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Concepts Of Physics MCQ Edition [Volume 1]
Exam
Concepts Of Physics MCQ Edition [Volume 1]
Subject
Physics
Chapter
Simple Harmonic Motion

Concepts Of Physics MCQ Edition [Volume 1] · Physics · Simple Harmonic Motion

Suppose a tunnel is excavated along a chord of the earth at a...

Suppose a tunnel is excavated along a chord of the earth at a perpendicular distance R/2R/2 from the earth's centre, where RR is the radius of the earth. The wall of the tunnel is frictionless. A particle of mass mm is placed in the tunnel at a distance xx from the centre of the tunnel. Find the magnitudes of the components of the earth's gravitational force on the particle along the tunnel and perpendicular to the tunnel, respectively.

Options

  1. AGMmR3x\dfrac{GMm}{R^3} x, GMmR3x2+R24\dfrac{GMm}{R^3} \sqrt{x^2 + \dfrac{R^2}{4}}
  2. BGMmR2x\dfrac{GMm}{R^2} x, GMm2R3\dfrac{GMm}{2R^3}
  3. CGMmR3x\dfrac{GMm}{R^3} x, GMm2R2\dfrac{GMm}{2R^2}
  4. DGMm2R2\dfrac{GMm}{2R^2}, GMmR3x\dfrac{GMm}{R^3} x

Correct answer

C. GMmR3x\dfrac{GMm}{R^3} x, GMm2R2\dfrac{GMm}{2R^2}

Step-by-step solution

Let the centre of the earth be the origin (0,0)(0,0). Let the tunnel be parallel to the x-axis at a perpendicular distance y=R2y = \dfrac{R}{2}.

The position vector of the particle at a distance xx from the centre of the tunnel is given by r⃗=xi^+R2j^\vec{r} = x \hat{i} + \dfrac{R}{2} \hat{j}.

The gravitational force on a particle of mass mm inside the earth at a position vector r⃗\vec{r} from the centre is directed towards the centre and is given by:

F⃗=−GMmR3r⃗\vec{F} = -\dfrac{GMm}{R^3} \vec{r}

Substituting the position vector r⃗\vec{r} into the force equation, we get:

\vec{F} = -\dfrac{GMm}{R^3} \left( x \hat{i} +\dfrac{R}{2} \hat{j} \right)

F⃗=\vec{F} =-\dfrac{GMm}{R^3}xi^−x \hat{i} -\dfrac{GMm}{2R^2} \hat{j}

The magnitude of the component of the force along the tunnel (x-direction) is:

F∥=F_{\parallel} =\dfrac{GMm}{R^3}xx

The magnitude of the component of the force perpendicular to the tunnel (y-direction) is:

F⊥=F_{\perp} =\dfrac{GMm}{2R^2}
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