Answer
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Hint: In order to solve this question we need to understand hooke's law.According to hooke's law the force on a spring is constant and it is directly proportional to the displacement and acts opposite to it. Removing the proportionality, the magnitude of a force on mass attached with spring is equal to the product of stiffness or spring constant and displacement of body.
Complete step by step answer:
Consider a spring of spring constant “k” and let us assume that mass “m” is attached to its one end and also let the length of spring be $l$. Then the mass oscillates and its motion is known as simple harmonic motion. Let the time period of SHM be “T”. Then from formula of SHM we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
So, Magnitude of Force on spring when it is not cut, is
$\left| {\vec F} \right| = kl \to (i)$
So when the spring is cut into two equal parts, then the magnitude of force on one spring would be,
$\left| {\vec F'} \right| = k'\dfrac{l}{2} \to (ii)$
We know, force on spring on spring always remains constant, equating equation (i) and (ii) we get,
$kl = k'\dfrac{l}{2}$
$\Rightarrow k' = 2k$
(a) When the mass is suspended from one part, the new time period would be, $T' = 2\pi \sqrt {\dfrac{m}{{k'}}} $
Putting values we get,
$T' = \dfrac{1}{{\sqrt 2 }}(2\pi \sqrt {\dfrac{m}{k}} )$
Since we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
$\therefore T' = \dfrac{T}{{\sqrt 2 }}$
(b) When the two parts are connected in parallel, then net effective stiffness constant would be,
$k'' = k' + k'$
Putting values we get,
$k'' = 2k'$
$\Rightarrow k'' = 4k$
So the new time period would be,
$T'' = 2\pi \sqrt {\dfrac{m}{{k''}}} $
Putting values we get,
$T'' = 2\pi \sqrt {\dfrac{m}{{4k}}} $
$\Rightarrow T'' = \dfrac{1}{2}(2\pi \sqrt {\dfrac{m}{k}} )$
Since we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
$\therefore T'' = \dfrac{T}{2}$
So the correct option is D.
Note: It should be remembered that although the suspending force of gravity acts on mass, this would not change the time period of SHM as it is only a constant force. SHM motion is defined as Simple Harmonic Motion, in which a body oscillates with a time period and the force causing oscillation acts in the opposite direction of displacement.
Complete step by step answer:
Consider a spring of spring constant “k” and let us assume that mass “m” is attached to its one end and also let the length of spring be $l$. Then the mass oscillates and its motion is known as simple harmonic motion. Let the time period of SHM be “T”. Then from formula of SHM we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
So, Magnitude of Force on spring when it is not cut, is
$\left| {\vec F} \right| = kl \to (i)$
So when the spring is cut into two equal parts, then the magnitude of force on one spring would be,
$\left| {\vec F'} \right| = k'\dfrac{l}{2} \to (ii)$
We know, force on spring on spring always remains constant, equating equation (i) and (ii) we get,
$kl = k'\dfrac{l}{2}$
$\Rightarrow k' = 2k$
(a) When the mass is suspended from one part, the new time period would be, $T' = 2\pi \sqrt {\dfrac{m}{{k'}}} $
Putting values we get,
$T' = \dfrac{1}{{\sqrt 2 }}(2\pi \sqrt {\dfrac{m}{k}} )$
Since we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
$\therefore T' = \dfrac{T}{{\sqrt 2 }}$
(b) When the two parts are connected in parallel, then net effective stiffness constant would be,
$k'' = k' + k'$
Putting values we get,
$k'' = 2k'$
$\Rightarrow k'' = 4k$
So the new time period would be,
$T'' = 2\pi \sqrt {\dfrac{m}{{k''}}} $
Putting values we get,
$T'' = 2\pi \sqrt {\dfrac{m}{{4k}}} $
$\Rightarrow T'' = \dfrac{1}{2}(2\pi \sqrt {\dfrac{m}{k}} )$
Since we know,
$T = 2\pi \sqrt {\dfrac{m}{k}} $
$\therefore T'' = \dfrac{T}{2}$
So the correct option is D.
Note: It should be remembered that although the suspending force of gravity acts on mass, this would not change the time period of SHM as it is only a constant force. SHM motion is defined as Simple Harmonic Motion, in which a body oscillates with a time period and the force causing oscillation acts in the opposite direction of displacement.
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