Advanced Electromagnetics for ECE
Comprehensive test covering transmission lines, waveguides, antennas, Maxwell's equations, plane wave propagation, and electromagnetic wave properties for Electronics and Communication Engineering students
Questions
In a microwave test bench, why is the microwave signal amplitude modulated at 1 kHz?
- To increase the sensitivity of measurement
- To transmit the signal to a far-off place
- To study amplitude modulations
- Because crystal detector fails at microwave frequencies
Consider a 300 $\Omega$, quarter - wave long (at 1 GHz) transmission line as shown in figure. It is connected to a 10 V, 50 $\Omega$ source at one end and is left open circuited at the other end. The magnitude of the voltage at the open circuit end of the line is

- 10 V
- 5 V
- 60 V
- 60/7 V
If the electric field intensity is given by E = (xux + yuy + zuz) volt/m, the potential difference between X(20,0) and Y(1,2,3) is
- +1 volt
- -1 volt
- +5 volt
- +6 volt
A transmission line of characteristic impedance 50 Ω is terminated by a 50 Ωload.
When excited by a sinusoidal voltage source at 10 GHz, the phase difference between two points spaced 2 mm apart on the line is found to be $\dfrac{2\pi}{\lambda}$ radians. The phase velocity of the wave along the line is
- 0.8 x 108 m/s
- 1.2 x 108 m/s
- 1.6 x 108 m/s
- 3 x 108 m/s
A coaxial cable with an inner diameter of 1 mm and outer diameter of 2.4 mm if filled with a dielectric of relative permittivity 10.89. Given $\mu_0 = 4\pi\times10^{-7}$H/m, $\epsilon_0$= $\dfrac{10^-9}{36 \pi}$F/m, the characteristic impedance of the cable is
- 330 $\Omega$
- 100 $\Omega$
- 143.3 $\Omega$
- 43.4$\Omega$
A transmission line is feeding 1 Watt of power to a horn antenna having a gain of 10 dB. The antenna is matched to the transmission line. The total power radiated by the horn antenna into the free-space is
- 10 Watts
- 1 Watt
- 0.1 Watt
- 0.01 Watt
For static electric and magnetic fields in an inhomogeneous source-free medium, which of the following represents the correct form of Maxwell`s equations?
- $\nabla$. E = 0, $\nabla$ X B = 0
- $\nabla$. E = 0,$\nabla$. B = 0
- $\nabla$ X B = 0,$\nabla$ x B = 0
- $\nabla$ x E = 0,$\nabla$. B = 0
A uniform plane wave in the free space is normally incident on an infinitely thick dielectric slab (dielectric constant $\epsilon$= 9). The magnitude of the reflection coefficient is
- 0
- 0.3
- 0.5
- 0.8
The electric and magnetic fields for a TEM wave of frequency 14 GHz in a homogeneous medium of relative permittivity $\epsilon_r$ and relative permeability $\mu_r$ = 1 are given by
$\vec E = E_p e^{j(\omega t - 280\pi \gamma)} \widehat U_z V/m
\qquad
\vec H = 3 e^{j(\omega t - 280\pi \gamma)} \widehat U_x A/m
$
Assuming the speed of light in free space to be 3 x 108 m/s, the intrinsic impedance of free space to be 120$\pi$, the relative permittivity$\epsilon_r$of the medium and the electric field amplitude Ep are
- $\epsilon_r$= 3, Ep = 120
- $\epsilon_r$= 3, Ep = 360
- $\epsilon_r$= 9, Ep = 360
- $\epsilon_r$= 9, Ep = 120
A transmission line terminates in two branches, each of length $\dfrac{\lambda}{4}$, as shown.
The branches are terminated by 50 $\Omega$ loads. The lines are lossless and have the characteristic impedances shown. Determine the impedance Zi as seen by the source.

