

Key Concepts and Formulas of Simple Harmonic Motion for Students
Simple harmonic motion (SHM) is one of the most important topics in oscillations and waves, often appearing in JEE Main and Advanced exams. Its foundational concepts are key to mastering advanced physics and problem-solving skills.
Definition and Core Principle of Simple Harmonic Motion
Simple harmonic motion can be defined as motion in which the acceleration of the particle is always directed towards a fixed point and is proportional to the particle's displacement from that point but in the opposite direction.
This central property is mathematically expressed as $a = -\omega^2 x$, where $a$ is acceleration, $x$ is displacement, and $\omega$ is the angular frequency of the motion.
Differential Equation Governing SHM
The equation describing SHM can also be written using Newton’s second law. If a mass $m$ is attached to a spring with constant $k$, the restoring force is $F = -kx$.
Applying Newton’s second law gives $m a = -k x$.
This leads to the second-order differential equation $m\dfrac{d^2x}{dt^2} = -k x$.
Rearranging, we obtain $\dfrac{d^2x}{dt^2} + \dfrac{k}{m}x = 0$.
Comparing with $a = -\omega^2 x$, it follows that $\omega = \sqrt{\dfrac{k}{m}}$.
General Solution and Key Quantities in SHM
The general solution of the SHM equation is $x(t) = A \sin(\omega t + \phi)$, where $A$ is amplitude, $\omega$ is angular frequency, and $\phi$ is phase constant.
The amplitude $A$ represents the maximum displacement from equilibrium. The phase constant $\phi$ defines the initial position at $t = 0$.
The period $T$ of oscillation is given by $T = \dfrac{2\pi}{\omega}$. The frequency $f$ is $f = \dfrac{1}{T}$.
Displacement, Velocity, and Acceleration Relationships
Displacement as a function of time in SHM is $x(t) = A \sin(\omega t + \phi)$. Differentiating once, the velocity becomes $v(t) = \omega A \cos(\omega t + \phi)$.
The acceleration at any instant is $a(t) = -\omega^2 x(t)$. This direct proportionality but opposite direction defines SHM uniquely.
Energy Transformations in Simple Harmonic Oscillators
In SHM, energy constantly transforms between kinetic and potential forms, but the total mechanical energy remains constant.
Potential energy at displacement $x$ is $U = \dfrac{1}{2} k x^2$, while kinetic energy is $K = \dfrac{1}{2} m v^2$.
At the mean position, the kinetic energy is maximized, and potential energy is zero. At the extremes, kinetic energy is zero, and potential energy is maximized.
For a deeper exploration of the energy distribution in oscillations, refer to the in-depth article on Energy in Simple Harmonic Motion.
Real-Life Visualisation: Circular Motion Analogy
The motion of a particle in SHM is mathematically equivalent to the projection of uniform circular motion onto a diameter.
If a particle revolves uniformly in a circle of radius $A$, its projection along a diameter exhibits SHM with the same frequency as the angular frequency of revolution.
Key Physical Quantities Comparison Table
| Physical Quantity | Expression in SHM |
|---|---|
| Displacement $x$ | $A \sin(\omega t + \phi)$ |
| Velocity $v$ | $\omega A \cos(\omega t + \phi)$ |
| Acceleration $a$ | $-\omega^2 x$ |
| Period $T$ | $\dfrac{2\pi}{\omega}$ |
| Frequency $f$ | $\dfrac{1}{T}$ |
Common Types of Simple Harmonic Systems
- Mass-spring oscillators follow Hooke’s Law precisely.
- Pendulums exhibit SHM only for small angular displacement.
For a step-by-step analysis of pendulum time periods, review the page on Time Period of Simple Pendulum.
Numerical Example: Maximum Speed and Acceleration in SHM
A block of mass 0.5 kg attached to a spring (k = 200 N/m) oscillates with amplitude 0.1 m. Calculate its maximum speed and acceleration.
Known values: $m = 0.5$ kg, $k = 200$ N/m, $A = 0.1$ m.
Formula for angular frequency: $\omega = \sqrt{\dfrac{k}{m}}$.
Substituting values:
$\omega = \sqrt{\dfrac{200}{0.5}}$
$\omega = \sqrt{400} = 20$ rad/s
Maximum speed: $v_{max} = \omega A$.
$v_{max} = 20 \times 0.1$
$v_{max} = 2$ m/s
Maximum acceleration: $a_{max} = \omega^2 A$.
$a_{max} = (20)^2 \times 0.1$
$a_{max} = 400 \times 0.1 = 40$ m/s$^2$
Final answers: Maximum speed is 2 m/s; maximum acceleration is 40 m/s$^2$.
Simple Harmonic Motion vs. General Oscillations Table
| Feature | Simple Harmonic Motion |
|---|---|
| Restoring Force | Proportional and opposite to displacement |
| Equation of Motion | $a = -\omega^2 x$ |
| Energy Conversion | Total mechanical energy is constant |
| Occurs In | Mass-spring systems, pendulums |
Simple Harmonic Motion in Real World Applications
- Pendulum clocks and quartz movements in wristwatches
- Vibrational modes in musical instruments
- Automotive shock absorbers
- Seismic isolators in earthquake-resistant buildings
Oscillatory motion, a foundational physics concept, underpins many technologies and natural phenomena. Deepen your understanding by exploring detailed notes on Oscillations and Waves.
