Textbook: Max Born, Principles of optics: Electromagnetic theory of propagation, interference and diffraction of light
Optics(Max Born, CUP, 1999)
Ch1 Basic Properties of the Electromagnetic Field
The electromagnetic field.
The wave equation and the velocity of light:
When j=0,ρ=0 and the medium is homogeneous, we have ∇2E−c2εμE¨=0,∇2H−c2εμH¨=0. The “velocity” can be determined as v=εμc by comparing ∇2V−v21∂t2∂2V=0.
Note this holds only for plane waves. Thus v=εμc should better be conceived as a “characteristic velocity of propagation”.
The law of refraction: sinθ2sinθ1=v2v1=:n12(refractive index). An absolute refractive indexn:=vc then satisfies n12=n1n2.
Equivalent to that the wave-front is continuous, or the intersection of the incident and refracted wave moves at a same speed on both sides of the boundary, v1=v′sinθ1,v2=v′sinθ2.
Maxwell’s formula: n=εμ. In fact μ is close to unity for most of nonmagnetic substances.
Scalar waves: Solving ∇2V−v21∂t2∂2V=0.
Plane waves: V=V(r⋅s,t) where r=r(x,y,z) is a position vector and s=s(sx,sy,sz) is a unit vector in a fixed direction. The term “plane wave” is due to that V holds constant over planes r⋅s=const which are perpendicular to s. We may take ζ=r⋅s and find ∇2V=∂ζ2∂2V, simplifying the equation to ∂(ζ−vt)∂(ζ+vt)∂2V=0. The general solution is V=V1(ζ−vt)+V2(ζ+vt). V1 holds constant for (ζ,t)→(ζ+vτ,t+τ). Therefore it represents a disturbance propagated with v in the +ζ direction. Likewise V2 -> −ζ direction.