From the previous post "Loss, So What",
Uloss=12[εoE2cos2(θ){1−(εaεo)2}+μoB2sin2(θ){1−(μoμa)2}]
When the point is very sharp, θ→0, sin(θ)=0 and all the loss is wholly due to E. When the point flatten, θ→90o, cos(θ)=0 and all the loss is due to B.
Consider,
∂Uloss∂θ=12[−εoE22cos(θ)sin(θ){1−(εaεo)2}+μoB22cos(θ)sin(θ){1−(μoμa)2}]
∂Uloss∂θ=cos(θ)sin(θ)[μoB2{1−(μoμa)2}−εoE2{1−(εaεo)2}]
=12sin(2θ)[μoB2{1−(μoμa)2}−εoE2{1−(εaεo)2}]
∂2Uloss∂θ2=cos(2θ)[μoB2{1−(μoμa)2}−εoE2{1−(εaεo)2}]
∂2Uloss∂θ2>0 when θ=0o, this implies a sharp point has minimum loss and is mainly due to E.
∂2Uloss∂θ2<0 when θ=90o, this implies a flat surface has maximum loss and is mainly due to B.
Note: For material μaμo>>1 and εaεo>>1.
So, So What?