PhysLean Documentation

PhysLean.Electromagnetism.PointParticle.ThreeDimension

Electrostatics of a stationary point particle in 3d #

i. Overview #

In this module we give the electromagnetic properties of a point particle sitting at the origin in 3d space.

ii. Key results #

iii. Table of contents #

iv. References #

A. The current density #

The current density of a point particle in 3d space is given by:

$$J(r) = (c q \delta(r - r₀), 0, 0, 0) $$

where $c$ is the speed light, $q$ is the charge of the particle and $r₀$ is the position of the particle in 3d space.

The current density of a point particle stationary at a point r₀ of 3d space.

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    A.1. The charge density #

    The charge density of a point particle in 3d space is given by: $$ρ(r) = q \delta(r - r₀) $$

    where $q$ is the charge of the particle and $r₀$ is the position of the particle in 3d space.

    A.2. The 3-current density #

    The 3-current density of a point particle in 3d space is given by: $$\vec J(r) = 0.$$

    In other words, there is no current flow for a point particle at rest.

    B. The Potentials #

    B.1. The electromagnetic potential #

    The 4-potential of a point particle in 3d space is given by:

    $$A(r) = \frac{q μ₀ c}{4 π |r - r₀|} (1, 0, 0, 0) $$

    where $μ₀$ is the permeability of free space, $c$ is the speed of light, $q$ is the charge of the particle and $r₀$ is the position of the particle in 3d space.

    The electromagnetic potential of a point particle stationary at r₀ of 3d space.

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      B.2. The scalar potential #

      The first component of the 4-potential is the scalar potential, once one has taken account of factors of the speed of light. It is given by:

      $$V(r) = \frac{q}{4 π \epsilon_0 |r - r_0|}.$$

      B.3. The vector potential is zero #

      The spatial components of the 4-potential give the vector potential, which is zero for a stationary point particle.

      $$\vec A(r) = 0.$$

      C. The electric field #

      The electric field of a point particle in 3d space is given by: $$\vec E(r) = \frac{q}{4 π \epsilon_0} \frac{\vec r - \vec r₀}{|\vec r - \vec r₀|^3}.$$

      C.1. the time derivative of the electric field #

      D. The magnetic field #

      Given that the vector potential is zero, the magnetic field is also zero.

      E. Maxwell's equations #

      The divergence of the electric field of a point particle in 3d space is given by: $$∇ · \vec E(r) = \frac{1}{\epsilon_0} q \delta(r - r₀).$$

      From this, it follows that the electromagnetic potential of a point particle in 3d space satisfies Maxwell's equations for a point particle at rest.