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Question: The electric fields part of an electromagnetic wave in a medium is represented by \(E_{x} = 0,\) \(...

The electric fields part of an electromagnetic wave in a medium is represented by Ex=0,E_{x} = 0,

Ey=2.5NCcos[(2π×106radm)t(π×102rads)x]Ez=0,TheE_{y} = 2.5\frac{N}{C}\cos\left\lbrack \left( 2\pi \times 10^{6}\frac{rad}{m} \right)t - \left( \pi \times 10^{- 2}\frac{rad}{s} \right)x \right\rbrack E_{z} = 0,Thewave is

A

Moving along x direction with frequency 10610^{6}Hz and wavelength 100 m

B

Moving along x direction with frequency 10610^{6}Hz and wavelength 200m

C

Moving along -x direction with frequency 10610^{6}Hz and wavelength 200m

D

Moving along y direction with frequency 2π×1062\pi \times 10^{6}Hz and wavelength 200m

Answer

Moving along x direction with frequency 10610^{6}Hz and wavelength 200m

Explanation

Solution

: Ey=2.5NC×cos[(2π×106radm)t(π×102rads)x]E_{y} = 2.5\frac{N}{C} \times \cos\left\lbrack \left( 2\pi \times 10^{6}\frac{rad}{m} \right)t - \left( \pi \times 10^{- 2}\frac{rad}{s} \right)x \right\rbrack

Ez=0,Ex=0E_{z} = 0,E_{x} = 0

The wave is moving in the positive direction of x. This is in the form Ey=E0(ωtkx)E_{y} = E_{0}(\omega t - kx)

ω=2π×106\omega = 2\pi \times 10^{6}

2πυ=2π×106υ=106Hz2\pi\upsilon = 2\pi \times 10^{6} \Rightarrow \upsilon = 10^{6}Hz

λ=2ππ×102=2×102=200m\Rightarrow \lambda = \frac{2\pi}{\pi \times 10^{- 2}} = 2 \times 10^{2} = 200m