Potential Energy and Conservative Force Question

AI Thread Summary
Potential energy is directly related to conservative forces, with the relationship given by F = -∇U, indicating that the force is derived from the potential energy function. The force represents the net conservative force acting on an object within the system, which can vary based on the object's position. In a multi-body system, such as three particles, the force on one particle is calculated by considering the potential energy contributions from the other particles while excluding the singularity of the particle in question. The force acts as a vector field representing the gravitational influence of the masses on an external object. Understanding this relationship clarifies how potential energy and forces interact in a given system.
e(ho0n3
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Hello everyone,

I'm a little confused on how potential energy is related to a conservative force. Say some system has potential energy U. There is a relation stating that
\vec{F} = \nabla U
I understand the F is some conservative force, but does it represent the net conservative force acting on the system or on an object within the system or what?

e(ho0n3
 
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e(ho0n3 said:
I'm a little confused on how potential energy is related to a conservative force. Say some system has potential energy U. There is a relation stating that
\vec{F} = \nabla U
That should be:
\vec{F} = - \nabla U
I understand the F is some conservative force, but does it represent the net conservative force acting on the system or on an object within the system or what?
That conservative force is the force associated with that potential energy. Given the potential energy function you can calculate the force as above. For example, gravitational PE between two masses is:
GPE = - G\frac{m_1m_2}{r}
thus the gravitational force associated with this potential energy is:
F = - G\frac{m_1m_2}{r^2}

Does this get at your question at all? If not, ask again.
 
Last edited:
Still Confused

Doc Al said:
That should be:
\vec{F} = - \nabla U

Right.

Doc Al said:
That conservative force is the force associated with that potential energy. Given the potential energy function you can calculate the force as above. For example, gravitational PE between two masses is:
GPE = - G\frac{m_1m_2}{r}
thus the gravitational force associated with this potential energy is:
F = - G\frac{m_1m_2}{r^2}

Does this get at your question at all? If not, ask again.

But where is F acting. I guess in this simple case, F can act on either one of the masses since it's all the same. Let me make a more concrete example. Suppose we have a system of three particles with potential energy
U = -G\Big(\frac{m_1m_2}{r_{12}} + \frac{m_1m_3}{r_{13}} + \frac{m_2m_3}{r_{23}}\Big)​
You can calculate the force associated with this potential energy, but what does the force represent?

e(ho0n3
 
To find the force on m3, for example, you start with the PE of m3. Don't include the m1m2 term.

Interesting question, though. There is probably a subtlety that I am missing.
 
But where is F acting.

THe potential is defined everywhere (except the singularities). The forces at any point that arise form a force field. So it depends on the point in which you want to know the energy and force (force changes with position).

does it represent the net conservative force acting on the system or on an object within the system or what?

the force at a certain point within the system (of an object)
 
If you start with the potential (not potential energy), then you can calculate the field at any point. In our 3 body gravity example, if we want to calculate the force on m3, we need to find the potential at m3. As remcook notes you must exclude m3 to avoid the singularity. Then you can calculate the field, then the force on m3.

Try it and you'll see that the methods are equivalent.
 
remcook said:
THe potential is defined everywhere (except the singularities). The forces at any point that arise form a force field. So it depends on the point in which you want to know the energy and force (force changes with position).

OK. So the force in the system I described is the net force that will act on an external object within the system given that this external object is not located where the masses are. In other words, F is a vector field correspoding to the force of gravity produced by the three masses.

Am I right?
e(ho0n3
 
looks about right. But the third mass (for which the force holds then) is attracted by only two other bodies.

So I would also like to say:
Don't include the m1m2 term.
 
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