Question 705058

SCQMEDIUM

A radio station antenna on the earth's surface radiates 50 kW power isotropically. Assume the electromagnetic waves to be sinusoidal and the ground to be a perfect absorber. Neglecting any transmission loss and effects of earth's curvature, the peak value of the magnetic field (in Tesla) detected at a distance of 100 km is closest to

(A)

1.5×10−111.5 \times 10^{-11}

(B)

5.5×10−115.5 \times 10^{-11}

(C)

3.85×10−113.85 \times 10^{-11}

(D)

3.5×10−113.5 \times 10^{-11}

Detailed Solution

1. Identify the Given Parameters

  • Power radiated isotropically, P=50 kW=50×103 WP = 50 \text{ kW} = 50 \times 10^3 \text{ W}
  • Distance from the antenna, R=100 km=100×103 m=105 mR = 100 \text{ km} = 100 \times 10^3 \text{ m} = 10^5 \text{ m}
  • Speed of light, c=3×108 m/sc = 3 \times 10^8 \text{ m/s}
  • Permeability of free space, μ0=4π×10−7 Tâ‹…m/A\mu_0 = 4\pi \times 10^{-7} \text{ T}\cdot\text{m/A}

2. Calculate the Intensity (II) of the Wave The problem states the antenna radiates "isotropically" (equally in all directions). Furthermore, the ground is a "perfect absorber." Because the ground does not reflect any waves, there is no reflected energy to interfere with or add to the direct wave. Therefore, the intensity at distance RR is identical to what it would be in free space. The energy is spread over a full spherical area 4Ï€R24\pi R^2. I=P4Ï€R2I = \frac{P}{4\pi R^2}

I=50×1034π(105)2I = \frac{50 \times 10^3}{4\pi (10^5)^2}

I=50×1034π×1010=504π×10−7 W/m2I = \frac{50 \times 10^3}{4\pi \times 10^{10}} = \frac{50}{4\pi} \times 10^{-7} \text{ W/m}^2

3. Relate Intensity to Peak Magnetic Field (B0B_0) The average intensity of a sinusoidal electromagnetic wave is related to its peak magnetic field by the standard formula: I=cB022μ0I = \frac{c B_0^2}{2\mu_0}

Rearranging this formula to solve for the peak magnetic field B0B_0: B02=2μ0IcB_0^2 = \frac{2\mu_0 I}{c}

4. Execute the Calculation Substitute the expression for II into the equation for B02B_0^2:

B02=2μ0c(P4πR2)B_0^2 = \frac{2\mu_0}{c} \left( \frac{P}{4\pi R^2} \right)

B02=2(4π×10−7)3×108(50×1034π×1010)B_0^2 = \frac{2 (4\pi \times 10^{-7})}{3 \times 10^8} \left( \frac{50 \times 10^3}{4\pi \times 10^{10}} \right)

Cancel 4Ï€4\pi from the numerator and denominator:

B02=2×10−7×50×1033×108×1010B_0^2 = \frac{2 \times 10^{-7} \times 50 \times 10^3}{3 \times 10^8 \times 10^{10}}

B02=100×10−43×1018B_0^2 = \frac{100 \times 10^{-4}}{3 \times 10^{18}}

B02=10−23×1018B_0^2 = \frac{10^{-2}}{3 \times 10^{18}}

B02=13×10−20B_0^2 = \frac{1}{3} \times 10^{-20}

Now, take the square root to find B0B_0:

B0=13×10−20B_0 = \sqrt{\frac{1}{3} \times 10^{-20}}

B0=13×10−10B_0 = \frac{1}{\sqrt{3}} \times 10^{-10}

B0≈0.577×10−10 TB_0 \approx 0.577 \times 10^{-10} \text{ T}

B0≈5.77×10−11 TB_0 \approx 5.77 \times 10^{-11} \text{ T}

5. Conclusion The calculated peak magnetic field is approximately 5.77×10−11 T5.77 \times 10^{-11} \text{ T}. Looking at the given options, this value is closest to 5.5×10−115.5 \times 10^{-11}.

Correct Option: 2

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