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Relativity GATE

Q.No:1 GATE-2012

A rod of proper length \(l_0\) oriented parallel to the \(x\)-axis moves with speed \(2c/3\) along the \(x\)-axis in the \(S\)-frame, where \(c\) is the speed of the light in free space. The observer is also moving along the \(x\)-axis with speed \(c/2\) with respect to the \(S\)-frame. The length of the rod as measured by the observer is
(A) \(0.35l_0\)
(B) \(0.48l_0\)
(C) \(0.87l_0\)
(D) \(0.97l_0\)

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Option D

Q.No:2 GATE-2013

An electron is moving with a velocity of \(0.85c\) in the same direction as that of a moving photon. The relative velocity of the electron with respect to photon is
(A) \(c\)
(B) \(-c\)
(C) \(0.15c\)
(D) \(-0.15c\)

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Option B

Q.No:3 GATE-2013

The relativistic form of Newton's second law of motion is
(A) \(F=\frac{mc}{\sqrt{c^2-v^2}} \frac{dv}{dt}\)
(B) \(F=\frac{m\sqrt{c^2-v^2}}{c} \frac{dv}{dt}\)
(C) \(F=\frac{mc^2}{c^2-v^2} \frac{dv}{dt}\)
(D) \(F=m\frac{c^2-v^2}{c^2} \frac{dv}{dt}\)

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Option C

Q.No:4 GATE-2014

If the half-life of an elementary particle moving with speed \(0.9c\) in the laboratory frame is \(5\times 10^{-8} s\), then the proper half-life is _____________(\times 10^{-8} s\). (\(c=3\times 10^8 m/s\))

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Ans 2.1-2.3

Q.No:5 GATE-2015

In an inertial frame \(S\), two events \(A\) and \(B\) take place at (\(ct_A=0, \vec{r}_A=0\)) and (\(ct_B=0, \vec{r}_B=2\hat{y}\)), respectively. The times at which these events take place in a frame \(S'\) moving with a velocity \(0.6c\hat{y}\) with respect to \(S\) are given by
(A) \(ct'_A=0; ct'_B=-3/2\)
(B) \(ct'_A=0; ct'_B=0\)
(C) \(ct'_A=0; ct'_B=3/2\)
(D) \(ct'_A=0; ct'_B=1/2\)

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Option A

Q.No:6 GATE-2016

The kinetic energy of a particle of rest mass \(m_0\) is equal to its rest mass energy. Its momentum in units of \(m_0 c\), where \(c\) is the speed of light in vacuum, is ___________. (Give your answer upto two decimal places)

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Ans 1.72-1.74

Q.No:7 GATE-2016

In an inertial frame of reference \(S\), an observer finds two events occurring at the same time at coordinates \(x_1=0\) and \(x_2=d\). A different inertial frame \(S'\) moves with velocity \(v\) with respect to \(S\) along the positive \(x\)-axis. An observer in \(S'\) also notices these two events and finds them to occur at times \(t_1'\) and \(t_2'\) and at positions \(x_1'\) and \(x_2'\), respectively. If \(\Delta t'=t_2'-t_1', \Delta x'=x_2'-x_1'\) and \(\gamma=\frac{1}{\sqrt{1-\frac{v^2}{c^2}}}\), which of the following statements is true?
(A) \(\Delta t'=0, \Delta x'=\gamma d\)
(B) \(\Delta t'=0, \Delta x'=d/\gamma\)
(C) \(\Delta t'=-\gamma vd/c^2, \Delta x'=\gamma d\)
(D) \(\Delta t'=-\gamma vd/c^2, \Delta x'=d/\gamma\)

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Option C

Q.No:8 GATE-2017

An object travels along the \(x\)-direction with velocity \(c/2\) in a frame \(O\). An observer in a frame \(O'\) sees the same object travelling with velocity \(c/4\). The relative velocity of \(O'\) with respect to \(O\) in units of \(c\) is __________. (up to two decimal places).

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Ans 0.27-0.31

Q.No:9 GATE-2019

Two spaceships A and B, each of the same rest length \(L\), are moving in the same direction with speeds \(\frac{4c}{5}\) and \(\frac{3c}{5}\), respectively, where \(c\) is the speed of light. As measured by B, the time taken by A to completely overtake B [see figure below] in units of \(L/c\) (to the nearest integer) is _____________
Image

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Ans 5

Q.No:10 GATE-2019

Two events, one on the earth and the other one on the Sun, occur simultaneously in the earth's frame. The time difference between the two events as seen by an observer in a spaceship moving with velocity \(0.5c\) in the earth's frame along the line joining the earth to the Sun is \(\Delta t\), where \(c\) is the speed of light. Given that light travels from the Sun to the earth in \(8.3\) minutes in the earth's frame, the value of \(|\Delta t|\) in minutes (rounded off to two decimal places) is _______________-.

