Expression of the force derived from this potential

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SUMMARY

The discussion focuses on calculating the force derived from a potential function in a field, specifically using the equation $$\vec{F}=-q\nabla U$$. The gradient $$\nabla U$$ must be calculated in spherical coordinates, represented as $$\nabla U=\frac{\partial U}{\partial r}\hat r+\frac{1}{r}\frac{\partial U}{\partial \theta}\hat\theta+\frac{1}{r\sin\theta}\frac{\partial U}{\partial \phi}\hat\phi$$. In this case, since the potential function $$U(r,\theta,\phi)$$ does not depend on $$\theta$$ and $$\phi$$, the gradient simplifies significantly. This provides a clear guideline for deriving the force from the potential energy function.

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Andrei0408
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Homework Statement
Knowing that the potential is U = - α / r , where α is a positive constant and r the distance from the
potential field source, find the expression of the force deriving from this potential; Give examples of forces that derive from such a potential.
Relevant Equations
Not sure
I just don't know what equations I should use, or what exactly I need to do. I just need some guidelines, thank you!
 
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It is a well known fact that given the potential function ##U(r,\theta,\phi)## of a field , the force that the field applies to a test point charge (or test point mass or whatever is the field subject)## q## is given by $$\vec{F}=-q\nabla U$$.

So all you have to do is calculate the gradient ##\nabla U## of the function ##U##. I assume from the context that the calculation must be done in spherical coordinates. So it will be $$\nabla U=\frac{\partial U}{\partial r}\hat r+\frac{1}{r}\frac{\partial U}{\partial \theta}\hat\theta+\frac{1}{r\sin\theta}\frac{\partial U}{\partial \phi}\hat\phi$$

Also note that in your case the function U does not depend on ##\theta## and ##\phi## so the above formula for the gradient of U simplifies a lot.
 
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