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GATE EC Electromagnetics questions

Practise Electromagnetics questions for GATE EC. Explore official PYQs and original subject-wise quizzes, check answers and view available solutions. Free, no sign-in.

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Official PYQ2014ElectromagneticsMaxwell's EquationsNAT · 2 marks
A 1616 – bit ripple carry adder is realized using 1616 identical full adders (FA) as shown in the figure. The carry-propagation delay of each FA is 1212 ns and the sum-propagation delay of each FA is 1515 ns. The worst case delay (in ns) of this 1616-bit adder will be _______
Official PYQ2014ElectromagneticsMaxwell's EquationsNAT · 2 marks
The electric field (assumed to be one-dimensional) between two points AA and BB is shown. Let ψA\psi _A and ψB\psi _B be the electrostatic potentials at AA and BB, respectively. The value of ψB–ψA\psi _B – \psi _A in Volts is ____________
Official PYQ2014ElectromagneticsMaxwell's EquationsMCQ · 2 marks
If E→=−(2y3–3yz2)x^–(6xy2−3xz2)y^+(6xyz)z^\overrightarrow{E} = -(2y^3 – 3yz^2)\hat{x} – (6xy^2-3xz^2) \hat{y}+(6xyz) \hat{z} is the electric field in a source free region, a valid expression for the electrostatic potential is
Official PYQ2013ElectromagneticsTransmission LinesMCQ · 1 mark
In a voltage-voltage feedback as shown below, which one of the following statements is TRUE if the gain kk is increased?
Official PYQ2013ElectromagneticsTransmission LinesMCQ · 1 mark
A source vs(t)=Vcos⁡100 πtv_{s}(t) = V\cos100\:\pi t has an internal impedance of (4+j3) Ω.(4 + j3)\:\Omega. If a purely resistive load connected to this source has to extract the maximum power out of the source, its value in Ω\Omega should be
Official PYQ2012ElectromagneticsPlane Waves and PropertiesMCQ · 1 mark
A plane wave propagating in air with E→=(8a^x+6a^y+5a^z)ej(ωt+3x−4y) V/m\overrightarrow{E}=(8\hat{a}_x+6\hat{a}_y+5\hat{a}_z)e^{j(\omega t+3x-4y)}\:V/m is incident on a perfectly conducting slab positioned at x≤0x\le0 . The E→\overrightarrow{E} field of the reflected wave is
Official PYQ2012ElectromagneticsPlane Waves and PropertiesMCQ · 1 mark
The electric field of a uniform plane electromagnetic wave in free space, along the positive xx direction, is given by E→=10(a^y+ja^z)e−j 25x\overrightarrow{E}=10(\hat{a}_y+j\hat{a}_z)e^{-j\:25x}. The frequency and polarization of the wave, respectively, are
Official PYQ2012ElectromagneticsMaxwell's EquationsMCQ · 1 mark
The average power delivered to an impedance (4−j3) Ω(4-j3)\:\Omega by a current 5cos⁡(100πt+100) A5\cos(100\pi t+100)\:A is
Official PYQ2012ElectromagneticsTransmission LinesMCQ · 1 mark
A coaxial cable with an inner diameter of 1 mm1\:mm and outer diameter of 2.4 mm2.4\:mm is filled with a dielectric of relative permittivity 10.8910.89. Given μ0=4π×10−7 H/m\mu_0=4\pi\times10^{-7}\:H/m, ε0=10−936π F/m\varepsilon_0=\frac{10^{-9}}{36\pi}\:F/m, the characteristic impedance of the cable is
Official PYQ2012ElectromagneticsTransmission LinesMCQ · 1 mark
The radiation pattern of an antenna in spherical co-ordinates is given by F(θ)=cos⁡4θ   ;   0≤θ≤π2F(\theta)=\cos^4\theta\:\:\:;\:\:\:0\le \theta\le \frac{\pi}{2} The directivity of the antenna is
Official PYQ2012ElectromagneticsTransmission LinesMCQ · 1 mark
The impedance looking into nodes 11 and 22 in the given circuit is
Official PYQ2012ElectromagneticsTransmission LinesMCQ · 2 marks
A trasmission line with a characteristic impedance of 100 Ω100\:\Omega is used to match a 50 Ω50\:\Omega section to a 200 Ω200\:\Omega section. If the matching is to be done both at 429 MHz429\:MHz and 1 GHz1\:GHz, the length of the transmission line can be approximately
Official PYQ2012ElectromagneticsTransmission LinesMCQ · 2 marks
The magnetic field along the propagation direction inside a rectangular waveguide with the cross-section shown in the figure is HZ=3 cos⁡(2.094×102x) cos⁡(2.618×102y) cos⁡(6.283×1010t−βz)H_Z=3\:\cos(2.094\times10^2x)\:\cos(2.618\times10^2y)\:\cos(6.283\times10^{10}t-\beta z) The phase velocity vpv_p of the wave inside the waveguide satisfies
Official PYQ2008ElectromagneticsTransmission LinesMCQ · 1 mark
For a Hertz dipole antenna, the half power beam width (HPBW)\text{(HPBW)} in the E\text{E}-plane is
Official PYQ2006ElectromagneticsPlane Waves and PropertiesMCQ · 1 mark
The electric field of an electomagnetic wave propagating in the positive zz-direction is given by E=ax^sin⁡(ωt−βz)+ay^sin⁡(ωt−βz+π2)\left.\text{E}=\hat{a_x} \sin (\omega t-\beta z\right)+\hat{a_y} \sin \left(\omega t-\beta z+\frac{\pi}{2}\right) The wave is
Official PYQ2006ElectromagneticsTransmission LinesMCQ · 1 mark
A transmission line is feeding 1Watt1 \mathrm{Watt} of power to a horn antenna having a gain of 10 dB10 \mathrm{~dB}. The antenna is matched to the transmission line. The total power radiated by the horn antenna into the free-space is
Official PYQ2006ElectromagneticsPlane Waves and PropertiesMCQ · 1 mark
A medium of relative permittivity εr2=2\varepsilon_{r 2}=2 forms an interface with free-space. A point source of electronagnetic energy is located in the medium at a depth of 11 meter from the interface. Due to the total internal reflection, the transmitted beam has a circular cross-section over the interface. The area of the beam cross-section at the …
Official PYQ2006ElectromagneticsMaxwell's EquationsMCQ · 1 mark
A medium is divided into regions I and II about x=0x=0 plane, as shown in the figure below. An electromagnetic wave with electric field E1=4a^x+3a^y+5a^z\mathrm{E}_{1}=4 \hat{a}_{x}+3 \hat{a}_{y}+5 \hat{a}_{z} is incident normally on the interface from region-I. The electric field E2E_{2} in region-II at the interface is
Official PYQ2006ElectromagneticsPlane Waves and PropertiesMCQ · 1 mark
When a plane wave travelling in free-space is incident normally on a medium having εt=4.0\varepsilon_{t}=4.0, then fraction of power transmitted into the medium is given by
Official PYQ2006ElectromagneticsTransmission LinesMCQ · 1 mark
A rectangular waveguide having TE10\mathrm{TE}_{10} mode as dominant mode is having a cutoff frequency of 18−GHz18-\mathrm{GHz} for the TEw,\mathrm{TE}_{w,} mode. The inner broad-wall dimension of the rectangular waveguide is