Correct Answer - Option 1 : (A) and (C) only
Concept:
Total loss per unit area of the conductor surface:
\(W = \mathop \smallint \nolimits_0^\infty σ E_0^2{e^{ - 2\alpha z}}dz\)
Since σE2 = energy density (W/m3)
E = E0e-αz
\(W = \frac{{σ \;{{\left| {{E_0}} \right|}^2}}}{{2\alpha }}\)
Calculation:
Given:
f = 2 GHz
σ =107 ℧/m
\(\alpha = \sqrt {\frac{{\omega \mu \sigma }}{2}} = \sqrt {\frac{{2\pi f \times \mu \sigma }}{2}} \)
\(\alpha = \sqrt {\frac{{2\pi \times 2 \times {{10}^9} \times 4\pi \times {{10}^{ - 7}} \times {{10}^7}}}{2}} \)
α = 280992.5892
\(W = \frac{{\sigma \;{{\left| {{E_0}} \right|}^2}}}{{2\alpha }}\)
\(3 \times {10^{ - 6}} = \frac{{{{10}^7}{{\left| {{E_0}} \right|}^2}}}{{2\alpha }}\)
|E0| = 4.106 × 10-4 V/m
|H
0| = 1.089 × 10
-6 A/m