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Question: A' is a huge planet with uniform mass distribution, mass M, radius R. B is a circular tunnel made in...

A' is a huge planet with uniform mass distribution, mass M, radius R. B is a circular tunnel made in it, concentric with planet. Radius of tunnel is r,(r=R2)(r = \frac{R}{2}) cross sectional diameter is d (d << r). C is a small ball of mass m (m <<M) which is moving freely inside the tunnel without friction in a uniform circular motion, take acceleration due to gravity on surface of A as g:

A

If contact force on C is double the gravitational force, its time period =2πR3g2\pi \sqrt{\frac{R}{3g}}

B

If contact force on C is double the gravitational force, its time period =2πRg2\pi \sqrt{\frac{R}{g}}

C

If contact force is zero, time period T, radius of tunnel r, than TrT \propto r

D

If contact force is zero, time period T, radius of tunnel r, than T would be independent of r.

Answer

If contact force on C is double the gravitational force, its time period =2πR3g2\pi \sqrt{\frac{R}{3g}}

Explanation

Solution

The gravitational force on the ball C at a distance r from the center of the planet is given by Fg=GMmrR3F_g = \frac{GMmr}{R^3}. We are given that the acceleration due to gravity on the surface of the planet is g=GMR2g = \frac{GM}{R^2}. So, GM=gR2GM = gR^2.
The gravitational force can be written as Fg=gR2mrR3=mgrRF_g = \frac{gR^2 mr}{R^3} = \frac{mgr}{R}.
In this problem, the radius of the tunnel is r=R2r = \frac{R}{2}.
So, the gravitational force on the ball is Fg=mg(R/2)R=mg2F_g = \frac{m g (R/2)}{R} = \frac{mg}{2}. This force is directed towards the center of the planet.

The ball C is moving in a uniform circular motion inside the tunnel of radius r, concentric with the planet. The center of the circular motion is the center of the planet O. The radius of the circular motion is r. For uniform circular motion with speed v, the centripetal force required is Fc=mv2rF_c = \frac{mv^2}{r}, directed towards the center O.

The forces acting on the ball are the gravitational force FgF_g towards O and the contact force N from the tunnel wall. Since the ball is moving in a circular path of radius r around O, the contact force N must be radial. Let's assume the contact force N is positive when directed inwards.
The net force towards the center O is the sum of the gravitational force and the contact force (with appropriate sign).
Net force towards O = Fg+N=mv2rF_g + N = \frac{mv^2}{r}.
Here, FgF_g is always towards O. If N is inwards, it is positive. If N is outwards, it is negative.

Consider the first option: If contact force on C is double the gravitational force, its time period =2πR3g2\pi \sqrt{\frac{R}{3g}}.
Let N=2FgN = 2F_g. For the net force to be towards the center, the contact force must be directed inwards.
Net force towards O = Fg+N=Fg+2Fg=3FgF_g + N = F_g + 2F_g = 3F_g.
So, 3Fg=mv2r3F_g = \frac{mv^2}{r}.
3(mg2)=mv2r3 \left(\frac{mg}{2}\right) = \frac{mv^2}{r}.
3mg2=mv2r\frac{3mg}{2} = \frac{mv^2}{r}.
v2=3gr2v^2 = \frac{3gr}{2}.
The time period of uniform circular motion is T=2πrvT = \frac{2\pi r}{v}.
T2=4π2r2v2=4π2r2(3gr/2)=8π2r3gT^2 = \frac{4\pi^2 r^2}{v^2} = \frac{4\pi^2 r^2}{(3gr/2)} = \frac{8\pi^2 r}{3g}.
T=2π2r3gT = 2\pi \sqrt{\frac{2r}{3g}}.
We are given r=R2r = \frac{R}{2}. Substitute this into the expression for T:
T=2π2(R/2)3g=2πR3gT = 2\pi \sqrt{\frac{2(R/2)}{3g}} = 2\pi \sqrt{\frac{R}{3g}}.
This matches the first option.

Let's check the other options.
Option 2: If contact force on C is double the gravitational force, its time period =2πRg2\pi \sqrt{\frac{R}{g}}.
Our calculated time period is 2πR3g2\pi \sqrt{\frac{R}{3g}}. So, option 2 is incorrect.

Option 3: If contact force is zero, time period T, radius of tunnel r, than TrT \propto r.
If contact force N = 0, then the net force towards O is FgF_g.
Fg=mv2rF_g = \frac{mv^2}{r}.
mg2=mv2r\frac{mg}{2} = \frac{mv^2}{r}.
v2=gr2v^2 = \frac{gr}{2}.
The time period T=2πrv=2πrgr/2=2πr2gr=2π4π2r22gr=2π2rgT = \frac{2\pi r}{v} = \frac{2\pi r}{\sqrt{gr/2}} = 2\pi r \sqrt{\frac{2}{gr}} = 2\pi \sqrt{\frac{4\pi^2 r^2 \cdot 2}{gr}} = 2\pi \sqrt{\frac{2r}{g}}.
So, T=2π2rgT = 2\pi \sqrt{\frac{2r}{g}}.
This shows that TrT \propto \sqrt{r}. Option 3 states TrT \propto r, which is incorrect.

Option 4: If contact force is zero, time period T, radius of tunnel r, than T would be independent of r.
From the calculation in option 3, T=2π2rgT = 2\pi \sqrt{\frac{2r}{g}}, which clearly depends on r. So, option 4 is incorrect.

Therefore, only the first option is correct.