Can a solid sphere only be considered a point for inverse-square forces?

AI Thread Summary
The discussion centers on whether a solid sphere can be treated as a point source for forces that are not of the inverse-square type. It is established that while the field inside a uniform spherical shell is zero for inverse-square forces, this does not apply to other force types, suggesting different symmetries may exist. Forces such as electric dipoles decay as \frac{1}{r^3}, while intermolecular forces like dipole-dipole and Van der Waals interactions can decay as \frac{1}{r^8}, raising questions about their spherical symmetry. The consensus indicates that treating a sphere as a point source may not hold without inverse-square decay, but could still be valid under certain conditions. Ultimately, the nature of the force and its symmetry significantly influence the treatment of the sphere in calculations.
cyborg6060
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I am curious as to whether the force of solid sphere can be considered to be originating entirely at its center when the force is not of \frac{1}{r^2} nature.

It is said that the field inside a uniform spherical shell is zero for any \frac{1}{r^2} type force and not for any others. It would seem likely that the other such conclusions would not hold for any force that was not proportional to the inverse square of the distance.

If so, are there any similar conclusions or symmetries that are independent of the type of decay of the force?
 
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If you have a force that is NOT proportional to the inverse of r^2 then your dealing with some sort of crazy scenario where energy or space is not symmetrical.

So you can't treat the sphere as a point without taking into consideration the modifications you have made to the system to make it non-symmetrical.
 
To my knowledge there existed a fair amount of forces that are not inverse-square in nature.

When electric dipoles are involved, for instance, the decay becomes one of \frac{1}{r^3}. Also, the macroscopic functions for intermolecular forces such as those due to dipole-dipole and Van der Waals attractions are usually proportional to \frac{1}{r^8}.

Would the proof for considering the force from solid sphere to be from its center (from outside the sphere) fall apart without the inverse-square force decay?
 
Actually as long as it proportional to r of any order than it should not fall apart. Because if each part of the sphere that you move further away you also move another part the same distance closer when treating the sphere as a point at the center.
 
cyborg6060 said:
To my knowledge there existed a fair amount of forces that are not inverse-square in nature.

When electric dipoles are involved, for instance, the decay becomes one of \frac{1}{r^3}. Also, the macroscopic functions for intermolecular forces such as those due to dipole-dipole and Van der Waals attractions are usually proportional to \frac{1}{r^8}.
But do those things have spherical symmetry?
 
uart said:
But do those things have spherical symmetry?

You raise a very good point. The dipole-dipole force falls off as \frac{1}{r^3} only along the plane equidistant between the two poles. Doh.

As far as the LDF intermolecular forces go, the attraction is entirely independent of direction and therefore spherically symmetrical.
 
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