Wikipedia comments: "Maxwell's equations are a set of partial differential equations that, together with the Lorentz force law, form the foundation of classical electrodynamics, classical optics, and electric circuits. These fields in turn underlie modern electrical and communications technologies. Maxwell's equations describe how electric and magnetic fields are generated and altered by each other and by charges and currents. They are named after the Scottish physicist and mathematician James Clerk Maxwell who published an early form of those equations between 1861 and 1862."

Differential form in a vacuum:

I. Gauss' law
for electricity

∇ ⋅ E = 0

II. Gauss'
law for magnetism

∇ ⋅ B = 0

III. Faraday's law of induction

∇ x E = -

∂B/∂t

IV. Ampere's law

∇ x B = ε_{0}
μ_{0}i ∂E/∂t ∫ E ⋅ dA

Have a Maxwell's equation to solve? Or any other math equations? For the next few months of 2014, we are willing to help you solve them using Calculus-level programming. To start, copy and modify the source code below in a file we'll call it {abc}{123}.fc where {abc} = your initials and {123} = any number or id; 8 characters max. for filename. Edit your {abc}{123}.fc file, especially lines starting with a "!" character.
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User's Maxwell's Equation Source Code:

For 1-dimensional (1D) Maxwell's Equation:

global all
problem MaxwellsPDE
C ------------------------------------------------------------------------
C --- Calculus Programming example: Maxwell's 1D Equation; a PDE Initial
C --- Value Problem solved using Method of Lines.
C ------------------------------------------------------------------------
dynamic U, Ut, Ut0
C
C User parameters ...
e0 = 8.854187817e-12 ! F/m or A^{2 }s^{4} kg^{-1}m^{−3} permittivity of free space
pi = 4*atan(1)
u0 = 4*pi*e-7 ! N·A^{−2} ... permeability of free space
! ipoints = 101 ! grid pts. over x-axis
! tFinal = 1 ! final time
C
C x-parameter initial settings: x ==> i
! xFinal = 1: ip = ipoints: dx= xFinal/(ipoints-1)
C
C t-parameter initial settings: t ==> m
pi = 4*atan(1): tPrint = tFinal/20
allot U(ip), Ut(ip), Ut0(ip)
C
call tAxis !
end ! Stmt.s not necessary in IVP, but used in BVP versions
model tAxis !
C ... Integrate over t-axis
C
t= 0: tPrt = tPrint: dt = tPrt/10
Initiate janis; for PDE;
~ equations Ut/U; of t; step dt; to tPrt
do while (t .lt. tFinal)
Integrate PDE; by janis
if( t .ge. tPrt) then
print 79, t, (U(ij), ij = 1, ip)
tPrt = tPrt + tPrint
end if
end do
79 format( 1x, f8.4, 1x, 20(g14.5, 1x))
end
model PDE ! Partial Differential Equation
C ! Method of Lines
! U(1)=U0(x): Ux(1)=0: Uxx(1)=0 ! Initial Conditions
do 20 ij = 2, ipoints-1 ! System of ODEs
Ux = (U(ij)-U(ij-1))/dx ! approx. partial of U w.r.t. x
Uxx = (U(ij+1) - 2*U(ij) + U(ij-1))/dx**2
! Uxx(ij)= ... f(x, U(ij), Ux(ij), Ut)
! Ut = U
20 continue
end
Fmodel U0(xx) ! Initial starting values @ t = 0
! if( xx .lt. 0) then
! U0 = 0
! elseif( xx .lt. .5 ) then
! U0 = (1 - cos( 4 * pi * xx))/2
! else
! U0 = 0
! endif
end

User's Maxwell's Equation Output:

selected output goes here ...

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<a href="http://goal-driven.net/math-problems/maxwell-equation.html"><img style="float:left; width:100px" src="http://goal-driven.net/image/fc-compiler-icon.png"/> <strong>Maxwell's (Partial Differential) Equation</strong> </a>; Simulation to Optimization, Tweak Parameters for Optimal Solution.