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Important Terms In Simple Harmonic Motion MCQ - Practice Questions with Answers

Edited By admin | Updated on Sep 25, 2023 25:23 PM | #NEET

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  • Terms associated with SHM is considered one of the most asked concept.

  • 21 Questions around this concept.

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The correct figure that shows, schematically , the wave pattern produced by the superposition of two waves of frequencies 9 Hz and 11 Hz, is: 

 

Two simple harmonic motions are represented by the equations y_{1}= 0.1\sin \left ( 100\pi t+\frac{\pi }{3} \right )\: and \: y_{2}= 0.1\cos \pi t.

The phase difference of the velocity of particle 1 with respect to the velocity of particle 2 at t=0 is:

A point mass oscillates along the x-axis according to law x= x_{0}\cos \left ( \omega t-\pi /4 \right ). If the acceleration of the particle is written as a= A\cos \left ( \omega t+\delta \right ) then

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Terms associated with SHM
  1. Amplitude:- 

We know that displacement of a particle in SHM is given by:

x=A Sin(\omega t+\phi )

The quantity A is called the amplitude of the motion. It is a positive constant which represents the magnitude of the maximum displacement of the particle from mean position in either direction.

  1. Time period:-

  • In SHM, a particle repeats its motion after a fixed interval of time. And this time interval after which the particle repeats its motion is called time period. It is denoted by T.
  • Time period is also defined as the time taken to complete one oscillation. And after one time period, both displacement and velocity of the particle are repeated.
  • We know that:-

x=A Sin(\omega t+\phi )

If a motion is periodic with a period T, then the displacement x (t) must return to its initial value after one period of the motion; that is, x (t) must be equal to x (t + T ) for all t and velocity v(t) must also return to its initial value, i.e., v(t) must be equal to v(t+T). So,

x(t)=x(t+T)

\Rightarrow A Sin(\omega t+\phi)=ASin[\omega [t+T]+\phi]

\Rightarrow Sin(\omega t+\phi)=Sin[\omega [t+T]+\phi]

And

v(t)=v(t+T)

\Rightarrow A \omega Cos(\omega t+\phi)=A\omega Cos[\omega [t+T]+\phi]

\Rightarrow Cos(\omega t+\phi)=Cos[\omega [t+T]+\phi]

As we know both Sine and Cosine function repeats itself when their argument increases by 2π,i.e.,

\omega t+\phi+2\pi=\omega (t+T)+\phi

\Rightarrow 2\pi=T\omega

\\\Rightarrow T=\frac{2\pi}{\omega}=2\pi \sqrt\frac{m}{k}; \\ where\ k=force\ or\ spring\ constant\ and\ m=mass

  • Time period can also be written as:-

T=\frac{2\pi}{\omega}=2\pi \sqrt\frac{m}{k}=2\pi \sqrt \frac{m}{\frac{Force}{displacement}}=2\pi \sqrt \frac{m \times displacement}{m \times acceleration}

\Rightarrow T=2\pi \sqrt \frac{displacement}{acceleration}

  1. Frequency:-

The reciprocal of T gives the number of repetitions that occur per unit time. This quantity is called the frequency of the periodic motion.

  • It is denoted by f.

f=\frac{1}{T}=\frac{\omega}{2\pi}=\frac{1}{2\pi} \sqrt \frac{k}{m}

\Rightarrow \omega=2\pi f;\ where\ \omega\ is\ angular\ frequency

  • The unit of frequency is or Hertz(Hz).

  1. Phase:-

  • The\ quantity\ (\omega t+\Delta \phi)\ is\ called\ the\ phase.
  • It determines the status of the particle in simple harmonic motion.
  • If the phase is zero at a certain instant, then:

x=A\ Sin(\omega t+\phi)=0\ and\ v=A\omega \ Cos(\omega t+\phi)=A\omega

which means that the particle is crossing the mean position and is going towards the positive direction. 

               

             Fig:- Status of the particle at different phases

  1. Phase constant:-

  • The constant \phi  is called the phase constant (or phase angle). 

  • The value of \phi depends on the displacement and velocity of the particle at t = 0 or we can say the phase constant signifies the initial conditions.

  • Any instant can be chosen as t = 0 and hence the phase constant can be chosen arbitrarily.

 

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Terms associated with SHM

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Terms associated with SHM

Physics Part II Textbook for Class XI

Page No. : 345

Line : 7

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