Maxwell's equations

Maxwell's equations are partial differential equations that state the relationships between electric and magnetic fields. They underlie the wave nature of light. Equation (1) and (2) are Gauss' laws, (3) Faraday's law of induction, (4) Ampere's circuital law.

The four equations were originally formulated based on observations. Equation 3, for example, comes from Faraday's law. It relates the rate at which magnetic field is changing, [math]\frac{\partial\mathbf{B}}{\partial t}[/math] to circular flow of electric current, [math]\nabla\boldsymbol{\times}\mathbf{E}[/math].

Maxwell's genius was in completing the four equations and from the combination conjecturing that light and radio waves were electromagnetic phenomenon. In particular, the speed at which light travels can be deduced from the equations.

Prerequisities

The maths of these equations will make no sense to you whatsoever without the following foundations:

• Understanding of Simple harmonic motion. The key idea is that differential equations relating position, velocity and acceleration can lead to a solution that oscillates.
• Familiarity with vectors in 3 dimensions, Vector product and Cross product. The vector product allows you to calculate the angle between two vectors. The cross product, given two vectors, finds another vector that is perpendicular to both.
• The Div Grad and Curl differential operations in 3D that are shown here, and in particular why [math]\nabla\cdot(\nabla\times\mathbf{B}) = 0[/math]. Div, Grad and Curl are differential operations in 3D space. Maxwell's 3rd and 4th equation relate the results of a spatial derivative of one field (magnetic or electric) with a temporal derivative of the other kind of field.

No Magnetic Monopoles

To-Be-Written.

Integral Version

The four differential equations are equivalent to these four integral equations. If you differentiate these integral equations, you get the differential ones.

[math] \begin{align} \oint_{\scriptstyle\partial \Omega } & \mathbf{E}\cdot\mathrm{d}\mathbf{S} = 4 \pi \iiint_\Omega \rho_e \,\mathrm{d}V\tag{1} \end{align} [/math]

[math] \begin{align} \oint_{\scriptstyle \partial \Omega } & \mathbf{B}\cdot\mathrm{d}\mathbf{S} = 4 \pi \iiint_\Omega \rho_m \,\mathrm{d}V\tag{2} \end{align} [/math]

[math] \begin{align} - \oint_{\partial \Sigma} & \mathbf{E} \cdot \mathrm{d}\boldsymbol{l} = \frac{1}{c} \left(\frac{\mathrm{d}}{\mathrm{d}t} \iint_{\Sigma} \mathbf{B} \cdot \mathrm{d}\mathbf{S} + 4 \pi \iint_{\Sigma} \mathbf{J_m} \cdot \mathrm{d}\mathbf{S} \right) \tag{3}\\ \end{align} [/math]

[math] \begin{align} \oint_{\partial \Sigma} & \mathbf{B} \cdot \mathrm{d}\boldsymbol{l} = \frac{1}{c} \left(\frac{\mathrm{d}}{\mathrm{d}t} \iint_{\Sigma} \mathbf{E} \cdot \mathrm{d}\mathbf{S} + 4 \pi \iint_{\Sigma} \mathbf{J_e} \cdot \mathrm{d}\mathbf{S} \right) \tag{4}\\ \end{align} [/math]

In equation (1) you consider any volume of space, [math]\Omega[/math]. The right hand side is a spatial integral, integrating all charge in that [math]\rho_e[/math] in that volume. [math]\scriptstyle \partial \Omega[/math] represents the surface of that volume. The left hand side is a surface integral, over the surface of [math]\Omega[/math], of electric field. The dot product inside the integral is measuring how much electric field crosses the surface.

Equation (2) is the same thing for magnetic field and 'magnetic charge'. As [math]\rho_m[/math] is zero everywhere, the right hand side evaluates to zero.

In equation (4) you consider a 'loop' in space that is the edge of some surface [math]\Sigma[/math]. [math]\Sigma[/math] is the surface itself. [math]\scriptstyle \partial \Sigma[/math] is its edge, the loop. The left hand side with its dot product is measuring the magnetic field around the loop. The right hand side is measuring the change in electric field through the surface, and the electric current (electric current density integrated over the surface [math]\Sigma[/math]).

Equation (3) does the same thing for electric field around the loop and magnetic field crossing the surface, and as [math]J_m = 0[/math] the 'magnetic current' term disappears.

The equivalence of the integral and differential forms of the equations follows from Stoke's Theorem and Green's Theorem.

To Dig Deeper

To dig deeper: Caches-to-Caches - A nuanced description of Maxwell's equations that aim to make the physics more understandable. The use of the more symmetric version of the equations is inspired by that article.

To dig deeper: Wikipedia - As ever Wikipedia aims to be encyclopedic, making the subject matter more than a bit impenetrable.