
A simple pendulum has a time period of $3.0{\rm{ s}}$. If the point of suspension of the pendulum starts moving vertically upward with a velocity $\upsilon = Kt$ where $K = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$, the new time period will be (Take $g = 10{\rm{ m}}{{\rm{s}}^{ - 2}}$)
(1) $\dfrac{9}{4}s$
(2) $\dfrac{5}{3}s$
(3) $2.5s$
(4) $4.4s$
Answer
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Hint:Hint: For a simple pendulum in an oscillating motion having the length of the string of the pendulum be $l$ and the mass of the bob be $m$, then the time period $T$ of the pendulum is given by this relation-
$T = 2\pi \sqrt {\dfrac{l}{g}} $
Where, $g$ is the acceleration due to gravity.
Complete step by step answer:
Given:
The time period of given simple pendulum at suspended position ${T_1} = 3.0{\rm{ s}}$
Also, from the formula for the time period of the pendulum we have,
${T_1} = 2\pi \sqrt {\dfrac{l}{g}} $
Substituting, ${T_1} = 3.0{\rm{ s}}$ and $g = 10{\rm{ m}}{{\rm{s}}^{ - 2}}$ in the formula we get,
$\begin{array}{l}
3.0 = 2\pi \sqrt {\dfrac{l}{{10}}} \\
\dfrac{{3.0}}{{2\pi }} = \sqrt {\dfrac{l}{{10}}}
\end{array}$
Squaring both sides and solving we get,
$\begin{array}{l}
{\left( {\dfrac{{3.0}}{{2\pi }}} \right)^2} = \dfrac{l}{{10}}\\
l = {\left( {\dfrac{{3.0}}{{2\pi }}} \right)^2} \times 10\\
l = 2.28{\rm{ m}}
\end{array}$
So, the length of the string of the pendulum is $2.28{\rm{ m}}$.
The expression for the upward velocity of the pendulum is given as-
$\upsilon = Kt$
Where, $K = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ and $t$ is the instantaneous time period.
Now, since the pendulum is moving upwards with a velocity $\upsilon $ the acceleration in this direction will be-
$a = \dfrac{{d\upsilon }}{{dt}}$
Substituting the value of $\upsilon $ in the expression we get,
$a = \dfrac{d}{{dt}}\left( {Kt} \right)$
We can write this as-
$\begin{array}{l}
a = K\dfrac{{dt}}{{dt}}\\
{\rm{or}}\\
a = K
\end{array}$
We know the value of $K$, so substituting $K = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ we get,
$a = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$
So, for this position of the pendulum the total effective acceleration due to gravity becomes, ${g_{eff}} = \left( {g + a} \right)$
We know that, $g = 10{\rm{ m}}{{\rm{s}}^{ - 2}}$ and $a = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$, substituting the value we get,
$\begin{array}{l}
{g_{eff}} = \left( {10 + 4.4} \right)\\
{g_{eff}} = 14.4{\rm{ m}}{{\rm{s}}^{ - 2}}
\end{array}$
Now using the formula for the new period of the pendulum we get,
${T_2} = 2\pi \sqrt {\dfrac{l}{{{g_{eff}}}}} $
Substituting the values $l = 2.28{\rm{ m}}$ and ${g_{eff}} = 14.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ in the formula we get,
$\begin{array}{l}
{T_2} = 2\pi \sqrt {\dfrac{{2.28}}{{14.4}}} \\
\Rightarrow {T_2} = 2\pi \times 0.398\\
\Rightarrow {T_2} = 2.5{\rm{ s}}
\end{array}$
Therefore, the new period of the pendulum is $2.5{\rm{ s}}$ and the correct answer is (3) $2.5s$
Note:It should be noted that the value of acceleration $a$ used in calculating the effective acceleration due to gravity ${g_{eff}}$ has same value of magnitude but the direction is opposite to the direction of motion of the pendulum i.e. the direction of $a$ is downwards.
$T = 2\pi \sqrt {\dfrac{l}{g}} $
Where, $g$ is the acceleration due to gravity.
Complete step by step answer:
Given:
The time period of given simple pendulum at suspended position ${T_1} = 3.0{\rm{ s}}$
Also, from the formula for the time period of the pendulum we have,
${T_1} = 2\pi \sqrt {\dfrac{l}{g}} $
Substituting, ${T_1} = 3.0{\rm{ s}}$ and $g = 10{\rm{ m}}{{\rm{s}}^{ - 2}}$ in the formula we get,
$\begin{array}{l}
3.0 = 2\pi \sqrt {\dfrac{l}{{10}}} \\
\dfrac{{3.0}}{{2\pi }} = \sqrt {\dfrac{l}{{10}}}
\end{array}$
Squaring both sides and solving we get,
$\begin{array}{l}
{\left( {\dfrac{{3.0}}{{2\pi }}} \right)^2} = \dfrac{l}{{10}}\\
l = {\left( {\dfrac{{3.0}}{{2\pi }}} \right)^2} \times 10\\
l = 2.28{\rm{ m}}
\end{array}$
So, the length of the string of the pendulum is $2.28{\rm{ m}}$.
The expression for the upward velocity of the pendulum is given as-
$\upsilon = Kt$
Where, $K = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ and $t$ is the instantaneous time period.
Now, since the pendulum is moving upwards with a velocity $\upsilon $ the acceleration in this direction will be-
$a = \dfrac{{d\upsilon }}{{dt}}$
Substituting the value of $\upsilon $ in the expression we get,
$a = \dfrac{d}{{dt}}\left( {Kt} \right)$
We can write this as-
$\begin{array}{l}
a = K\dfrac{{dt}}{{dt}}\\
{\rm{or}}\\
a = K
\end{array}$
We know the value of $K$, so substituting $K = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ we get,
$a = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$
So, for this position of the pendulum the total effective acceleration due to gravity becomes, ${g_{eff}} = \left( {g + a} \right)$
We know that, $g = 10{\rm{ m}}{{\rm{s}}^{ - 2}}$ and $a = 4.4{\rm{ m}}{{\rm{s}}^{ - 2}}$, substituting the value we get,
$\begin{array}{l}
{g_{eff}} = \left( {10 + 4.4} \right)\\
{g_{eff}} = 14.4{\rm{ m}}{{\rm{s}}^{ - 2}}
\end{array}$
Now using the formula for the new period of the pendulum we get,
${T_2} = 2\pi \sqrt {\dfrac{l}{{{g_{eff}}}}} $
Substituting the values $l = 2.28{\rm{ m}}$ and ${g_{eff}} = 14.4{\rm{ m}}{{\rm{s}}^{ - 2}}$ in the formula we get,
$\begin{array}{l}
{T_2} = 2\pi \sqrt {\dfrac{{2.28}}{{14.4}}} \\
\Rightarrow {T_2} = 2\pi \times 0.398\\
\Rightarrow {T_2} = 2.5{\rm{ s}}
\end{array}$
Therefore, the new period of the pendulum is $2.5{\rm{ s}}$ and the correct answer is (3) $2.5s$
Note:It should be noted that the value of acceleration $a$ used in calculating the effective acceleration due to gravity ${g_{eff}}$ has same value of magnitude but the direction is opposite to the direction of motion of the pendulum i.e. the direction of $a$ is downwards.
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