- 200 $\Omega$
- 100 $\Omega$
- 50 $\Omega$
- 25 $\Omega$
The radiation pattern of an antenna in spherical co - ordinates is given by
F ($\theta$) = cos4$\theta$; 0$\le$$\theta$$\le$$\pi$/2
The directivity of the antenna is
- 10 dB
- 12.6 dB
- 11.5 dB
- 18 dB
The parallel branches of a 2-wire transmission line are terminated in 100 $\Omega$ and 200 $\Omega$ resistors as shown in the figure. The characteristic impedance of the line is Z0 = 50 $\Omega$ and each section has a length of $\dfrac{\lambda}{4}$. The voltage reflection coefficient
at the input is

- - j $\dfrac{7}{5}$
- $\dfrac{-5}{7}$
- j$\dfrac{5}{7}$
- $\dfrac{5}{7}$
A uniform plane wave travelling in air is incident on the plane boundary between air and another dielectric medium with $\epsilon_r$= 4. The reflection coefficient for the normal incidence, is
- zero
- 0.5$\angle$180�
- 0.333$\angle$0�
- 0.333$\angle$180�
Which of the following statements is true regarding the fundamental mode of the metallic waveguides shown?

- Only P has no cutoff-frequency
- Only Q has no cutoff-frequency
- Only R has no cutoff-frequency
- All three have cutoff-frequencies
The depth of penetration of electromagnetic wave in a medium having conductivity $\sigma$ at a frequency of 1 MHz is 25 cm. The depth of penetration at a frequency of 4 MHz will be
- 6.25 cm
- 12.50 cm
- 50.00 cm
- 100.00 cm
The modes in a rectangular waveguide are denoted by where m and n are the eigen numbers along the larger and smaller dimensions of the waveguide respectively. Which one of the following statements is TRUE?
- The TM10 mode of the wave does not exist
- The TE10 mode of the wave does not exist
- The TM10 and the TE10 modes both exist and have the same cut-off frequencies
- The TM10 and TM01 modes both exist and have the same cut-off frequencies
Refractive index of glass is 1.5. Find the wavelength of a beam of light with a frequency of 1014 Hz in glass. Assume velocity of light is 3 × 108 m/s in vacuum.
- 3 $\mu$m
- 3 mm
- 2 $\mu$m
- 1 m
A plane wave of wavelength $\lambda$ is travelling in a direction making an angle 30° with positive x-axis and 90° with positive y-axis. The $\vec E$ field of the plane wave can be represented as (E0 is constant)
- $\vec E$ = $\widehat Y$ E0 ej $\left( \omega t + \dfrac{\pi}{\lambda}x \times \dfrac{\sqrt 3 \pi}{\gamma} z \right)$
- $\vec E$ = $\widehat Y$ E0 ej $\left( \omega t - \dfrac{\pi}{\lambda} \times \dfrac{\sqrt 3 \pi}{\gamma} z \right)$
- $\vec E$ = $\widehat Y$E0 ej $\left( \omega t + \dfrac{\sqrt 3 \pi}{\gamma} \times \dfrac{\pi}{\lambda} z \right)$
- $\vec E$ = $\widehat Y$ E0 ej $\left( \omega t - \dfrac{\pi}{\lambda} x + \dfrac{\sqrt 3 \pi}{\gamma} z \right)$
The magnetic field along the propagation direction inside a rectangular waveguide with the cross section shown in the figure is
Hz = 3 Cos(2.094 x 102x) cos(2.618 x 102 y) cos (6.283 x 1010 t -$\beta z$
The phase velocity Vp of the wave inside the wave guide satisfies
- vp > c
- vp = c
- o < vp < c
- vp = 0
A current sheet $\vec j$= 10$\widehat u_y$A/m lies on the dielectric interface x = 0 between two dielectric media with $\epsilon_{r1}$= 5, $\mu_{r1}$ = 1 in Region - 1 (x < 0) and $\epsilon_{r2}$ = 5, $\mu_{r2}$ = 2 in Region - 2 (x > 0). If the magnetic field in Region -1 at x = 0- is $\vec H_1$ = 3$\widehat u_x$+ 30$\widehat u_y$A /m the magnetic field in Region -2 at x = 0 + is
- $\vec H_2$ = 1.5$\widehat u_x$ + 30$\widehat u_y$ - 10$\widehat u_z$A/m
- $\vec H_2$ = 3$\widehat u_x$ + 30$\widehat u_y$ - 10$\widehat u_z$A/M
- $\vec H_2$ = 1.5$\widehat u_x$ + 40$\widehat u_y$A/M
- $\vec H_2$ = 3$\widehat u_x$ + 30$\widehat u_y$ + 10$\widehat u_z$A/M












