Basic equations in some matter are written by rotE(x,t)+∂t∂B(x,t)=0divB(x,t)=0∫−∞∞dωeiωtμ(ω)1[rotB~(x,ω)−v2(ω)iωE~(x
Posted: Thu Jul 14, 2022 2:11 pm
Please be careful to use basic conditions and equations toderive wave equations separately. Thank you.
Basic equations in some matter are written by rotE(x,t)+∂t∂B(x,t)=0divB(x,t)=0∫−∞∞dωeiωtμ(ω)1[rotB~(x,ω)−v2(ω)iωE~(x,ω)]=0 ∫−∞∞dωeiωtϵ(ω)divE~(x,ω)=0 where D(x,t)=∫−∞∞D~(x,ω)eiωt dω,E(x,t)=∫−∞∞E~(x,ω)eiωt dωD~(x,ω)=ϵ(ω)E~(x,ω).(B~(x,ω)=μ(ω)H~(x,ω) as well )
Using the potentials and the Lorenz gauge condition, E(x,t)=−∂t∂A′(x,t)−gradϕ′(x,t)B(x,t)=rotA′(x,t)divA~′(x,ω)+v2(ω)iωϕ~′(x,ω)=0 derive the wave equations for A~′(x,ω) and ϕ~′(x,ω).
Basic equations in some matter are written by rotE(x,t)+∂t∂B(x,t)=0divB(x,t)=0∫−∞∞dωeiωtμ(ω)1[rotB~(x,ω)−v2(ω)iωE~(x,ω)]=0 ∫−∞∞dωeiωtϵ(ω)divE~(x,ω)=0 where D(x,t)=∫−∞∞D~(x,ω)eiωt dω,E(x,t)=∫−∞∞E~(x,ω)eiωt dωD~(x,ω)=ϵ(ω)E~(x,ω).(B~(x,ω)=μ(ω)H~(x,ω) as well )
Using the potentials and the Lorenz gauge condition, E(x,t)=−∂t∂A′(x,t)−gradϕ′(x,t)B(x,t)=rotA′(x,t)divA~′(x,ω)+v2(ω)iωϕ~′(x,ω)=0 derive the wave equations for A~′(x,ω) and ϕ~′(x,ω).