Angular momentum conserved for central forces not at origin?

OmegaKV
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My textbook says that for a central force at the origin, the angular momentum is constant, because the derivative rxF is zero since F points radially outwards so it is in the same direction as r. Ok, but what about the angular momentum about a point other than the origin, or the angular momentum with respect to the origin of a central force that is not located at the origin? Would angular momentum still conserved in these cases?
 
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What would it mean if angular momentum were not conserved in those cases?

Can you do the maths to see what would happen?
 
Of course then you have to relate the angular momentum to the new point of rotational symmetry. So you have to define
$$\vec{J}=(\vec{r}-\vec{r}_0) \times \vec{p},$$
if ##\vec{r}_0## is the position vector of the point around which the situation is rotatinal symmetric (isotropic). It's very obvious in view of Noether's theorem.
 
OmegaKV said:
Angular momentum with respect to the origin of a central force that is not located at the origin?
Momentum is conserved in a closed or isolated system. If there is a central force not located at the origin, then from the frame of the origin, that force must be exerting a torque on something with respect to the origin, and would need to be taken into account.
 

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