Practice Question: Displacement in SHM
A particle executes SHM with amplitude 2 cm and frequency 1 Hz. Write the equation for its displacement if its initial phase is zero.
Common Mistakes in SHM Problems
- Confusing displacement with amplitude
- Misreading the direction of restoring force
- Incorrect substitution of values for angular frequency
- Neglecting phase when initial conditions are nonzero
Integration with Other Oscillation Topics
Simple harmonic motion, along with advanced problems, often features in JEE mock tests covering interconnected concepts.
For preparation resources and self-assessment, use the Oscillations and Waves Mock Test designed for competitive exams.
Concept Extensions: Spring Force and SHM Conservation Principles
The origin of SHM lies in the linear relationship described by Hooke’s Law. This law governs the restoring force in a wide variety of oscillating systems.
To review derivations and formulas for forces in springs, see Spring Force and Hooke's Law in detail.
Related physics topics you should study next: damped and forced oscillations, resonance, phase and wave superposition, Fourier analysis, and energy dissipation in vibrations.
FAQs on What Is Simple Harmonic Motion (SHM)?
1. What is simple harmonic motion (SHM)?
Simple harmonic motion (SHM) is a type of periodic motion where a particle moves to and fro about its mean position under a restoring force proportional to its displacement.
- Restoring force acts always towards the mean position
- The amplitude, frequency, and time period are key parameters
- Examples include oscillations of a spring and motion of a simple pendulum under small angles
2. What are the characteristics of simple harmonic motion?
Simple harmonic motion has several distinct characteristics:
- The motion is periodic and repeats after a fixed time interval
- Restoring force is directly proportional to displacement and acts towards mean position: F = -kx
- The path is straight or along a single axis
- The amplitude and frequency remain constant unless disturbed
3. What is the equation of simple harmonic motion?
The equation of simple harmonic motion describes the displacement of a particle as a function of time:
- x(t) = A sin(ωt + φ) or x(t) = A cos(ωt + φ)
- Here, A = amplitude, ω = angular frequency, t = time, φ = phase constant
- The acceleration is given by a = -ω2x
4. What is the difference between simple harmonic motion and periodic motion?
Simple harmonic motion is a specific kind of periodic motion in which the restoring force is proportional to displacement.
- Periodic motion: Any motion that repeats at regular intervals (e.g., Earth's rotation)
- SHM: Special kind of periodic motion, always governed by F = -kx
- SHM has constant amplitude and frequency, while periodic motion may not
5. What is angular frequency in SHM?
Angular frequency (ω) in simple harmonic motion is the rate at which the particle oscillates.
- It is measured in radians per second (rad/s)
- ω = 2πf, where f is the frequency in Hz
- It defines how quickly the phase of the motion changes
6. What are the main examples of simple harmonic motion in daily life?
Simple harmonic motion is found in several everyday phenomena:
- Pendulum (for small angles)
- Mass-spring system
- Vibrations of tuning forks
- Oscillations in electrical circuits (LC)
- Swinging of a cradle
7. What is the time period of a simple pendulum?
The time period (T) of a simple pendulum is the time taken for one complete oscillation.
- T = 2π√(l/g)
- l = length of the pendulum
- g = acceleration due to gravity
8. What factors affect the amplitude and frequency of SHM?
The amplitude in simple harmonic motion depends on the initial conditions, while frequency depends on system properties.
- Amplitude (A): Determined by how far the oscillator is pulled initially; not affected by mass or spring constant
- Frequency (f): For a mass-spring system, f = (1/2π)√(k/m), depends on mass (m) and spring constant (k)
- Neither is affected by energy loss in ideal SHM
9. Why is simple harmonic motion important in physics?
Simple harmonic motion is fundamental because it models many natural and engineering systems.
- Forms the basis for understanding waves, oscillations, and resonance
- Helps in the analysis of sound, light, and quantum systems
- Enables prediction of system behavior under oscillatory forces
10. What is meant by phase in simple harmonic motion?
Phase in simple harmonic motion indicates the position and direction of motion of the oscillating particle at any given instant.
- Expressed as the argument (ωt + φ) in the SHM equation
- Helps determine whether the particle is at mean, extreme, or intermediate position
- Phase difference is used to compare two oscillations
11. Describe the energy changes in simple harmonic motion.
In simple harmonic motion, energy continually shifts between kinetic and potential forms while total energy remains constant.
- At the mean position, kinetic energy is maximum and potential energy is minimum
- At extreme positions, potential energy is maximum and kinetic energy is zero
- Total mechanical energy: E = ½ kA² (for mass-spring system)
12. State the condition for simple harmonic motion to occur.
A system will exhibit simple harmonic motion only if the restoring force is directly proportional to displacement and oppositely directed.
- Mathematically, F = -kx
- Applies to many oscillating systems for small displacements





















