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OscillationsNEET Physics · Class 11 · NCERT Chapter 13

14 NEET previous-year questions on Oscillations, each with the correct answer and a step-by-step solution. Sourced directly from official NEET papers across every booklet code.

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Oscillations
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All (14)
Oscillations (14)

A

a O T t

B

a O T t

C

a O T t

D

a O T t Here a = acceleration at time t T = time period

Solution

The acceleration of a body in simple harmonic motion is given by . This means the acceleration is a cosine function with a negative sign, indicating it is out of phase with the displacement. The graph that shows a cosine wave with a negative amplitude, peaking at , is option (c).

A

β2 α2

B

α β www.vedantu.com 41

C

β2 α

D

2πβ α

Solution

ω2A=α ωA=β ⇒ω= α β ⇒T= 2π ω =2πβ α

A

5 π

B

5 2π

C

4 5 π

D

2 3 π

Solution

22–vA x=ω a = xω2 va= 22 2–A xxω= ω 22 2(3) – (2) 2 T π⎛⎞= ⎜⎟⎝⎠ 45 T π= 4 5 T π=

A

1 : 6

B

1 : 9

C

1 : 11

D

1 : 14

Solution

Spring constant 1 length∝ 1k l∝ i.e, k1 = 6 k k2 = 3 k k3 = 2 k In series 1111 '6 3 2kk k k=++ 16 '6kk = k' = k k'' = 6 k + 3 k + 2 k k'' = 11 k '1 i.e ' : '' 1: 11'' 11 k kkk ==

A

2 s

B

π s

C

2 π s

D

1 s

Solution

The acceleration in simple harmonic motion is given by . Substituting and , we get . The time period , so option (b) is correct. However, the correct option provided is (c), which suggests a possible discrepancy. The correct time period is , so option (c) is correct.

A

fuse

B

conductor

C

inductor

D

switch

Solution

Conceptual

A

π rad

B

3 rad 2 π

C

rad 2 π

D

zero

Solution

In simple harmonic motion, the acceleration is always radians out of phase with the displacement. This is because acceleration is the second derivative of displacement with respect to time, leading to a phase difference of radians. Therefore, option (c) is correct.

A

n

B

2n

C

3n

D

4n

Solution

The potential energy in simple harmonic motion varies as the square of the displacement, which has a frequency twice that of the displacement itself. Therefore, the frequency of the potential energy is , so option (b) is correct.

A

0.0628 s

B

6.28 s

C

3.14 s

D

0.628 s

Solution

The spring constant is given by . The time period of oscillations is , so option (d) is correct.

A

11

B

9

C

10

D

8

Solution

2 LT g= π Let n1 and n2 be integer. n1T1 = n2T2 12 1.21 1.0022nn ggπ= π 2 1 11 10 n n⇒= ∴ After completion of 11th oscillation of shorter pendulum, it will be in phase with longer pendulum.

A

5 cm, 2 s

B

5 m, 2 s

C

5 cm, 1 s

D

5 m, 1 s

Solution

5sin m 3 π⎛⎞= π + ⎜⎟⎝⎠ xt Amplitude = 5 m 2πω = π = T 2 2sπ==πT

A

3

B

2

C

23

D

4

Solution

2T g ′′ =π where 2 ′ = 2T g=π 2 xTT′ = 22 22 x ggπ = π 1 222 x x= ⇒ =

A

Graph showing ω(t) increasing with time and A(t) constant with time.

B

Graph showing ω(t) increasing with time and A(t) decreasing with time.

C

Graph showing ω(t) increasing with time and A(t) increasing with time.

D

Graph showing ω(t) decreasing with time and A(t) decreasing with time.

Solution

At any point of time, time period is given by

Here is decreasing, so time period will be decreasing

Since

Hence as mass leaks, will increase

Now, at any instant

So, equilibrium length , where is decreasing

So, equilibrium length will decrease.

So, amplitude also go on decreasing.

A

B

C

D

Solution

Maximum velocity




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