JEE Challenger
More from Oscillations

Match Periodic Functions with Time Period and SHM Behavior

Match List - I with List - II.

List - IList - IIA.sin2ωtI.Periodic with time period T=πω but not simple harmonic motion (SHM)B.sin3(2ωt)II.Periodic with time period T=2πω but Not SHMC.sin(ωt)+cos(πωt)III.Periodic with time period T=πω and SHMD.cosωt+cos2ωtIV.Non-periodic\begin{array}{clcl} \text{List - I} & & \text{List - II} & \\ A. & \sin^2 \omega t & I. & \text{Periodic with time period } T=\frac{\pi}{\omega} \text{ but not simple harmonic motion (SHM)} \\ B. & \sin^3(2\omega t) & II. & \text{Periodic with time period } T=\frac{2\pi}{\omega} \text{ but Not SHM} \\ C. & \sin(\omega t) + \cos(\pi \omega t) & III. & \text{Periodic with time period } T=\frac{\pi}{\omega} \text{ and SHM} \\ D. & \cos \omega t + \cos 2\omega t & IV. & \text{Non-periodic} \end{array}

Choose the correct answer from the options given below :

Options

A

A-III, B-I, C-IV, D-II

Correct
B

A-II, B-I, C-III, D-IV

C

A-III, B-II, C-IV, D-I

D

A-II, B-I, C-IV, D-III

Topics & Concepts

OscillationsSHM

Step-by-Step Solution

To determine the correct match between List - I and List - II, we analyze each function given in List - I:

1. Analysis of Function A: y=sin2ωty = \sin^2 \omega t

Using the trigonometric power-reduction identity, we can rewrite yy as: y=1cos(2ωt)2=1212cos(2ωt)y = \frac{1 - \cos(2\omega t)}{2} = \frac{1}{2} - \frac{1}{2}\cos(2\omega t)

Differentiating with respect to time tt: dydt=ωsin(2ωt)\frac{dy}{dt} = \omega \sin(2\omega t) d2ydt2=2ω2cos(2ωt)\frac{d^2 y}{dt^2} = 2\omega^2 \cos(2\omega t)

Since cos(2ωt)=12y\cos(2\omega t) = 1 - 2y, substituting this back gives: d2ydt2=2ω2(12y)=4ω2(y12)\frac{d^2 y}{dt^2} = 2\omega^2 (1 - 2y) = -4\omega^2 \left(y - \frac{1}{2}\right)

This differential equation is of the standard SHM form d2ydt2=ω2(yy0)\frac{d^2 y}{dt^2} = -\omega'^2 (y - y_0) where ω=2ω\omega' = 2\omega and the mean position is y0=12y_0 = \frac{1}{2}.

Thus, the motion is Simple Harmonic Motion (SHM) with a time period: T=2πω=2π2ω=πωT = \frac{2\pi}{\omega'} = \frac{2\pi}{2\omega} = \frac{\pi}{\omega}

Hence, A matches with III.


2. Analysis of Function B: y=sin3(2ωt)y = \sin^3(2\omega t)

Using the identity sin(3θ)=3sinθ4sin3θ\sin(3\theta) = 3\sin\theta - 4\sin^3\theta, we get: sin3θ=3sinθsin(3θ)4\sin^3\theta = \frac{3\sin\theta - \sin(3\theta)}{4}

For θ=2ωt\theta = 2\omega t: y=34sin(2ωt)14sin(6ωt)y = \frac{3}{4}\sin(2\omega t) - \frac{1}{4}\sin(6\omega t)

This is a linear combination of two harmonic functions with different angular frequencies (ω1=2ω\omega_1 = 2\omega and ω2=6ω\omega_2 = 6\omega). Because it contains multiple frequencies, it cannot be represented as a single sine or cosine term, so it is not SHM.

The fundamental angular frequency is ω0=gcd(2ω,6ω)=2ω\omega_0 = \text{gcd}(2\omega, 6\omega) = 2\omega. The time period of the periodic motion is: T=2πω0=2π2ω=πωT = \frac{2\pi}{\omega_0} = \frac{2\pi}{2\omega} = \frac{\pi}{\omega}

Hence, B matches with I.


3. Analysis of Function C: y=sin(ωt)+cos(πωt)y = \sin(\omega t) + \cos(\pi \omega t)

The angular frequencies of the two constituent waves are: ω1=ωandω2=πω\omega_1 = \omega \quad \text{and} \quad \omega_2 = \pi \omega

Taking their ratio: ω1ω2=ωπω=1π\frac{\omega_1}{\omega_2} = \frac{\omega}{\pi \omega} = \frac{1}{\pi}

Since 1π\frac{1}{\pi} is an irrational number, there exists no common time period TT such that y(t+T)=y(t)y(t+T) = y(t) for all tt. Therefore, the function is non-periodic.

Hence, C matches with IV.


4. Analysis of Function D: y=cosωt+cos2ωty = \cos \omega t + \cos 2\omega t

This function is a sum of two harmonic oscillations with angular frequencies ω1=ω\omega_1 = \omega and ω2=2ω\omega_2 = 2\omega. Since it contains more than one frequency, it is not SHM.

The ratio of frequencies ω1ω2=12\frac{\omega_1}{\omega_2} = \frac{1}{2} is a rational number, so the motion is periodic. The fundamental angular frequency is ω0=gcd(ω,2ω)=ω\omega_0 = \text{gcd}(\omega, 2\omega) = \omega.

The time period is: T=2πωT = \frac{2\pi}{\omega}

Hence, D matches with II.


Conclusion:

  • A \rightarrow III
  • B \rightarrow I
  • C \rightarrow IV
  • D \rightarrow II

This corresponds to Option A.

Match Periodic Functions with Time Period and SHM Behavior | Physics PYQ Solution - JEE Challenger