358899
The elecric field part of an electromagnetic wave in a medium is represented by \(E_{X}=0\);
\({E_y} = 2.5\frac{N}{C}\cos \left[ {\left( {2\pi \times {{10}^6}\frac{{rad}}{m}} \right)t} \right.\)
\(\left. { - \left( {\pi \times {{10}^{ - 2}}\frac{{rad}}{s}} \right)x} \right];\quad {E_z} = 0.{\rm{ The wave is }}\)
358899
The elecric field part of an electromagnetic wave in a medium is represented by \(E_{X}=0\);
\({E_y} = 2.5\frac{N}{C}\cos \left[ {\left( {2\pi \times {{10}^6}\frac{{rad}}{m}} \right)t} \right.\)
\(\left. { - \left( {\pi \times {{10}^{ - 2}}\frac{{rad}}{s}} \right)x} \right];\quad {E_z} = 0.{\rm{ The wave is }}\)
358899
The elecric field part of an electromagnetic wave in a medium is represented by \(E_{X}=0\);
\({E_y} = 2.5\frac{N}{C}\cos \left[ {\left( {2\pi \times {{10}^6}\frac{{rad}}{m}} \right)t} \right.\)
\(\left. { - \left( {\pi \times {{10}^{ - 2}}\frac{{rad}}{s}} \right)x} \right];\quad {E_z} = 0.{\rm{ The wave is }}\)
358899
The elecric field part of an electromagnetic wave in a medium is represented by \(E_{X}=0\);
\({E_y} = 2.5\frac{N}{C}\cos \left[ {\left( {2\pi \times {{10}^6}\frac{{rad}}{m}} \right)t} \right.\)
\(\left. { - \left( {\pi \times {{10}^{ - 2}}\frac{{rad}}{s}} \right)x} \right];\quad {E_z} = 0.{\rm{ The wave is }}\)