show that angular momentum conservation is equivalent to kepler's 2nd law?
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Consider a small wedge of the orbit traced out in time dt:
So the area of the wedge is
And the rate at which area is swept out on the orbit is
Now, remember(?) the definition of Angular Momentum:
Inserting this previous equation , we get
"Equal areas in equal times" means the rate at which area is swept out on the orbit (dA/dt) is constant.
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