Variations of electrostatic potential energy

In summary, the expression for the total electrostatic potential energy is given by \displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E} \cdot \textbf{E} \; dV over all space, which represents the work required to assemble the charge distribution that produces the electric field. For a system of two charge distributions, the total potential energy is equal to the self energy of each distribution plus the interaction energy between the two systems. The interaction energy can be calculated by substituting ##\vec{E} = -\vec{\nabla} \phi## into the integral. However, the self energy is usually ignored for point charges due to its infinite value.
  • #1
Poley
31
2
Hello,

(this isn't homework but I thought it wasn't worthy of the main forums)

I'm looking to clarify some thoughts about the various forms of electrostatic potential energy.

As I understand, the expression

[itex]\displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E} \cdot \textbf{E} \; dV[/itex]

over all space gives the total work required to assemble the charge distribution that produces the field [itex]\textbf{E}[/itex].

Two questions:

1. Suppose I have two charge distributions. Is the total potential energy of the system equal to the self energy of each distribution alone plus the interaction energy between the two systems? (are there other components of potential energy?)

2. How do you calculate the interaction energy of two charge distributions? I know how to do it for point charges ([itex]q_1 \phi_2[/itex] or [itex]q_2 \phi_1[/itex]).

Thoughts:

If distribution 1 has field [itex]\textbf{E}_1[/itex] and distribution 2 has field [itex]\textbf{E}_2[/itex], the TOTAL energy should be

[itex]\displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E}_1 \cdot \textbf{E}_1 + 2\textbf{E}_1 \cdot \textbf{E}_2 + \textbf{E}_2 \cdot \textbf{E}_2 \; dV[/itex].

Speculation: Is the first term the self energy of distribution 1, the second term the interaction energy, and the last term the self energy of distribution 2?

Is there any way to find expressions for the energies of charge distributions using potential?

Thank you very much!
 
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  • #2
Poley said:
[itex]\displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E} \cdot \textbf{E} \; dV[/itex]

over all space gives the total work required to assemble the charge distribution that produces the field [itex]\textbf{E}[/itex].

Two questions:

1. Suppose I have two charge distributions. Is the total potential energy of the system equal to the self energy of each distribution alone plus the interaction energy between the two systems?

Yes. However, for a system of point charges the self energy is usually ignored because it is a fixed quantity that doesn't depend on the relative positions of the charges and, moreover, it is infinite!
2. How do you calculate the interaction energy of two charge distributions? I know how to do it for point charges ([itex]q_1 \phi_2[/itex] or [itex]q_2 \phi_1[/itex]).

Thoughts:

If distribution 1 has field [itex]\textbf{E}_1[/itex] and distribution 2 has field [itex]\textbf{E}_2[/itex], the TOTAL energy should be

[itex]\displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E}_1 \cdot \textbf{E}_1 + 2\textbf{E}_1 \cdot \textbf{E}_2 + \textbf{E}_2 \cdot \textbf{E}_2 \; dV[/itex].

Speculation: Is the first term the self energy of distribution 1, the second term the interaction energy, and the last term the self energy of distribution 2?

Yes, that is correct. The "self energy of distribution 1" (represented by your first integral) would include the self energy of the particles making up distribution 1 as well as the interaction energy of the particles within distribution 1.
Is there any way to find expressions for the energies of charge distributions using potential?

You could substitute ##\vec{E} = -\vec{\nabla} \phi## into your integral [itex]\displaystyle \frac{\epsilon_{o}}{2} \int \textbf{E} \cdot \textbf{E} \; dV[/itex]
 
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  • #3
Thanks, TSny! Very helpful! I think I understand it now.
 

FAQ: Variations of electrostatic potential energy

What is electrostatic potential energy?

Electrostatic potential energy is the energy stored in a system due to the interactions between static electric charges. It is a type of potential energy that can be calculated using the equation U = kQq/r, where k is the Coulomb's constant, Q and q are the magnitudes of the charges, and r is the distance between them.

How does distance affect electrostatic potential energy?

The electrostatic potential energy between two charges is inversely proportional to the distance between them. This means that as the distance between the charges increases, the electrostatic potential energy decreases. Therefore, the closer two charges are to each other, the higher their electrostatic potential energy will be.

What is the relationship between electrostatic potential energy and work?

Electrostatic potential energy and work are closely related. Work is defined as the force applied over a distance, and in the case of electrostatic potential energy, the force is the electric force between two charges. Therefore, the work done in moving a charge from one point to another is equal to the change in electrostatic potential energy between those two points.

How does the charge of an object affect its electrostatic potential energy?

The charge of an object directly affects its electrostatic potential energy. The higher the charge of an object, the higher its electrostatic potential energy will be. This is because the electric force between two charges increases as their magnitudes increase, resulting in a higher potential energy.

Can electrostatic potential energy be negative?

Yes, electrostatic potential energy can be negative. This occurs when the charges have opposite signs, resulting in an attractive force between them. In this case, the work done in bringing the charges closer together will be negative, and so will the electrostatic potential energy between them.

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