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Ans 4.77-4.81

Q.No:11 GATE-2021

Two observers \(O\) and \(O'\) observe two events \(P\) and \(Q\). The observers have a constant relative speed of \(0.5c\). In the units, where the speed of light, \(c\), is taken as unity, the observer \(O\) obtained the following coordinates: Event \(P\): \(x=5, y=3, z=5, t=3\) Event \(Q\): \(x=5, y=1, z=3, t=5\) The length of the space-time interval between these two events, as measured by \(O'\), is \(L\). The value of \(|L|\) (in integer) is ____________________.

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Ans 2

Q.No:1 CSIR Dec-2014

According to the special theory of relativity, the speed \(v\) of a free particle of mass \(m\) and total energy \(E\) is:
(1) \(v=c\sqrt{1-\frac{mc^2}{E}}\)
(2) \(v=\sqrt{\frac{2E}{m}}\left(1+\frac{mc^2}{E}\right)\)
(3) \(v=c\sqrt{1-\left(\frac{mc^2}{E}\right)^2}\)
(4) \(v=c\left(1+\frac{mc^2}{E}\right)\)

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Option 3

Q.No:2 CSIR June-2015

Consider three inertial frames of reference A. B and C. The frame B moves with a vclocity \(c/2\) with respect to A, and C moves with a velocity $c/10$ with respect to B in the same direction. The velocity of C as measured in A is
(1) \(\frac{3c}{7}\)
(2) \(\frac{4c}{7}\)
(3) \(\frac{c}{7}\)
(4) \(\frac{\sqrt{3c}}{7}\)

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Option 2

Q.No:3 CSIR June-2015

A rod of length \(L\) carries a total charge \(Q\) distributed uniformly. If this is observed in a frame moving with a speed \(v\) along the rod, the charge per unit length (as measured by the moving observer) is
(1) \(\frac{Q}{L}\left(1-\frac{v^{2}}{c^{2}}\right)\)
(2) \(\frac{Q}{L} \sqrt{1-\frac{v^{2}}{c^{2}}}\)
(3) \(\frac{Q}{L \sqrt{1-\frac{v^{2}}{c^{2}}}}\)
(4) \(\frac{Q}{L\left(1-\frac{v^{2}}{c^{2}}\right)}\)

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Option 3

Q.No:4 CSIR Dec-2015

Consider a particle of mass \(m\) moving with a speed \(v\). If \(T_R\) denotes the relativistic kinetic energy and \(T_N\) its non-relativistic approximation, then the value of \((T_R-T_N)/T_R\) for \(v=0.01 c\), is
(1) \(1.25\times 10^{-5}\)
(2) \(5.0\times 10^{-5}\)
(3) \(7.5\times 10^{-5}\)
(4) \(1.0\times 10^{-4}\)

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Option 3

Q.No:5 CSIR Dec-2015

A distant source, emitting radiation of frequency \(\omega\), moves with a velocity \(4c/5\) in a certain direction with respect to a receiver (as shown in the figure).
Image
The upper cut-off frequency of the receiver is \(3\omega/2\). Let \(\theta\) be the angle as shown. For the receiver to detect the radiation, \(\theta\) should at least be
(1) \(\cos^{-1}{\left(\frac{1}{2}\right)}\)
(2) \(\cos^{-1}{\left(\frac{3}{4}\right)}\)
(3) \(\cos^{-1}{\left(\frac{2}{\sqrt{5}}\right)}\)
(4) \(\cos^{-1}{\left(\sqrt{\frac{2}{3}}\right)}\)

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Option 2

Q.No:6 CSIR June-2016

Let \((x, t)\) and \((x', t')\) be the coordinate systems used by the observers \(O\) and \(O'\), respectively. Observer \(O'\) moves with a velocity \(v=\beta c\) along their common positive \(x\)-axis. If \(x_+=x+ct\) and \(x_-=x-ct\) are the linear combinations of the coordinates, the Lorentz transformation relating \(O\) and \(O'\) takes the form
(1) \(x_+'=\frac{x_--\beta x_+}{\sqrt{1-\beta^2}}\) and \(x_-'=\frac{x_+-\beta x_-}{\sqrt{1-\beta^2}}\),
(2) \(x_+'=\sqrt{\frac{1+\beta}{1-\beta}}x_+\) and \(x_-'=\sqrt{\frac{1-\beta}{1+\beta}}x_-\),
(3) \(x_+'=\frac{x_+-\beta x_-}{\sqrt{1-\beta^2}}\) and \(x_-'=\frac{x_--\beta x_+}{\sqrt{1-\beta^2}}\),
(4) \(x_+'=\sqrt{\frac{1-\beta}{1+\beta}}x_+\) and \(x_-'=\sqrt{\frac{1+\beta}{1-\beta}}x_-\),

