Simple Harmonic Motion (SHM): Definition, Formula, Working Principle, Equations, and More

Physics Oscillations 2025

Syed Aquib Ur Rahman
Updated on Aug 11, 2025 15:47 IST

By Syed Aquib Ur Rahman, Assistant Manager

Simple Harmonic Motion (SHM) occurs when an object oscillates, and the force pulling it back to its starting position is directly proportional to the distance it has moved from that position. When reading about oscillations in Class 11 Physics, you know that a body, when it repeats its motion along a definite path and does so at regular time intervals, is said to exhibit periodic motion. The time interval is often referred to as the harmonic motion period (T). This path of periodic motion can be linear, circular, elliptical, or another other curve.

SHM is special because it has a unique characteristic: the restoring force that pulls the object back toward its equilibrium position is directly proportional to how far the object has moved from that position. This proportional relationship between force and displacement is what distinguishes simple harmonic motion from other types of periodic motion. We uncover about Simple Harmonic Motion more today. 

Table of content
  • What is Simple Harmonic Motion?
  • NCERT Definition of Simple Harmonic Motion
  • Working Principle of Simple Harmonic Motion
  • Types of SHM
  • Simple Harmonic Motion (SHM) Equation
  • Characteristics of SHM
  • Graph of Speed (v) vs Displacement (x) in Simple Harmonic Motion
  • SHM as a Projection of Uniform Circular Motion
  • Energy of SHM
  • Simple Pendulum and SHM
  • Compound Pendulum / Physical Pendulum and SHM
  • Torsional Pendulum and SHM
  • Superposition of Two Simple Harmonic Motions
  • Revision Notes for Physics Class 11
  • NCERT Solutions Physics Class 11
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What is Simple Harmonic Motion?

Simple Harmonic Motion (SHM) represents a specific form of repetitive motion in which an object moves to and from a central rest position. This motion is termed "simple" due to its mathematical description using basic trigonometric functions such as sine or cosine waves.

Importance of Learning Simple Harmonic Motion for Exams

  • SHM frequently appears in JEE Main and Advanced exams, with at least one question expected annually. Problems typically focus on finding time period, frequency, amplitude, phase, velocity, acceleration, and energy for systems like springs and pendulums. These variables are also part of your later chapter on Waves, especially when you are learning about displacement relation of progressive waves.   
  • If you can master SHM concepts and problem patterns that we show here, you can easily score full marks, as most questions involve direct formula application or basic analysis.

Practice exercises for NCERT Solutions for Chapter 13 free!

 

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NCERT Definition of Simple Harmonic Motion

The NCERT textbook defines Simple Harmonic Motion as - 

"Consider a particle oscillating back and forth about the origin of an x-axis between the limits +A and –A ... This oscillatory motion is said to be simple harmonic if the
displacement x of the particle from the origin varies with time as : x (t) = A cos (ω t + φ)". 

Key points to remember about Simple Harmonic Motion

  • Repetitive motion between fixed boundaries
  • Displacement varies sinusoidally with time
  • Motion is described by three constants (A, ω, φ) that define its amplitude, frequency, and phase

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Working Principle of Simple Harmonic Motion

SHM operates on the fundamental principle of restoring force.

When an object is displaced from its equilibrium position, a force acts to pull it back toward that central position. This restoring force is directly proportional to the displacement and always points toward equilibrium.

Key Operating Mechanisms:

  1. The driving mechanism that maintains oscillation by constantly pulling the object back to its rest position
  2. In ideal SHM, mechanical energy remains constant as it continuously converts between kinetic energy (at equilibrium) and potential energy (at extreme positions)
  3. The proportional restoring force creates regular, repeating motion with fixed time intervals



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Types of SHM

We need to learn about two major types of simple harmonic motion. 

  • Linear SHM: When a moving body or particle undergoes to and fro motion along a straight line in equilibrium position. A and B are two extreme ends. M is the mean position. A and B are extreme positions. M is the mean position. A M = M B = A m p l i t u d e
  • Angular SHM: This occurs when a moving particle freely rotates in a predefined axis with the path curved.  This concept would be clearer when you go brush up on torque and angular momentum

 

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Simple Harmonic Motion (SHM) Equation

For SHM to work, the main condition is

F = - k x


Where,

k = positive constant for an SHM = Force constant
x = displacement from the mean position.
or

m d 2 x d t 2 = - k x


d 2 x d t 2 + k m x = 0 [differential equation of SHM]
d 2 x d t 2 + ω 2 x = 0

where ω = k m
Its solution is x = A s i n ( ω t + ϕ )

 

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Characteristics of SHM

Let's look at the characteristics of Simple Harmonic Motion. 

Note: In the figure shown, the path of the particle is on a straight line.

