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A plane electromagnetic wave-varies sinu...

A plane electromagnetic wave-varies sinusoidally at 900 MHz as it travels along the positive X Direction. The peak value of the electric field is `2mv//m` and is directed`pm`direction. The average power per unit area perpendicular to the direction of propagation is

A

`2W//m^(2)`

B

`10W//m^(2)`

C

`2xx10^(-9)W//m^(2)`

D

`5.31xx10^(-9)W//m^(2)`

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The correct Answer is:
To solve the problem of finding the average power per unit area of a plane electromagnetic wave, we can follow these steps: ### Step 1: Identify the given parameters - Frequency \( f = 900 \, \text{MHz} = 900 \times 10^6 \, \text{Hz} \) - Peak value of the electric field \( E_0 = 2 \, \text{mV/m} = 2 \times 10^{-3} \, \text{V/m} \) ### Step 2: Calculate the speed of light The speed of light \( c \) is a constant: \[ c = 3 \times 10^8 \, \text{m/s} \] ### Step 3: Calculate the peak value of the magnetic field \( B_0 \) Using the relationship between the electric field and magnetic field in an electromagnetic wave: \[ B_0 = \frac{E_0}{c} \] Substituting the values: \[ B_0 = \frac{2 \times 10^{-3}}{3 \times 10^8} \] \[ B_0 = \frac{2}{3} \times 10^{-11} \, \text{T} \] ### Step 4: Calculate the energy density \( u \) of the electromagnetic wave The energy density \( u \) is given by the sum of the electric and magnetic energy densities: \[ u = \frac{1}{2} \epsilon_0 E^2 + \frac{1}{2} \frac{B^2}{\mu_0} \] Since \( \frac{E^2}{c^2} = B^2 \), we can simplify this to: \[ u = \epsilon_0 E^2 \] Where \( \epsilon_0 \) (the permittivity of free space) is approximately: \[ \epsilon_0 = 8.85 \times 10^{-12} \, \text{F/m} \] Now substituting the values: \[ u = \epsilon_0 E_0^2 \] \[ u = 8.85 \times 10^{-12} \times (2 \times 10^{-3})^2 \] \[ u = 8.85 \times 10^{-12} \times 4 \times 10^{-6} \] \[ u = 35.4 \times 10^{-18} \, \text{J/m}^3 \] ### Step 5: Calculate the average power per unit area \( S \) The average power per unit area \( S \) is given by: \[ S = u \cdot c \] Substituting the values: \[ S = 35.4 \times 10^{-18} \times 3 \times 10^8 \] \[ S = 106.2 \times 10^{-10} \] \[ S = 1.062 \times 10^{-9} \, \text{W/m}^2 \] ### Final Answer The average power per unit area perpendicular to the direction of propagation is: \[ S \approx 1.06 \times 10^{-9} \, \text{W/m}^2 \] ---
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