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Option 4

Q.No:7 CSIR June-2016

For a particle of energy \(E\) and momentum \(\mathbf{p}\) (in a frame \(F\)), the rapidity \(y\) is defined as \(y=\frac{1}{2}\ln{\left(\frac{E+p_3 c}{E-p_3 c}\right)}\). In a frame \(F'\) moving with velocity \(\mathbf{v}=(0, 0, \beta c)\) with respect to \(F\), the rapidity \(y'\) will be
(1) \(y'=y+\frac{1}{2}\ln{(1-\beta^2)}\)
(2) \(y'=y-\frac{1}{2}\ln{\left(\frac{1+\beta}{1-\beta}\right)}\)
(3) \(y'=y+\ln{\left(\frac{1+\beta}{1-\beta}\right)}\)
(4) \(y'=y+2\ln{\left(\frac{1+\beta}{1-\beta}\right)}\)

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Option 2

Q.No:8 CSIR Dec-2016

A relativistic particle moves with a constant velocity \(v\) with respect to the laboratory frame. In time \(\tau\), measured in the rest frame of the particle, the distance that it travels in the laboratory frame is
(1) \(v\tau\)
(2) \(\frac{c\tau}{\sqrt{1-\frac{v^2}{c^2}}}\)
(3) \(v\tau\sqrt{1-\frac{v^2}{c^2}}\)
(4) \(y'=y+2\ln{\left(\frac{1+\beta}{1-\beta}\right)}\)

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Option 4

Q.No:9 CSIR Dec-2016

Consider a radioactive nucleus that is travelling at a speed \(c/2\) with respect to the lab frame. It emits \(\gamma\)-rays of frequency \(\nu_0\) in its rest frame. There is a stationary detector (which is not on the path of the nucleus) in the lab. If a \(\gamma\)-ray photon is emitted when the nucleus is closest to the detector, its observed frequency at the detector is
(1) \(\frac{\sqrt{3}}{2}\nu_0\)
(2) \(\frac{1}{\sqrt{3}}\nu_0\)
(3) \(\frac{1}{\sqrt{2}}\nu_0\)
(4) \(\sqrt{\frac{2}{3}}\nu_0\)

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Option 1

Q.No:10 CSIR June-2017

An inertial observer sees two events \(E_1\) and \(E_2\) happening at the same location but \(6 \mu s\) apart in time. Another observer moving with a constant velocity \(v\) (with respect to the first one) sees the same events to be \(9 \mu s\) apart. The spatial distance between the events, as measured by the second observer, is approximately
(1) \(300 m\)
(2) \(1000 m\)
(3) \(2000 m\)
(4) \(2700 m\)

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Option 3

Q.No:11 CSIR Dec-2017

A light signal travels from a point A to a point B, both within a glass slab that is moving with uniform velocity (in the same direction as the light) with speed \(0.3c\) with respect to an external observer. If the refractive index of the slab is \(1.5\), then the observer will measure the speed of the signal as
(1) \(0.67c\)
(2) \(0.81c\)
(3) \(0.97c\)
(4) \(c\)

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Option 2

Q.No:12 CSIR Dec-2017

In an inertial frame \(\mathbf{S}\), the magnetic vector potential in a region of space is given by \(\vec{A}=az\hat{i}\) (where \(a\) is a constant) and the scalar potential is zero. The electric and magnetic fields seen by an inertial observer moving with a velocity \(v\hat{i}\) with respect to \(\mathbf{S}\), are, respectively [In the following \(\gamma=\frac{1}{\sqrt{1-v^2/c^2}}\).]
(1) \(0\) and \(\gamma a\hat{j}\)
(2) \(-va\hat{k}\) and \(\gamma a\hat{i}\)
(3) \(v\gamma a\hat{k}\) and \(v\gamma a\hat{j}\)
(4) \(v\gamma a\hat{k}\) and \(\gamma a\hat{j}\)

