Due to presence of an em-wave whose electric component is given by \( E = 100 \sin(\omega t - kx) \, NC^{-1} \), a cylinder of length 200 cm holds certain amount of em-energy inside it. If another cylinder of same length but half diameter than previous one holds same amount of em-energy, the magnitude of the electric field of the corresponding em-wave should be modified as:
\( 200 \sin(\omega t - kx) \, NC^{-1} \)
\( 25 \sin(\omega t - kx) \, NC^{-1} \)
\( 50 \sin(\omega t - kx) \, NC^{-1} \)
\( 400 \sin(\omega t - kx) \, NC^{-1} \)
The energy of an electromagnetic wave is proportional to the square of the electric field \( E \), and the energy density is given by: \[ U = \frac{\epsilon_0 E^2}{2} \]
Step 1: Since both cylinders contain the same amount of energy, we have: \[ U_1 = U_2 \]
Step 2: The energy is proportional to the square of the electric field: \[ E_1^2 \propto E_2^2 \] For the second cylinder, the diameter is half, which reduces the area by a factor of 4.
Step 3: Therefore, the electric field should decrease by a factor of 2 to compensate for the reduced area.
Step 4: Thus, the new electric field will be \( \frac{1}{2} \) of the original, making the new electric field: \[ E_2 = 50 \sin(\omega t - kx) \, NC^{-1} \]
Final Conclusion: The modified electric field is \( 50 \sin(\omega t - kx) \, NC^{-1} \), which corresponds to Option (3).
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by:
In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: