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, \( \gamma = 2.14 \times 10^5 { angle } 45^\circ { m}^{-1} \).
The Lagrangian of a particle of mass \( m \) and charge \( q \) moving in a uniform magnetic field of magnitude \( 2B \) that points in the \( z \)-direction, is given by: \[ L = \frac{m}{2} v^2 + qB(x v_y - y v_x) \] where \( v_x, v_y, v_z \) are the components of its velocity \( v \). If \( p_x, p_y, p_z \) denote the conjugate momenta in the \( x, y, z \)-directions and \( H \) is the Hamiltonian, which of the following option(s) is/are correct?
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:
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:
A closed-loop system has the characteristic equation given by: $ s^3 + k s^2 + (k+2) s + 3 = 0 $.
For the system to be stable, the value of $ k $ is:
A digital filter with impulse response $ h[n] = 2^n u[n] $ will have a transfer function with a region of convergence.