derivation for attenuation constant and phase constant for propagation constant of plane wave in lossy media
i'd done some equating stuffs and got \[\alpha ^{2}-\beta^{2}+j2\alpha \beta=-w^{2}\mu \epsilon'+jw^{2}\mu \epsilon''\] now i just need to equate the real and imaginary parts which will be\[\alpha^{2}-\beta^{2}=-w^2 \mu \epsilon'\]and\[2 \alpha \beta=w^2 \mu \epsilon''\]
but i cant reach the final derived expression,\[\alpha=w \sqrt{\frac{\mu \epsilon'}{2}[\sqrt{1+(\frac{\epsilon''}{\epsilon'})^{2}}-1]}\]\[\beta=w \sqrt{\frac{\mu \epsilon'}{2}[\sqrt{1+(\frac{\epsilon''}{\epsilon'})^{2}}+1]}\]
its like after equating the real and imaginary parts, the alpha and beta cant be factorized ompltely
use wolframalpha and check
wolfrom allows so many unknowns?
it can
how to make it interpret correctly? i tried solve a^2-b^2+j(2ab)= -(omega)^2 (mu)(epsilon)+j(omega)^2(mu)(sigma/omega) but it doesnt return the answer i need
isolate b from 2ab = ... put it in a^2-b^2 = .... you will get something in b^2 and b^4 assume b^2 =x so you will get quadratic in x use quadratic formula to solve then plug back x = b^2 and take square root to find b (cumbersome process, but you should get that)
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