Test 4 - Electromagnetics | Electronics and Communication (ECE)
Topic wise test for Electronicmagnetics of Electronics and Communication (ECE)
Questions
If a vector field $\vec V$is related to another vector field $\vec A$through $\vec V$= $\nabla$x $\vec A$, which of the following is true? (Note : C and Sc refer to any closed contour and any surface whose boundary is C.)
- $\oint_0 \vec V. \vec{dl} = \int_z \int \vec A. \vec d S$
- $\oint_0 \vec A. \vec{dl} = \int_z \int \vec V. \vec d S$
- $\oint_0 \vec V. \vec{dl} = \int_z \int \Delta x \vec A. \vec d S$
- $\oint_0 \Delta x \vec V. \vec{dl} = \int_z \int \vec V. \vec d S$
A $\dfrac{\lambda}{2}$ dipole is kept horizontally at a height of $\dfrac{\lambda_0}{2}$ above a perfectly conducting infinite ground plane. The radiation pattern in the plane of the dipole ($\vec E$ plane) looks approximately as
Characteristic impedance of a transmission line is 50$\Omega$. Input impedance of the open circuited line is Zoc = 100 + j150$\Omega$. When the transmission line is short-circuited, the value of the input impedance will be
- 50 $\Omega$
- 100 + j150 $\Omega$
- 7.69 + j11.54 $\Omega$
- 7.69 - j11.54 $\Omega$
A plane wave having the electric field component $E_1$ = 24 cos(3$\times$108t -$\beta$y)$\widehat a_z$V/m and traveling in free space is incident normally on a lossless medium with m = m0 and e = 9e0 which occupies the region y ≥ 0. The reflected magnetic field component is given by
- $\dfrac{1}{10\pi} cos(3 \times 10^8 t + y) a_x \ A/m $
- $\dfrac{1}{20\pi}$cos (3$\times$108t + y)$\widehat a_x$ A/m
- -$\dfrac{1}{20\pi}$cos (3$\times$108t + y)$\widehat a_x$ A/m
- - $\dfrac{1}{10\pi}$cos (3$\times$108t + y)$\widehat a_x$ A/m
A plane electromagnetic wave propagating in free space is incident normally on a large slab of loss-less, non-magnetic, dielectric material with $\epsilon \gt \epsilon_0$. Maxima and minima are observed when the electric field is measured in front of the slab. The maximum electric field is found to be 5 times the minimum field. The intrinsic impedance of the medium should be
- 120$x \Omega$
- 60$x \Omega$
- 600$x \Omega$
- 24$x \Omega$
A rectangular metal wave-guide filled with a dielectric material of relative permittivity $\epsilon_r$ = 4 has the inside dimensions 3.0 cm $\times$ 1.2 cm. The cut-off frequency for the dominant mode is
- 2.5 GHz
- 5.0 GHz
- 10.0 GHz
- 12.5 GHz
In the circuit shown, all the transmission line sections are lossless. The Voltage Standing Wave Ration (VSWR) on the 60W line is
- 1.00
- 1.64
- 2.50
- 3.00
The direction of vector A is radially outward from the origin, with |A| = k rn where r2 = x2 + y2 + z2 and k is constant. The value of n for $\nabla$. A = 0 is
- –2
- 2
- 1
- 0
A mast antenna consisting of a 50 metre long vertical conductor operates over a perfectly conducting ground plane. It is base-fed at a frequency of 600 kHz. The radiation resistance of the antenna in Ohms is
- $\dfrac{2\pi^2}{5}$
- $\dfrac{\pi^2}{5}$
- $\dfrac{4\pi^2}{5}$
- $20\pi^2$
A right circularly polarised (RCP) plane wave is incident at an angle of 60° to the normal, on an air-dielectric interface. If the reflected wave is linearly polarised, the relative dielectric constant $\epsilon_{r2}$ is

- $\sqrt 2$
- $\sqrt 3$
- 2
- 3
A lossless transmission line is terminated in a load which reflects a part of the incident power. The measured VSWR is 2. The percentage of the power that is reflected back is
- 57.73
- 33.33
- 0.11
- 11.11
Voltage standing wave pattern in a lossless transmission line with characteristic impedance 50 $\Omega$ and a resistive load is shown in figure.

The reflection coefficient is given by
- - 0.6
- - 1
- 0.6
- 0
Voltage standing wave pattern in a lossless transmission line with characteristic impedance 50 $\Omega$ and a resistive load is shown in figure.

The value of the load resistance is
- 50 $\Omega$
- 200 $\Omega$
- 12.5 $\Omega$
- 0 $\Omega$
A medium is divided into regions I and II about x = 0 plane, as shown in the figure below. An electromagnetic wave with electric field E1 = 4$\widehat a$x + 3$\widehat a$y + 5$\widehat a$z is incident normally on the interface form region-I. The electric field E2 in region-II at the interface is

- E2 = E1
- 4$\widehat a$x + 0.75$\widehat a$y + 1.2 5$\widehat a$z
- 3$\widehat a$x + 3$\widehat a$y + 5$\widehat a$z
- - 3$\widehat a$x + 3$\widehat a$y + 5$\widehat a$z
Two identical antennas are placed in the $\theta$= $\dfrac{\pi}{2}$ plane as shown in figure. The elements have equal amplitude excitation with 180° polarity difference, operating at wavelength $\lambda$. The correct value of the magnitude of the far-zone resultant electric field strength normalized with that of a single element, both computed for $\phi$= 0, is

- 2 cos $\left( \dfrac{2\pi s}{\lambda} \right)$
- 2 sin $\left( \dfrac{2\pi s}{\lambda} \right)$
- 2 cos $\left( \dfrac{\pi s}{\lambda} \right)$
- 2 sin $\left( \dfrac{\pi s}{\lambda} \right)$











