Question

A mass $$m$$ is suspended from the two coupled springs connected in series. The force constant for springs are $${k_1}$$ and $${k_2}.$$ The time period of the suspended mass will be

A. $$T = 2\pi \sqrt {\frac{m}{{{k_1} - {k_2}}}} $$
B. $$T = 2\pi \sqrt {\frac{{m{k_1}{k_2}}}{{{k_1} + {k_2}}}} $$
C. $$T = 2\pi \sqrt {\frac{m}{{{k_1} + {k_2}}}} $$
D. $$T = 2\pi \sqrt {\frac{{m\left( {{k_1} + {k_2}} \right)}}{{{k_1}{k_2}}}} $$  
Answer :   $$T = 2\pi \sqrt {\frac{{m\left( {{k_1} + {k_2}} \right)}}{{{k_1}{k_2}}}} $$
Solution :
Derive an expression from the given values which must be similar to $$a = - {\omega ^2}x.$$   Then calculate time period from the values in place of $$\omega .$$
Simple Harmonic Motion (SHM) mcq solution image
The situation is shown in figure. Consider two springs of spring constants $${k_1}$$ and $${k_2}.$$ Here, the body of weight $$mg$$  is suspended at the free end of the two springs in series combination. When the body is pulled downwards through a little distance $$y,$$ the two springs suffer different extensions say $${y_1}$$ and $${y_2}.$$ But the restoring force is same in each spring.
$$\eqalign{ & \therefore F = - {k_1}{y_1} \cr & {\text{and}}\,\,F = - {k_2}{y_2} \cr & {\text{or}}\,\,{y_1} = - \frac{F}{{{k_1}}} \cr & {\text{and}}\,\,{y_2} = - \frac{F}{{{k_2}}} \cr} $$
$$\therefore $$ Total extension, $$y = {y_1} + {y_2}$$
$$\eqalign{ & = - \frac{F}{{{k_1}}} - \frac{F}{{{k_2}}} \cr & = - F\left( {\frac{{{k_1} + {k_2}}}{{{k_1}{k_2}}}} \right) \cr & {\text{or}}\,\,F = - \left( {\frac{{{k_1}{k_2}}}{{{k_1} + {k_2}}}} \right)y \cr} $$
If $$k$$ is the spring constant of series combination of springs then $$F = - ky$$
$$\therefore k = \frac{{{k_1}{k_2}}}{{{k_1} + {k_2}}}$$
If the body is left free after pulling down, it will execute $$SHM$$  of period
$$\eqalign{ & T = 2\pi \sqrt {\frac{m}{k}} \cr & = 2\pi \sqrt {\frac{{m\left( {{k_1} + {k_2}} \right)}}{{{k_1}{k_2}}}} \cr} $$

Releted MCQ Question on
Oscillation and Mechanical Waves >> Simple Harmonic Motion (SHM)

Releted Question 1

Two bodies $$M$$ and $$N$$ of equal masses are suspended from two separate massless springs of spring constants $${k_1}$$ and $${k_2}$$ respectively. If the two bodies oscillate vertically such that their maximum velocities are equal, the ratio of the amplitude of vibration of $$M$$ to that of $$N$$ is

A. $$\frac{{{k_1}}}{{{k_2}}}$$
B. $$\sqrt {\frac{{{k_1}}}{{{k_2}}}} $$
C. $$\frac{{{k_2}}}{{{k_1}}}$$
D. $$\sqrt {\frac{{{k_2}}}{{{k_1}}}} $$
Releted Question 2

A particle free to move along the $$x$$-axis has potential energy given by $$U\left( x \right) = k\left[ {1 - \exp \left( { - {x^2}} \right)} \right]$$      for $$ - \infty \leqslant x \leqslant + \infty ,$$    where $$k$$ is a positive constant of appropriate dimensions. Then

A. at points away from the origin, the particle is in unstable equilibrium
B. for any finite nonzero value of $$x,$$ there is a force directed away from the origin
C. if its total mechanical energy is $$\frac{k}{2},$$  it has its minimum kinetic energy at the origin.
D. for small displacements from $$x = 0,$$  the motion is simple harmonic
Releted Question 3

The period of oscillation of a simple pendulum of length $$L$$ suspended from the roof of a vehicle which moves without friction down an inclined plane of inclination $$\alpha ,$$ is given by

A. $$2\pi \sqrt {\frac{L}{{g\cos \alpha }}} $$
B. $$2\pi \sqrt {\frac{L}{{g\sin \alpha }}} $$
C. $$2\pi \sqrt {\frac{L}{g}} $$
D. $$2\pi \sqrt {\frac{L}{{g\tan \alpha }}} $$
Releted Question 4

A particle executes simple harmonic motion between $$x = - A$$  and $$x = + A.$$  The time taken for it to go from 0 to $$\frac{A}{2}$$ is $${T_1}$$ and to go from $$\frac{A}{2}$$ to $$A$$ is $${T_2.}$$ Then

A. $${T_1} < {T_2}$$
B. $${T_1} > {T_2}$$
C. $${T_1} = {T_2}$$
D. $${T_1} = 2{T_2}$$

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Simple Harmonic Motion (SHM)


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