NVAEasyJEE 2026Simple Harmonic Motion (SHM)

JEE Physics 2026 Question with Solution

The displacement of a particle executing simple harmonic motion with time period TT is expressed as x(t)=Asinωt,x(t)=A\sin\omega t, where AA is the amplitude of oscillation. If the maximum value of the potential energy of the oscillator is found at t=T2β,t=\frac{T}{2\beta}, then the value of β\beta is _____.

Answer

Correct answer:2

Step-by-step solution

Standard Method

Given: The displacement is x=Asinωtx = A\sin\omega t and the time period is TT.

Find: The value of β\beta if maximum potential energy occurs at t=T2βt = \frac{T}{2\beta}.

Concept: In SHM, potential energy is

U=12kx2U = \frac{1}{2}kx^2

So potential energy is maximum when the magnitude of displacement is maximum, that is, when x=A|x| = A.

From

x=Asinωtx = A\sin\omega t

maximum potential energy occurs when

sinωt=±1\sin\omega t = \pm 1

The first time for this is

ωt=π2\omega t = \frac{\pi}{2}

Therefore,

t=π2ωt = \frac{\pi}{2\omega}

Using

ω=2πT\omega = \frac{2\pi}{T}

we get

t=π2T2π=T4t = \frac{\pi}{2}\cdot\frac{T}{2\pi} = \frac{T}{4}

Given that

t=T2βt = \frac{T}{2\beta}

So,

T2β=T4\frac{T}{2\beta} = \frac{T}{4}

Hence,

2β=42\beta = 4

which gives

β=2\beta = 2

Therefore, the value of β\beta is 22.

Using extreme position condition

Given: The oscillator follows x=Asinωtx = A\sin\omega t.

Find: The value of β\beta.

Potential energy in SHM depends on displacement squared, so it is greatest at the extreme positions. Thus the required condition is that the particle must be at x=Ax = A or x=Ax = -A.

From

x=Asinωtx = A\sin\omega t

we require

Asinωt=±AA\sin\omega t = \pm A

so

sinωt=±1\sin\omega t = \pm 1

The earliest positive time occurs for

ωt=π2\omega t = \frac{\pi}{2}

Thus,

t=π2ωt = \frac{\pi}{2\omega}

Now substitute

ω=2πT\omega = \frac{2\pi}{T}

Then

t=π2(2πT)t = \frac{\pi}{2\left(\frac{2\pi}{T}\right)}

which simplifies to

t=πT4π=T4t = \frac{\pi T}{4\pi} = \frac{T}{4}

The question gives

t=T2βt = \frac{T}{2\beta}

Equating the two expressions:

T2β=T4\frac{T}{2\beta} = \frac{T}{4}

Cancel TT from both sides:

12β=14\frac{1}{2\beta} = \frac{1}{4}

Therefore,

2β=42\beta = 4

and hence

β=2\beta = 2

Therefore, the final answer is 22.

Common mistakes

  • Assuming potential energy is maximum at the mean position. This is wrong because at the mean position x=0x = 0, so U=12kx2=0U = \frac{1}{2}kx^2 = 0. Use the extreme position condition x=A|x| = A instead.

  • Using the time for a full cycle or half cycle instead of the first extreme position. This is wrong because the earliest time when sinωt=1\sin\omega t = 1 is at ωt=π2\omega t = \frac{\pi}{2}, giving t=T4t = \frac{T}{4}, not T2\frac{T}{2} or TT.

  • Substituting ω\omega incorrectly from the time period relation. This is wrong because for SHM, ω=2πT\omega = \frac{2\pi}{T}. Using any other relation gives an incorrect time and hence a wrong value of β\beta.

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