 

  • Displacement - It is defined as the distance of the particle from the mean position at that instant. Displacement in SHM at time t is given by x = A s i n ( ω t + ϕ )

 

  • Amplitude : It is the maximum value of the displacement of the particle from its equilibrium position. Amplitude = 1 2 [distance between extreme points or positions]. It depends on the energy of the system.
  • Angular Frequency is ( ω ) : ω = 2 π T = 2 π f and its unit is r a d / s e c .
  • Frequency (f): The number of oscillations completed in unit time interval is called the frequency of oscillations, f = 1 T = ω 2 π , its unit is s e c - 1 or Hz .
  • Time period (T) : This is the smallest time interval after which the oscillatory motion gets repeated is called time period, T = 2 π ω = 2 π m k
  • Phase: The physical quantity which represents the state of motion of particle (eg. its position and direction of motion at any instant). The argument ( ω t + ϕ ) of sinusoidal function is called instantaneous phase of the motion.
  • Phase constant ( ϕ ): Constant ϕ in equation of SHM is called the phase constant or the initial phase. It depends on the initial position and direction of velocity.
  • Velocity(v): Velocity at an instant is the rate of change of the particle's position w.r.t time at that instant.
    Let the displacement from the mean position be given by

x = A s i n ( ω t + ϕ )   Velocity,   v = d x d t = d d t [ A s i n ( ω t + ϕ ) ] v = A ω c o s ( ω t + ϕ )   or,   v = ω A 2 - x 2

At the mean position ( x = 0 ), the velocity is maximum.

V m a x = ω A

At the extreme position ( x = A ), velocity is minimum.

V m i n = z e r o

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Graph of Speed (v) vs Displacement (x) in Simple Harmonic Motion

Let's look at two graphical ways to represent Simple Harmonic Motion. 

When the Graph is Elliptical

The velocity equation in simple harmonic motion is

v = ω A 2 - x 2 v 2 = ω 2 A 2 - x 2 v 2 + ω 2 x 2 = ω 2 A 2 v 2 ω 2 A 2 + x 2 A 2 = 1

GRAPH WOULD BE AN ELLIPSE

Acceleration at an instant is the rate of change of the particle's velocity with respect to time at that instant.

Acceleration, a = d v d t = d d t [ A ω c o s ( ω t + ϕ ) ]

a = - ω 2 A s i n ( ω t + ϕ ) a = - ω 2 x

Note

A negative sign shows that acceleration is always directed towards the mean position. At the mean position ( x = 0 ), acceleration is minimum. a m i n =   zero  

At the extreme position ( x = A ), acceleration is maximum.

a m a x = ω 2 A

GRAPH OF ACCELERATION (A) vs DISPLACEMENT (x)

a = - ω 2 x

 

 

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SHM as a Projection of Uniform Circular Motion

Consider a particle moving on a circle of radius A with a constant angular speed ω as shown in figure.


Suppose the particle is on the top of the circle (Y-axis) at t = 0 .

The radius OP makes an angle θ = ω t with the Y-axis at time t .

Drop a perpendicular PQ on the x-axis. The components of the position vector, velocity vector and acceleration vector at time t on the X -axis are

x ( t ) = A s i n ω t v x ( t ) = A ω c o s ω t a x ( t ) = - ω 2 A s i n ω t

The above equations show that the foot of perpendicular Q executes a simple harmonic motion on the X-axis. The amplitude is A and the angular frequency is ω .

Similarly, the foot of a perpendicular on the Y-axis will also execute SHM of amplitude A and angular frequency ω [ y ( t ) = A c o s ω t ] .

The phases of the two simple harmonic motions differ by π / 2 .


Graphical Representation of Displacement, Velocity, and Acceleration in SHM

Displacement, x = A s i n ω t
Velocity, v = A ω c o s ω t = A ω s i n ω t + π 2  or v = A 2 - x 2 ω
Acceleration, a = - ω 2 A s i n ω t = ω 2 A s i n ( ω t + π ) or a = - ω 2 x
Note: - v = ω A 2 - x 2

a = - ω 2 x

These relations are true for any equation of x .

 

  • All three quantities - displacement, velocity and acceleration - vary harmonically with time, having the same period.
  • The velocity amplitude is A ω times the displacement amplitude ( ω ).
  • The acceleration amplitude is ω times the displacement amplitude ( - ω 2 A ).
  • In SHM, the velocity is ahead of displacement by a phase angle of ω 2 A .
  • In SHM, the acceleration is ahead of velocity by a phase angle of ω .
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Energy of SHM

Let's mathematically look into how mechanical energy is related to Simple Harmonic Motion.  

Kinetic Energy in SHM

 

Kinetic Energy (KE) (as a function of x)

( as a function of t)
Frequency of KE = 2*(frequency of SHM)

 

Potential Energy in SHM

 

Potential Energy (PE)

(as a function of x )= (as a function of time)

 

Total Mechanical Energy (TME)

Total mechanical energy = Kinetic energy + Potential energy =

Hence, total mechanical energy is constant in SHM.

Graphical Variation of Total Energy of a Particle in SHM

 
Methods to Determine Time Period and Angular Frequency  in SHM
 
  • Force / torque method
  • Energy method

 

 

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Simple Pendulum and SHM

If a heavy point mass is suspended by a weightless, inextensible and perfectly flexible string from a rigid support, then this arrangement is called a simple pendulum.

