Step 1: Given, the conductivity \( \sigma = 58 \times 10^6 S/m \), relative permeability \( \mu_r = 1 \), and frequency \( f = 100 \times 10^6 Hz \).
Step 2: First calculate angular frequency \(\omega\): \[ \omega = 2\pi f = 2\pi \times 100 \times 10^6 = 2\pi \times 10^8 rad/sec \]
Step 3: Calculate the propagation constant \( \gamma = \alpha + j\beta \), using the given values of the medium. \[ \gamma = \sqrt{j\omega\mu (\sigma + j\omega \epsilon)} \] Since conductivity is high, we can neglect the \(\omega\epsilon\) term, so the equation becomes: \[ \gamma = \sqrt{j\omega\mu \sigma} = \sqrt{j(2\pi \times 10^8) \times (4\pi \times 10^{-7} ) \times (58 \times 10^6)} = \sqrt{j \times 460224 \times 10^7} \] \[ \gamma = \sqrt{460224 \times 10^7} \sqrt{j} = 214526 \times 10^2 \times e^{j45^\circ} = 2.145 \times 10^5 \angle 45^\circ m^{-1} \] Therefore, \( \gamma = 2.14 \times 10^5 { angle } 45^\circ { m}^{-1} \).
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: