Question

Two simple harmonic motions given by,
$$x = a\sin \left( {\omega t + \delta } \right)$$    and $$y = a\sin $$
$$\left( {\omega t + \delta + \frac{\pi }{2}} \right)$$   act on a particle simultaneously, then the motion of particle will be

A. circular anti-clockwise
B. circular clockwise  
C. elliptical anti-clockwise
D. elliptical clockwise
Answer :   circular clockwise
Solution :
Two simple harmonic motions can be written as
$$\eqalign{ & x = a\sin \left( {\omega t + \delta } \right)\,......\left( {\text{i}} \right) \cr & {\text{and}}\,\,y = a\sin \left( {\omega t + \delta + \frac{\pi }{2}} \right) \cr & {\text{or}}\,\,y = a\cos \left( {\omega t + \delta } \right)\,......\left( {{\text{ii}}} \right) \cr} $$
Squaring and adding Eqs. (i) and (ii), we obtain
$$\eqalign{ & {x^2} + {y^2} = {a^2}\left[ {{{\sin }^2}\left( {\omega t + \delta } \right) + {{\cos }^2}\left( {\omega t + \delta } \right)} \right] \cr & {\text{or}}\,\,{x^2} + {y^2} = {a^2}\,\,\left( {\because {{\sin }^2}\theta + {{\cos }^2}\theta = 1} \right) \cr} $$
This is the equation of a circle.
$$\eqalign{ & {\text{At}}\,\,\left( {\omega t + \delta } \right) = 0;x = 0,y = a \cr & {\text{At}}\,\,\left( {\omega t + \delta } \right) = \frac{\pi }{2};x = a,y = 0 \cr & {\text{At}}\,\,\left( {\omega t + \delta } \right) = \pi ;x = 0,y = - a \cr & {\text{At}}\,\,\left( {\omega t + \delta } \right) = \frac{{3\pi }}{2};x = - a,y = 0 \cr & {\text{At}}\,\,\left( {\omega t + \delta } \right) = 2\pi ;x = 0,y = a \cr} $$
Simple Harmonic Motion (SHM) mcq solution image
Thus, it is obvious that motion of particle is traversed in clockwise direction.

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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