Calculate the time period of a simple pendulum of length $1.12m,$ when acceleration due to gravity is $9.8m{s^{ - 2}}.$
A. $0$
B. $1.2$
C. $2.12$
D. $4.24$
Answer
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Hint: 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$ = 2\pi \sqrt {\dfrac{\ell }{g}} $
Where $\ell $the length of the pendulum and g is acceleration due to gravity.
Complete step by step answer:
An ideal simple pendulum consists of a point mass suspended by a flexible, inelastic and weightless string of rigid support of infinite mass.
We know that in SHM, the equation is given
a$ = - {\omega ^2}x\,\,..........\left( 1 \right)$
And Time period, $T = \dfrac{{2\pi }}{\omega }.........\left( 2 \right)$
Where a is the acceleration
$\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\[ = \dfrac{{ - gx}}{\ell }\,..........\left( 3 \right)\]
Where $\ell $is length of pendulum
On comparing (1) and (3), we have
${\omega ^2} = \dfrac{g}{\ell }$
$ \implies \omega = \sqrt {\dfrac{g}{\ell }} $
So, Time period, $T = \dfrac{{2\pi }}{\omega } = 2\pi \sqrt {\dfrac{\ell }{g}} $
Here, length of pendulum is given to be
$\ell = 1.12m$
So, Time period becomes
$T = 2\pi \sqrt {\dfrac{{1.12}}{{9.8}}} $
$ \implies T = 2 \times \dfrac{{22}}{7}\sqrt {\dfrac{{1.12}}{{9.8}}} \,\,\,\,\,\,\,\,\,\left( {as\,\,\pi = \dfrac{{22}}{7}} \right)$
$\implies T = \dfrac{{44}}{7} \times \sqrt {0.114} $
$\implies T = \dfrac{{44}}{7} \times 0.338$
So, \[T = 2.12\sec \]
Therefore, Time period of simple pendulum is $2.12\sec $
So, the correct answer is “Option C”.
Note:
Remember that simple pendulum performs SHM can be made clear from its equation $a = \dfrac{{ - g}}{\ell }x.$ 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.
Time period of a simple pendulum is T$ = 2\pi \sqrt {\dfrac{\ell }{g}} $
Where $\ell $the length of the pendulum and g is acceleration due to gravity.
Complete step by step answer:
An ideal simple pendulum consists of a point mass suspended by a flexible, inelastic and weightless string of rigid support of infinite mass.
We know that in SHM, the equation is given
a$ = - {\omega ^2}x\,\,..........\left( 1 \right)$
And Time period, $T = \dfrac{{2\pi }}{\omega }.........\left( 2 \right)$
Where a is the acceleration
$\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\[ = \dfrac{{ - gx}}{\ell }\,..........\left( 3 \right)\]
Where $\ell $is length of pendulum
On comparing (1) and (3), we have
${\omega ^2} = \dfrac{g}{\ell }$
$ \implies \omega = \sqrt {\dfrac{g}{\ell }} $
So, Time period, $T = \dfrac{{2\pi }}{\omega } = 2\pi \sqrt {\dfrac{\ell }{g}} $
Here, length of pendulum is given to be
$\ell = 1.12m$
So, Time period becomes
$T = 2\pi \sqrt {\dfrac{{1.12}}{{9.8}}} $
$ \implies T = 2 \times \dfrac{{22}}{7}\sqrt {\dfrac{{1.12}}{{9.8}}} \,\,\,\,\,\,\,\,\,\left( {as\,\,\pi = \dfrac{{22}}{7}} \right)$
$\implies T = \dfrac{{44}}{7} \times \sqrt {0.114} $
$\implies T = \dfrac{{44}}{7} \times 0.338$
So, \[T = 2.12\sec \]
Therefore, Time period of simple pendulum is $2.12\sec $
So, the correct answer is “Option C”.
Note:
Remember that simple pendulum performs SHM can be made clear from its equation $a = \dfrac{{ - g}}{\ell }x.$ 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.
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