Solveeit Logo

Question

Question: If \( {T_1} \) , \( {T_2} \) and \( {T_3} \) are the time periods of a given simple pendulum on the ...

If T1{T_1} , T2{T_2} and T3{T_3} are the time periods of a given simple pendulum on the surface of the earth, at a depth of hh in a mine and at an altitude hh above the earth’s surface respectively, then
(A) T1=T2=T3{T_1} = {T_2} = {T_3}
(B) T2<T1>T3{T_2} < {T_1} > {T_3}
(C) T2>T1<T3{T_2} > {T_1} < {T_3}
(D) T1>T2>T3{T_1} > {T_2} > {T_3}

Explanation

Solution

Hint
The time period of oscillation of a pendulum is given by the formula, T=2πlgT = 2\pi \sqrt {\dfrac{l}{g}} . So when the value of gg changes with the altitude or the depth, the time period of oscillation changes accordingly. Therefore, the time period of oscillation changes with change in gg .
Formula used: T=2πlgT = 2\pi \sqrt {\dfrac{l}{g}}
where TT is the time period of oscillation of the pendulum, ll is the length of the pendulum and gg is the acceleration due to gravity.
gh=g(RR+h)2{g_h} = g{\left( {\dfrac{R}{{R + h}}} \right)^2} where gh{g_h} is the acceleration due to gravity at height hh , RR is the radius of earth and hh is the height above the earth’s surface.
and gd=g(1dR){g_d} = g\left( {1 - \dfrac{d}{R}} \right) where gd{g_d} is the acceleration due to gravity at depth dd .

Complete step by step answer
The acceleration due to gravity is the acceleration that is gained by a freely falling object due to the gravitational force on earth. It is denoted by the symbol gg and has a value 9.8m/s29.8m/{s^2} . The value of acceleration due to gravity is constant all over the surface of the earth but changes with the increase in altitude over the earth’s surface or the increase in depth below the earth’s surface. In the question, the time period of a pendulum is given T1{T_1} , T2{T_2} and T3{T_3} on the surface of the earth, at a depth of dd in a mine and an altitude hh above the earth’s surface respectively.
For a pendulum on the earth’s surface, the time period is given by T1=2πlg{T_1} = 2\pi \sqrt {\dfrac{l}{g}} .
Therefore, T11g{T_1} \propto \dfrac{1}{{\sqrt g }} .
The change in the value of gg due to depth is given by gd=g(1dR){g_d} = g\left( {1 - \dfrac{d}{R}} \right) .
So, as the depth below the earth’s surface increases, the value of dd increases. Since the value (1dR)\left( {1 - \dfrac{d}{R}} \right) is always less than 1, by multiplying gg with a value less than 1, the value gd{g_d} becomes less than gg .
Hence, the time period of the pendulum at depth dd is
T2=2πlgd{T_2} = 2\pi \sqrt {\dfrac{l}{{{g_d}}}}
T21gd\therefore {T_2} \propto \dfrac{1}{{\sqrt {{g_d}} }}
Since gd<g{g_d} < g ,
1gd>1g\therefore \dfrac{1}{{{g_d}}} > \dfrac{1}{g}
So we get T2>T1\therefore {T_2} > {T_1}
The change in the value of gg due to altitude is given by gh=g(RR+h)2{g_h} = g{\left( {\dfrac{R}{{R + h}}} \right)^2} .
As the altitude above the earth’s surface increases, the value of hh increases. Therefore, the value of the fraction RR+h\dfrac{R}{{R + h}} becomes less than 1 as the value of the denominator in more than the numerator. So, by multiplying gg with a value less than 1, the value of gh{g_h} becomes less than gg .
Hence, the time period of the pendulum at an altitude hh is
T3=2πlgh{T_3} = 2\pi \sqrt {\dfrac{l}{{{g_h}}}}
T31gh\therefore {T_3} \propto \dfrac{1}{{\sqrt {{g_h}} }}
Since gh<g{g_h} < g ,
1gh>1g\therefore \dfrac{1}{{{g_h}}} > \dfrac{1}{g}
So, we get T3>T1\therefore {T_3} > {T_1}
Therefore, we have obtained, T2>T1{T_2} > {T_1} and T3>T1{T_3} > {T_1} . Combining we get, T2>T1<T3{T_2} > {T_1} < {T_3}.
Hence, option (C) is correct.

Note
As we increase the altitude above the earth’s surface the value of acceleration due to gravity decreases because the distance from the center of the earth increases. And as we do down a depth from the surface of the earth, then the total mass enclosed within that radius decreases and so the gravity decreases.