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Question: Two dissimilar spring fixed at one end are stretched by 10cm and 20cm respectively, when mass \({{m}...

Two dissimilar spring fixed at one end are stretched by 10cm and 20cm respectively, when mass m1{{m}_{1}} and m2{{m}_{2}} are suspended at their lower ends. When displaced slightly from their mean positions and released, they will oscillate with period in the ratio
A. 1:21 : 2
B. 2:12 : 1
C. 1:1.411 : 1.41
D. 1.41:41.41 : 4

Explanation

Solution

In this case, the gravitational force acting on the masses will be equal to the spring force acting on each of the masses. Equate the two forces for both the spring mass system and use the formula for the time period of a hanging spring mass system.

Formula used:
T=2πmkT=2\pi \sqrt{\dfrac{m}{k}}
Fg=mg{{F}_{g}}=mg
Fs=kx{{F}_{s}}=kx
Where kk is the spring constant of the spring, gg is acceleration due to gravity, mm is the mass of the spring and xx be the extension in the spring.

Complete step by step answer:
The time period of a hanging spring block system is given to be equal to T=2πmkT=2\pi \sqrt{\dfrac{m}{k}}, where m is the mass of the block and k is the spring constant of the spring. It is said that when the masses m1{{m}_{1}} and m2{{m}_{2}} are suspended at the lower ends of the two springs, the springs are displaced by 10 cm and 20 cm respectively.
This is due to the gravitational force acting (in the downward direction) on the two masses. When the springs are displaced by the said amounts, the spring force exerted by the spring is equal in magnitude but opposite in direction to the gravitational force.
i.e. Fg=Fs{{F}_{g}}={{F}_{s}}.
The gravitational force acting on a mass m is given as Fg=mg{{F}_{g}}=mg, where g is acceleration due to gravity. When the spring is stretched by a length x, then the spring force acting on the mass is equal to Fs=kx{{F}_{s}}=kx.
Therefore, the gravitational force on mass m1{{m}_{1}} is equal to Fg,1=m1g{{F}_{g,1}}={{m}_{1}}g.
And the spring force acting on this mass is Fs,1=k1x1=k1(10){{F}_{s,1}}={{k}_{1}}{{x}_{1}}={{k}_{1}}(10).
But we know that Fg,1=Fs,1{{F}_{g,1}}={{F}_{s,1}}.
m1g=10k1\Rightarrow {{m}_{1}}g=10{{k}_{1}}
k1=m1g10\Rightarrow {{k}_{1}}=\dfrac{{{m}_{1}}g}{10}.
Therefore, the time period of the first spring is,
T1=2πm1k1 T1=2πm1m1g10{{T}_{1}}=2\pi \sqrt{\dfrac{{{m}_{1}}}{{{k}_{1}}}}\\\ \Rightarrow {{T}_{1}} =2\pi \sqrt{\dfrac{{{m}_{1}}}{\dfrac{{{m}_{1}}g}{10}}}.
T1=2π10g\Rightarrow {{T}_{1}}=2\pi \sqrt{\dfrac{10}{g}} ….. (i)
Similarly, the gravitational force on the mass m1{{m}_{1}} is equal to Fg,2=m2g{{F}_{g,2}}={{m}_{2}}g.
And the spring force acting on this mass is Fs,2=k2x2=k2(20){{F}_{s,2}}={{k}_{2}}{{x}_{2}}={{k}_{2}}(20).
But we know that Fg,2=Fs,2{{F}_{g,2}}={{F}_{s,2}}.
m2g=20k2\Rightarrow {{m}_{2}}g=20{{k}_{2}}
k2=m2g20\Rightarrow {{k}_{2}}=\dfrac{{{m}_{2}}g}{20}.
Therefore, the time period of the second spring is T2=2πm2k2=2πm2m2g20{{T}_{2}}=2\pi \sqrt{\dfrac{{{m}_{2}}}{{{k}_{2}}}}=2\pi \sqrt{\dfrac{{{m}_{2}}}{\dfrac{{{m}_{2}}g}{20}}}.
T2=2π20g\Rightarrow {{T}_{2}}=2\pi \sqrt{\dfrac{20}{g}} …. (ii).
Now, divide (i) by (ii).
T1T2=2π10g2π20g\dfrac{{{T}_{1}}}{{{T}_{2}}}=\dfrac{2\pi \sqrt{\dfrac{10}{g}}}{2\pi \sqrt{\dfrac{20}{g}}}
T1T2=1020 T1T2=12 T1T2=11.41\Rightarrow \dfrac{{{T}_{1}}}{{{T}_{2}}}=\sqrt{\dfrac{10}{20}}\\\ \Rightarrow \dfrac{{{T}_{1}}}{{{T}_{2}}} =\dfrac{1}{\sqrt{2}}\\\ \therefore \dfrac{{{T}_{1}}}{{{T}_{2}}} =\dfrac{1}{1.41}.
This means that the ratio of the time period of the first spring to the second spring is equal to 1 : 1.41.

Hence, the correct option is C.

Note: There can be some misconception that the time period of oscillations of a spring block system will depend on the amplitude of the oscillations. However, the time period is independent of the amplitude of the oscillations. This means that for a given spring block system, the time period remains the same for every value of amplitude.