angular momentum at point M, making me think I've missed something simple. Could anyone point me toward a better approach?