To determine the intensity of the plane electromagnetic wave described by \( E_y = (200 \, \text{V/m}) \sin(1.5 \times 10^7 t - 0.05 x) \), we need to use the formula for the intensity of an electromagnetic wave:
The intensity \( I \) of an electromagnetic wave is given by the formula:
\(I = \frac{1}{2} \varepsilon_0 c E_0^2\)
Where:
Substituting these values into the formula, we get:
\(I = \frac{1}{2} \times 8.85 \times 10^{-12} \, \text{F/m} \times 3 \times 10^8 \, \text{m/s} \times (200 \, \text{V/m})^2\)
Calculating step-by-step:
\(I = \frac{1}{2} \times 2.655 \times 10^{-3} \times 40000\)
\(I = 1.3275 \times 10^{-3} \times 40000\)
\(I = 53.1 \, \text{W/m}^2\)
This matches the option 53.1 W/m², confirming it as the correct answer.
The intensity \(I\) of an electromagnetic wave is given by:
\[ I = \frac{1}{2} \epsilon_0 c E_0^2 \]
where \(\epsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2/\text{N m}^2\), \(c = 3 \times 10^8 \, \text{m/s}\), and \(E_0 = 200 \, \text{V/m}\).
Substituting the values:
\[ I = \frac{1}{2} \times 8.85 \times 10^{-12} \times (3 \times 10^8) \times (200)^2 \] \[ I = 53.1 \, \text{W/m}^2 \]
Match the LIST-I with LIST-II:
| List-I | List-II | ||
| A. | Radio-wave | I. | is produced by Magnetron valve |
| B. | Micro-wave | II. | due to change in the vibrational modes of atoms |
| C. | Infrared-wave | III. | due to inner shell electrons moving from higher energy level to lower energy level |
| D. | X-ray | IV. | due to rapid acceleration of electrons |
Choose the correct answer from the options given below:

In the following \(p\text{–}V\) diagram, the equation of state along the curved path is given by \[ (V-2)^2 = 4ap, \] where \(a\) is a constant. The total work done in the closed path is: 