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Question: Calculate the time period of a simple pendulum of length \(1.12m,\) when acceleration due to gravity...

Calculate the time period of a simple pendulum of length 1.12m,1.12m, when acceleration due to gravity is 9.8ms2.9.8m{s^{ - 2}}.
A. 00
B. 1.21.2
C. 2.122.12
D. 4.244.24

Explanation

Solution

The time periodic of a simple pendulum and its dependence on length is to be used to solve this also the motion of a simple pendulum is SHM.
Time period of a simple pendulum is T=2πg= 2\pi \sqrt {\dfrac{\ell }{g}}
Where \ell the length of the pendulum and g is acceleration due to gravity.

Complete step by step answer:
An ideal simple pendulum consists of a point mass suspended by a flexible, inelastic and weightless string of rigid support of infinite mass.
We know that in SHM, the equation is given
a=ω2x..........(1) = - {\omega ^2}x\,\,..........\left( 1 \right)
And Time period, T=2πω.........(2)T = \dfrac{{2\pi }}{\omega }.........\left( 2 \right)
Where a is the acceleration
ω\omega is the angular frequency
x is displacement from mean position.
Now, as Simple pendulum also performs SHM and its equation is given by
a=gx..........(3) = \dfrac{{ - gx}}{\ell }\,..........\left( 3 \right)
Where \ell is length of pendulum
On comparing (1) and (3), we have
ω2=g{\omega ^2} = \dfrac{g}{\ell }
    ω=g\implies \omega = \sqrt {\dfrac{g}{\ell }}
So, Time period, T=2πω=2πgT = \dfrac{{2\pi }}{\omega } = 2\pi \sqrt {\dfrac{\ell }{g}}
Here, length of pendulum is given to be
=1.12m\ell = 1.12m
So, Time period becomes
T=2π1.129.8T = 2\pi \sqrt {\dfrac{{1.12}}{{9.8}}}
    T=2×2271.129.8(asπ=227)\implies T = 2 \times \dfrac{{22}}{7}\sqrt {\dfrac{{1.12}}{{9.8}}} \,\,\,\,\,\,\,\,\,\left( {as\,\,\pi = \dfrac{{22}}{7}} \right)
    T=447×0.114\implies T = \dfrac{{44}}{7} \times \sqrt {0.114}
    T=447×0.338\implies T = \dfrac{{44}}{7} \times 0.338
So, T=2.12secT = 2.12\sec
Therefore, Time period of simple pendulum is 2.12sec2.12\sec

So, the correct answer is “Option C”.

Note:
Remember that simple pendulum performs SHM can be made clear from its equation a=gx.a = \dfrac{{ - g}}{\ell }x. From this it is clear that acceleration is proportional to its displacement and is directed opposite to that of displacement which is nothing but SHM.