Simple Harmonic Motion (Introduction)

Periodic Motion:

 (i) When a body moves on a definite path and repeats its motion again and again after a definite interval of time, then its motion is called periodic motion. 

The constant time interval after which it repeats its motion called its time period of motion, T.

         Example : Motion of earth around Sun ( T=365.25 days), Motion of minutes hand in clock (T= 1hour), Motio of a simple pendulum in free space, etc.

So, for motion of a body to be periodic,

         * Body must move on a definite path.

         * It must repeat its motion after a definite time interval.

Oscilatory Motion:

When a body makes to and fro motion about a fixed point, on a almost straight line path and repeats its motion after a definite time interval, then the motion of the body is a vibratory motion or oscillatory motion

         * It must have periodic motion

         * The body must move to & fro about a fixed point on a almost straight line                 path.

The point about which the body makes to and fro motion is called its mean position. 

           Example:  

(i) Motion of a bob of a simple pendulum if displacement is small, (ii) Motion of a mass attached to a spring,

(iii) Motion of a block, moving with constant speed, on a smooth horizontal floor between two rigid walls.

* Every oscillatory motion must be a periodic motion but every periodic motion is not oscillatory.

Simple Harmonic Motion

When a body makes oscillatory motion about a fixed mean position such that the acceleration of the body at any instant is directly proportional to its displacement from the mean position & is always directed towards the mean position

                        a  ∝  –x

            or         a  =  – ω2 x      ……………….. (1)

                       Where,  ω (const)  =  angular frequency

According to Newtons second law –

                        F =  ma

            or         F = –mω2x

                        F = –k x                       ……………….. (2)

            i.e.       F      ∝  –x

                       Where,  k = Force constant

            Since, the force is always directed towards the mean position it is called restoring force.

  • Note :The necessary and sufficient condition for a motion of a particle to be S.H.M. that, force acting on it must be directed towards a fixed point called mean (equilibrium) position and magnitude of the force must be proportional to the displacement of the particle from the equilibrium position.
  • Note: For SHM                                                                                                                                                                                          F = –k x                      

Introduction to SHM Video [In HINDI+ENGLISH Mix Language]

Leave a Comment

************************************** Unique Offline ISC Classes (XI & XII) with Online Support

Get THREE days FREE Trial in 'ISC XI &XII Offline Classes' starting soon.

 

error: Content is protected !!