MCQMediumJEE 2023Simple Harmonic Motion (SHM)

JEE Physics 2023 Question with Solution

Assume that the Earth is a solid sphere of uniform density and a tunnel is dug along its diameter. When a particle is released in this tunnel, it executes a simple harmonic motion. The mass of the particle is 100g100 \, \text{g}. The time period of the motion of the particle will be (approximately):

  • A

    24hours24 \, \text{hours}

  • B

    1hour  24minutes1 \, \text{hour} \; 24 \, \text{minutes}

  • C

    1hour  40minutes1 \, \text{hour} \; 40 \, \text{minutes}

  • D

    12hours12 \, \text{hours}

Answer

Correct answer:B

Step-by-step solution

Standard Method

Given: Earth is assumed to be a uniform solid sphere, a tunnel is dug along its diameter, and the particle mass is 100g100 \, \text{g}.

Find: The time period of oscillation inside the Earth.

A circular cross-section of Earth with a horizontal diameter tunnel, a particle inside the tunnel, and displacement x marked from the centre.

At a distance xx from the centre of the Earth, the gravitational field inside a uniform sphere is proportional to displacement:

E=GMR3xE = \frac{GM}{R^3}x

Hence the acceleration of the particle is directed toward the centre:

a=GMR3x\vec{a} = -\frac{GM}{R^3}\vec{x}

This is the condition for simple harmonic motion, so

ω=GMR3\omega = \sqrt{\frac{GM}{R^3}}

Using g=GMR2g = \frac{GM}{R^2},

ω=gR\omega = \sqrt{\frac{g}{R}}

Therefore,

T=2πω=2πRgT = \frac{2\pi}{\omega} = 2\pi\sqrt{\frac{R}{g}}

Now substitute R=6400×103mR = 6400 \times 10^3 \, \text{m} and g=10m/s2g = 10 \, \text{m/s}^2:

T=2×3.14×6400×10310T = 2 \times 3.14 \times \sqrt{\frac{6400 \times 10^3}{10}} =2×3.14×800s= 2 \times 3.14 \times 800 \, \text{s}

So,

T5026sT \approx 5026 \, \text{s}

which is approximately 1hour  24minutes1 \, \text{hour} \; 24 \, \text{minutes}.

Therefore, the correct option is B.

Using the SHM result inside a uniform sphere

Given: Motion of a particle through a diameter tunnel inside a uniform Earth.

Find: The approximate time period.

For SHM inside the Earth, the effective force is proportional to displacement:

F=GMrR3F = -\frac{GMr}{R^3}

and therefore

a=Fm=GMR3ra = \frac{F}{m} = -\frac{GM}{R^3}r

So the time period is

T=2πR3GMT = 2\pi \sqrt{\frac{R^3}{GM}}

Using

g=GMR2g = \frac{GM}{R^2}

we get

T=2πRgT = 2\pi \sqrt{\frac{R}{g}}

Now take

R=6400km=6.4×106mR = 6400 \, \text{km} = 6.4 \times 10^6 \, \text{m}

and

g=10m/s2g = 10 \, \text{m/s}^2

Then

T=2π6.4×10610=2π6.4×105T = 2\pi \sqrt{\frac{6.4 \times 10^6}{10}} = 2\pi \sqrt{6.4 \times 10^5} T2π×800=5026sT \approx 2\pi \times 800 = 5026 \, \text{s}

This is approximately 1hour  24minutes1 \, \text{hour} \; 24 \, \text{minutes}.

The particle mass does not affect the time period. Although one the solution marks option A, the worked numerical result clearly matches 1hour  24minutes1 \, \text{hour} \; 24 \, \text{minutes}, so the correct option is B.

Common mistakes

  • Using the mass 100g100 \, \text{g} in the time-period calculation. This is wrong because for SHM inside a uniform sphere, the acceleration is independent of the particle mass. Use T=2πRgT = 2\pi\sqrt{\frac{R}{g}} only.

  • Assuming the gravitational field inside the Earth is constant and equal to surface gravity everywhere. This is wrong because inside a uniform sphere the field varies linearly with displacement from the centre. Use the restoring acceleration proportional to xx.

  • Using the outside-Earth gravitational formula directly for the entire motion. That formula applies outside or at the surface, not inside the sphere. For motion through the tunnel, use the inside-sphere relation axa \propto -x.

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