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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a O T t
a O T t
a O T t
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).
β2 α2
α β www.vedantu.com 41
β2 α
2πβ α
Solution
ω2A=α ωA=β ⇒ω= α β ⇒T= 2π ω =2πβ α
5 π
5 2π
4 5 π
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=
1 : 6
1 : 9
1 : 11
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 ==
2 s
π s
2 π s
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.
fuse
conductor
inductor
switch
Solution
Conceptual
π rad
3 rad 2 π
rad 2 π
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.
n
2n
3n
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.
0.0628 s
6.28 s
3.14 s
0.628 s
Solution
The spring constant is given by . The time period of oscillations is , so option (d) is correct.
11
9
10
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.
5 cm, 2 s
5 m, 2 s
5 cm, 1 s
5 m, 1 s
Solution
5sin m 3 π⎛⎞= π + ⎜⎟⎝⎠ xt Amplitude = 5 m 2πω = π = T 2 2sπ==πT
3
2
23
4
Solution
2T g ′′ =π where 2 ′ = 2T g=π 2 xTT′ = 22 22 x ggπ = π 1 222 x x= ⇒ =
Graph showing ω(t) increasing with time and A(t) constant with time.
Graph showing ω(t) increasing with time and A(t) decreasing with time.
Graph showing ω(t) increasing with time and A(t) increasing with time.
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.
Solution
Maximum velocity
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