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Waves question

2007 · Shift 2 · Q28
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Waves question

2007 · Shift 2 · Q28

JEE AdvancedPhysicsWavesMCQ+4 / −1

Column I describe some situations in which a small object moves. Column II describes some characteristics of these motions. Match the situation in Column I with the characteristics in Column II and indicate your answer by darkening appropriate bubbles in the 4×44 \times 44×4 matrix given in the ORS.

Column I Column II
(A) The object moves on the x-axis under a conservative force in such a way that its "speed" and "position" satisfy v=c1c2−x2v = {c_1}\sqrt {{c_2} - {x^2}}v=c1​c2​−x2​, where c1c_1c1​ and c2c_2c2​ are positive constants. (P) The object executes a simple harmonic motion.
(B) The object moves on the x-axis in such a way that its velocity and its displacement from the origin satisfy v=−kxv=-kxv=−kx, where kkk is a positive constant. (Q) The object does not change its direction.
(C) The object is attached to one end of a massless spring of a given spring constant. The other end of the spring is attached to the ceiling of an elevator. Initially everything is at rest. The elevator starts going upwards with a constant acceleration a. The motion of the object is observed from the elevator during the period it maintains this acceleration. (R) The kinetic energy of the object keeps on decreasing
(D) The object is projected from the earth's surface vertically upwards with a speed 2GMe/Reolimits2\sqrt {GMe/{\mathop{\rm Re} olimits} }2GMe/Reolimits​, where, M e_ee​ is the mass of the earth and R e_ee​ is the radius of the earth. Neglect forces from objects other than the earth. (S) The object can change its direction only once.

  1. A
    [A→(P);B→(Q,R);C→(P);D→(Q,R)][\mathrm{A} \rightarrow(\mathrm{P}); \mathrm{B} \rightarrow(\mathrm{Q}, \mathrm{R}); \mathrm{C} \rightarrow(\mathrm{P}); \mathrm{D} \rightarrow(\mathbf{Q}, \mathrm{R})][A→(P);B→(Q,R);C→(P);D→(Q,R)]
  2. B
    [A→(Q,R);B→(Q,R);C→(P);D→(S,R)][\mathrm{A} \rightarrow(\mathrm{Q, R}); \mathrm{B} \rightarrow(\mathrm{Q}, \mathrm{R}); \mathrm{C} \rightarrow(\mathrm{P}); \mathrm{D} \rightarrow(\mathbf{S}, \mathrm{R})][A→(Q,R);B→(Q,R);C→(P);D→(S,R)]
  3. C
    [A→(P,S);B→(Q,R);C→(P);D→(R)][\mathrm{A} \rightarrow(\mathrm{P, S}); \mathrm{B} \rightarrow(\mathrm{Q}, \mathrm{R}); \mathrm{C} \rightarrow(\mathrm{P}); \mathrm{D} \rightarrow(\mathbf{R})][A→(P,S);B→(Q,R);C→(P);D→(R)]
  4. D
    [A→(P,R);B→(Q,R);C→(P);D→(S)][\mathrm{A} \rightarrow(\mathrm{P, R}); \mathrm{B} \rightarrow(\mathrm{Q}, \mathrm{R}); \mathrm{C} \rightarrow(\mathrm{P}); \mathrm{D} \rightarrow(\mathbf{S})][A→(P,R);B→(Q,R);C→(P);D→(S)]
View written solutionFree

Correct answer: A

Analysis of each option in Column I:

1. Situation (A): The object's motion is described by the equation v=c1c2−x2v = c_1\sqrt{c_2 - x^2}v=c1​c2​−x2​, where vvv is the speed, xxx is the position, and c1,c2c_1, c_2c1​,c2​ are positive constants.

  • Squaring the equation gives: v2=c12(c2−x2)v^2 = c_1^2 (c_2 - x^2)v2=c12​(c2​−x2).
  • We find the acceleration, aaa, using the formula a=vdvdxa = v \frac{dv}{dx}a=vdxdv​. To find dvdx\frac{dv}{dx}dxdv​, we can differentiate the equation for v2v^2v2 with respect to xxx: 2vdvdx=c12(−2x)2v \frac{dv}{dx} = c_1^2 (-2x)2vdxdv​=c12​(−2x) vdvdx=−c12xv \frac{dv}{dx} = -c_1^2 xvdxdv​=−c12​x
  • Therefore, the acceleration is a=−c12xa = -c_1^2 xa=−c12​x.
  • This equation is of the form a=−ω2xa = -\omega^2 xa=−ω2x (with ω=c1\omega = c_1ω=c1​), which is the defining condition for Simple Harmonic Motion (SHM).
  • Thus, situation (A) matches with characteristic (P).
  • In SHM, the object oscillates, so it changes direction at the extreme points. Its kinetic energy increases and decreases periodically. Therefore, (Q), (R), and (S) are incorrect.
  • Match for (A): (P)