Time period of a simple pendulum T=2𝜋√l/g

(Some times we can take g= 𝜋2 for making calculation simple)
Note:

If the angular amplitude of the simple pendulum is greater,  time period


Where θ0 is in radians.

The general formula for time period of a simple pendulum when it is comparable to radius of Earth R.

Where, R = Radius of the Earth

 

The time period of a simple pendulum of infinite length is maximum and is given by:

2𝜋√r/g=84.6 min 

 

Where R is the radius of Earth.

 

Time period of seconds pendulum is 2 sec and ℓ =0.993 m.

The simple pendulum performs angular S.H.M. But but due to smaller angular displacement, it is considered as linear S.H.M.

If the time period of a clock is based on a simple pendulum that increases, the clock will be slow. But if the time period decreases, then the clock will be fast.

If g remains constant &△ℓ is change in length, then

 

If ℓ remains constant &△g is the change in acceleration, then,

 

If △ℓ is the change in length and △g is the change in acceleration due to gravity, then,

1 Time Period of Simple Pendulum in an Accelerating Reference Frame 

Where  

If forces other than gravity and tension acts, then :

  where

 

constant force acting on 'm'.
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Compound Pendulum / Physical Pendulum and SHM

When a rigid body is suspended from an axis and made to oscillate about that, then it is called a compound pendulum.

C = Position of centre of mass
S = Point of suspension
ℓ =   Distance between the point of suspension and centre of mass (it remains constant during motion)
For a small angular displacement "0" from the mean position, the restoring torque is given by

or where,

l = The Moment of inertia about the point of suspension.

or or

 

Time period,

Where Icm = moment of inertia relative to the axis which passes from the centre of mass & parallel to the axis of oscillation.

where Iсм =

k = gyration radius (about the axis passing from the centre of mass)

 T is minimum ℓ = k.

Graph of T vs ℓ

 

 

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Torsional Pendulum and SHM

In torsional pendulum, an extended object is suspended at the centre by a light torsion wire. A torsion wire is essentially inextensible, but is free to twist about its axis. When the lower end of the wire is rotated by a slight amount, the wire applies a restoring torque causing the body to oscillate (rotate) about vertical wire, when released.

The restoring torque produced is given by

 
Where,
C= Torsional constant
or  Moment of inertia about the vertical axis.

or Time Period,

 

 

 

 

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Superposition of Two Simple Harmonic Motions

In the same direction and of the same frequency.

, then resultant displacement

where

If θ= 0, both SHM's are in phase and

If θ=π, both SHM's are out of phase and

The resultant amplitude due to the superposition of two or more than two SHM's in this case, can also be found by a phasor diagram also.

In the same direction, but of different frequencies.

then resultant displacement

This resultant motion is not SHM.
In two perpendicular directions.

Case 1

 

So the path will be a straight line & resultant displacement will be

, which is the equation of SHM having amplitude

 

Case 2

so, resultant will be i.e. equation of an ellipse and if , then superposition will be the equation of circle. This resultant motion is not SHM.

 

The Phasor Diagram

If two or more SHMs are along the same line, their resultant can be obtained by vector addition by making a phasor diagram.

 

  • Amplitude of SHM is taken as the length (magnitude) of the vector
  • The phase difference between the vectors is taken as the angle between these vectors. The magnitude of the resultant vector gives the resultant amplitude of SHM and the angle of resultant vector gives the phase constant of the resultant SHM.

For example :

If equation of resultant SHM is taken as

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Revision Notes for Physics Class 11

These are some of the chapter overviews to revise before exams. We regularly update the expert-collaborated topics for each chapter as well.  

Units and Measurements Class 11 Notes Mechanical Properties of Solids Class 11 Notes
Motion in a Straight Line Class 11 Notes Mechanical Properties of Fluids Class 11 Notes
NCERT Class 11 Notes for Motion in a Plane Thermal Properties of Matter Class 11 Notes
Laws of Motion Class 11 Notes Thermodynamics Class 11 Notes
Work, Energy, and Power Class 11 Notes Kinetic Theory of Gas Class 11 Notes
System of Particles and Rotational Motion Class 11 Notes Oscillations Class 11 Notes
Gravitation Class 11 Notes Waves Class 11 Notes

Get a macroscopic view of Class 11 PCM chapters and topics below. 

NCERT Class 11 Notes for PCM
NCERT Class 11 Physics Notes

 

 

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NCERT Solutions Physics Class 11

Q&A Icon
Commonly asked questions
Q:  

What is the restoring force in Simple Harmonic Motion?

A: 

The restoring force in SHM is the force that always acts towards the mean position and is directly proportional to the displacement from it. It follows F=? kx. Here, the negative sign indicates the force is in the opposite direction to the displacement.

Q:  

What is meant by the phase of SHM?

A: 

The phase in SHM tells us the position and direction of motion of the particle at a specific instant. It determines the state of oscillation and includes both displacement and time information.

Q:  

What is resonance in forced oscillations?

A: 

Resonance occurs when the frequency of an external periodic force matches the natural frequency of a system. From that, physicists know that resonance causes the amplitude of oscillations to increase significantly. This can be beneficial in devices, such as musical instruments, but dangerous in structures like bridges.

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