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Potential, A General Definition of Potential Energy 📂Mathematical Physics

Potential, A General Definition of Potential Energy

Definition1

Scalar Potential

Let’s assume that the vector field V\mathbf{V} is a conservative field. In other words, let’s say ×V=0\nabla \times \mathbf{V} = \mathbf{0}. Then, there exists a scalar field WW that satisfies V=W\mathbf{V} = -\nabla W, and this is called the scalar potential of V\mathbf{V}.

Vector Potential

Assume the vector field V\mathbf{V} satisfies V=0\nabla \cdot \mathbf{V} = 0. Then, there exists a vector field A\mathbf{A} that satisfies V=×A\mathbf{V} = \nabla \times \mathbf{A}, and this is called the vector potential of V\mathbf{V}.

Description

The scalar potential is simply referred to as potential.

If the unit of vector field V\mathbf{V} is force, it is specifically called potential energy.

Mechanics

Potential Energy

In one dimension, the potential energy of the force FF is defined as VV that satisfies:

F(x)=dV(x)dx F(x) = -\dfrac{d V(x)}{d x}

This is just a simple reduction of the above definition from three to one dimension. Also, since FF is a force, VV is referred to as potential energy.

Electromagnetism

Electric Potential

For an electric field E\mathbf{E}, the scalar field VV that satisfies the following is called electric potential:

E=V \mathbf{E} = - \nabla V

The electric force experienced by a test charge with a charge QQ is given by Coulomb’s law as F=QE\mathbf{F} = Q \mathbf{E}. Therefore, since the unit of the electric field is not force, the electric potential is not referred to as potential energy.

Magnetic Potential

For a magnetic field B\mathbf{B}, the vector field A\mathbf{A} that satisfies the following is called magnetic potential:

B=×A \mathbf{B} = \nabla \times \mathbf{A}

Similarly, since the magnetic force is given as Fm=Q(v×B)\mathbf{F}_{m} = Q (\mathbf{v} \times \mathbf{B}) by the Lorentz force law, the unit of B\mathbf{B} is not force, therefore magnetic potential is not referred to as potential energy.


  1. Mary L. Boas, Mathematical Methods in the Physical Sciences (3rd Edition, 2008), p338-339 ↩︎