2. Situation (B): The motion is described by v=−kxv = -kxv=−kx, where kkk is a positive constant.

  • This is a differential equation: dxdt=−kx\frac{dx}{dt} = -kxdtdx​=−kx. The solution is x(t)=x0e−ktx(t) = x_0 e^{-kt}x(t)=x0​e−kt, where x0x_0x0​ is the initial position.
  • The position x(t)x(t)x(t) decays exponentially to 0. The object always moves towards the origin. If x0>0x_0 > 0x0​>0, v<0v < 0v<0 always. If x0<0x_0 < 0x0​<0, v>0v > 0v>0 always. The object never changes its direction.
  • Thus, situation (B) matches with characteristic (Q).
  • The kinetic energy is K=12mv2=12m(−kx)2=12mk2x2K = \frac{1}{2}mv^2 = \frac{1}{2}m(-kx)^2 = \frac{1}{2}mk^2x^2K=21​mv2=21​m(−kx)2=21​mk2x2. Since the magnitude of position, ∣x(t)∣=∣x0∣e−kt|x(t)| = |x_0|e^{-kt}∣x(t)∣=∣x0​∣e−kt, continuously decreases with time, the kinetic energy also continuously decreases.
  • Thus, situation (B) also matches with characteristic (R).
  • The acceleration is a=dvdt=−kdxdt=−k(v)=−k(−kx)=k2xa = \frac{dv}{dt} = -k\frac{dx}{dt} = -k(v) = -k(-kx) = k^2xa=dtdv​=−kdtdx​=−k(v)=−k(−kx)=k2x. This is not SHM. So (P) is incorrect. The object never changes direction, so (S) is incorrect.
  • Matches for (B): (Q), (R)

3. Situation (C): An object on a spring is inside an elevator accelerating upwards with acceleration aaa. The motion is observed from the elevator's frame.

  • In the non-inertial frame of the elevator, there is a downward pseudo-force Fpseudo=maF_{pseudo} = maFpseudo​=ma acting on the object.
  • The effective gravitational acceleration is geff=g+ag_{eff} = g + ageff​=g+a.
  • The object will oscillate about a new equilibrium position where the upward spring force balances the total downward force (gravity + pseudo-force), i.e., kxeq=m(g+a)kx_{eq} = m(g+a)kxeq​=m(g+a).
  • The net restoring force for a displacement zzz from this new equilibrium position is Fnet=−kzF_{net} = -kzFnet​=−kz.
  • The equation of motion is md2zdt2=−kzm\frac{d^2z}{dt^2} = -kzmdt2d2z​=−kz, which is the equation for SHM.
  • Thus, situation (C) matches with characteristic (P).
  • Since the motion is SHM, characteristics (Q), (R), and (S) are incorrect for the same reasons as in case (A).
  • Match for (C): (P)

4. Situation (D): An object is projected vertically upwards from Earth's surface with speed v0=2GMe/Rev_0 = 2\sqrt{GM_e/R_e}v0​=2GMe​/Re​​.

  • The escape velocity from the Earth's surface is ve=2GMe/Rev_e = \sqrt{2GM_e/R_e}ve​=2GMe​/Re​​.
  • The given initial speed is v0=4GMe/Re=2×2GMe/Re=2vev_0 = \sqrt{4GM_e/R_e} = \sqrt{2} \times \sqrt{2GM_e/R_e} = \sqrt{2}v_ev0​=4GMe​/Re​​=2​×2GMe​/Re​​=2​ve​.
  • Since v0>vev_0 > v_ev0​>ve​, the object will escape Earth's gravitational pull and will never return. It will continue to move away from the Earth.
  • As the object is projected upwards and the gravitational force is always downwards, the object's speed will decrease, but it will never become zero. The direction of velocity will always be upwards.
  • Therefore, the object does not change its direction. Thus, situation (D) matches characteristic (Q).
  • The speed of the object continuously decreases from v0=2vev_0 = \sqrt{2}v_ev0​=2​ve​ to a final, non-zero speed at infinity v∞=vev_\infty = v_ev∞​=ve​. Since the speed is always decreasing, the kinetic energy (K=12mv2K = \frac{1}{2}mv^2K=21​mv2) also keeps on decreasing.
  • Thus, situation (D) also matches characteristic (R).
  • The force is gravitational (F∝1/r2F \propto 1/r^2F∝1/r2), not linear, so it's not SHM. It never changes direction, so (S) is incorrect.
  • Matches for (D): (Q), (R)

Summary of Matches:

  • (A) →\rightarrow→ (P)
  • (B) →\rightarrow→ (Q), (R)
  • (C) →\rightarrow→ (P)
  • (D) →\rightarrow→ (Q), (R)

This corresponds to option A.

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