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Option 4

Q.No:13 CSIR June-2018

Two particles \(A\) and \(B\) move with relativistic velocities of equal magnitude \(v\), but in opposite directions, along the \(x\)-axis of an inertial frame of reference. The magnitude of the velocity of \(A\), as seen from the rest frame of \(B\), is
(1) \(2v/\left(1-\frac{v^2}{c^2}\right)\)
(2) \(2v/\left(1+\frac{v^2}{c^2}\right)\)
(3) \(2v\sqrt{\frac{c-v}{c+v}}\)
(4) \(2v/\sqrt{1-\frac{v^2}{c^2}}\)

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Option 2

Q.No:14 CSIR June-2018

An inertial frame \(K'\) moves with a constant speed \(v\) with respect to another inertial frame \(K\) along their common \(x\)-axis in the positive \(x\)-direction. Let \((x, ct)\) and \((x', ct')\) denote the space-time coordinates in the frames \(K\) and \(K'\), respectively. Which of the following space-time diagrams correctly describes the \(t'\)-axis (\(x'=0\) line) and the \(x'\)-axis (\(t'=0\) line) in the \(x\)-\(ct\) plane? (In the following figures \(\tan{\varphi}=v/c\).)
Image
Image
(1)
Image
(2)
Image
(3)
Image
(4)

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Option 2

Q.No:15 CSIR June-2018

The energy of a free relativistic particle is \(E=\sqrt{|\vec{p}|^2 c^2+m^2 c^4}\), where \(m\) is its rest mass, \(\vec{p}\) is its momentum and \(c\) is the speed of light in vacuum. The ratio \(v_g/v_p\) of the group velocity \(v_g\) of a quantum mechanical wave packet (describing this particle) to the phase velocity \(v_p\) is
(1) \(|\vec{p}| c/E\)
(2) \(|\vec{p}|mc^3/E^2\)
(3) \(|\vec{p}|^2 c^2/E^2\)
(4) \(|\vec{p}| c/2E\)

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Option 3

Q.No:16 CSIR Dec-2018

A relativistic particle of mass \(m\) and charge \(e\) is moving in a uniform electric field of strength \(\mathcal{E}\). Starting from rest at \(t=0\), how much time will it take to reach the speed \(c/2\)?
(1) \(\frac{1}{\sqrt{3}} \frac{mc}{e\mathcal{E}}\)
(2) \(\frac{mc}{e\mathcal{E}}\)
(3) \(\sqrt{2} \frac{mc}{e\mathcal{E}}\)
(4) \(\sqrt{\frac{3}{2}} \frac{mc}{e\mathcal{E}}\)

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Option 1

Q.No:17 CSIR June-2019

A point charge is moving with a uniform velocity \(\beta c\) along the positive \(x\)-direction, parallel to and very close to a corrugated metal sheet (see the figure below).
Image
The wavelength of the electromagnetic radiation received by an observer along the direction of motion is
(1) \(\frac{L}{\beta}\sqrt{1-\beta^2}\)
(2) \(L\sqrt{1-\beta^2}\)
(3) \(L\beta \sqrt{1-\beta^2}\)
(4) \(L\)

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Option 1

Q.No:18 Assam CSIR Dec-2019

Two particles, each of rest mass \(M\) and speed \(0.8c\) are moving towards each other in an inertial frame. They collide to form a single particle. The rest mass of the new particle is
(1) \(\frac{4}{3}M\)
(2) \(\frac{10}{3}M\)
(3) \(\frac{5}{3}M\)
(4) \(2M\)

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Option 2

Q.No:19 Assam CSIR Dec-2019

Light emitted at \((ct, x, y, z)\) is absorbed at \((c(t+\Delta t), x+\Delta x, y+\Delta y, z+\Delta z)\) when propagating in a medium with refractive index \(n\). The square of the proper time between the two events is
(1) \(\left(\frac{n^2-1}{n^2+1}\right)(\Delta t)^2\)
(2) \(\left(\frac{n^2}{n^2+1}\right)(\Delta t)^2\)
(3) \(\left(\frac{n^2-1}{n^2}\right)(\Delta t)^2\)
(4) \(\left(\frac{n-1}{n+1}\right)(\Delta t)^2\)

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Option 3

Q.No:20 CSIR June-2020

A heavy particle of rest mass \(M\) while moving along the positive \(z\)-direction, decays into two identical light particles with rest mass \(m\) (where \(M>2m\)). The maximum value of the momentum that any one of the lighter particles can have in a direction perpendicular to the \(z\)-direction, is
(a) \(\frac{1}{2}C\sqrt{M^2-4m^2}\)
(b) \(\frac{1}{2}C\sqrt{M^2-2m^2}\)
(c) \(C\sqrt{M^2-4m^2}\)
(d) \(\frac{1}{2}MC\)

Check Answer

Option a

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