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:
The potential energy for a configuration of point charges is given by:
U = ∑i<j \(\frac{K q_i q_j}{r_{ij}}\),
The distance between charges \( i \) and \( j \) is \( r_{ij} \).
Configuration (1): The charges are placed at the corners of the square. The distance between each pair of adjacent charges is \( a \), and the distance between diagonally opposite charges is \( \sqrt{2}a \).
Configuration (2): The charges are placed at the midpoints of the sides, so the distance between adjacent charges is \( \frac{a}{\sqrt{2}} \), and the distance between diagonally opposite charges is \( a \).
The potential energy of configuration (1) is:
\( U_1 = 4 \times \frac{K q_0^2}{a} + 2 \times \frac{K q_0^2}{\sqrt{2}a} \).
The potential energy of configuration (2) is:
\( U_2 = 4 \times \frac{K q_0^2}{\frac{a}{\sqrt{2}}} + 2 \times \frac{K q_0^2}{a} \).
The difference between the potential energies of configuration (2) and (1) gives the desired result:
\( \Delta U = U_2 - U_1 = \frac{K q_0^2}{a} (4\sqrt{2} - 2) \).
Final Answer: \( \frac{K q_0^2}{a} (4\sqrt{2} - 2) \).
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 \( 1.6 \times 10^{-27} \, \text{kg} \)).
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:
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: