Question

A particle moves with simple harmonic motion in a straight line. In first $$\tau s,$$ after starting from rest it travels a distance $$a,$$ and in next $$\tau s$$ it travels $$2a,$$ in same direction, then:

A. amplitude of motion is $$3a$$
B. time period of oscillations is 8$$\tau $$
C. amplitude of motion is $$4a$$
D. time period of oscillations is 6$$\tau $$  
Answer :   time period of oscillations is 6$$\tau $$
Solution :
In simple harmonic motion, starting from rest,
At $$t = 0,x = A$$
$$x = A\cos \omega t\,......\left( {\text{i}} \right)$$
When $$t = \tau ,x = A - a$$
When $$t = 2\tau ,x = A - 3a$$
From equation (i)
$$\eqalign{ & A - a = A\cos \omega \tau \,......\left( {{\text{ii}}} \right) \cr & A - 3a = A\cos 2\omega \tau \,......\left( {{\text{iii}}} \right) \cr & \cos 2\omega \tau = 2{\cos ^2}\omega \tau - 1......\left( {{\text{iv}}} \right) \cr} $$
From equation (ii), (iii) and (iv)
$$\eqalign{ & \frac{{A - 3a}}{A} = 2{\left( {\frac{{A - a}}{A}} \right)^2} - 1 \cr & \Rightarrow \frac{{A - 3a}}{A} = \frac{{2{A^2} + 2{a^2} - 4Aa - {A^2}}}{{{A^2}}} \cr & \Rightarrow {A^2} - 3aA = {A^2} + 2{a^2} - 4Aa \cr & \Rightarrow 2{a^2} = aA \Rightarrow A = 2a \cr & \Rightarrow \frac{a}{A} = \frac{1}{2} \cr & {\text{Now,}}\,A - a = A\cos \omega \tau \cr & \Rightarrow \cos \omega \tau = \frac{{A - a}}{A} \Rightarrow \cos \omega \tau = \frac{1}{2} \cr & {\text{or,}}\,\frac{{2\pi }}{T}\tau = \frac{\pi }{3} \Rightarrow T = 6\tau \cr} $$

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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