Simple Harmonic Motion is a type of periodic motion where the restoring force is directly proportional to the displacement from equilibrium and acts in the opposite direction.
Mathematically: F = −kx
F: Restoring force
k: Spring constant (N/m)
x: Displacement from equilibrium (m)
The motion is sinusoidal in nature, leading to predictable oscillations
Common systems exhibiting SHM:
Mass-spring systems
Simple pendulums (for small angles)
Tuning forks
Vibrating strings
Period (T): Time taken for one complete cycle of motion.
Units: seconds (s)
Frequency (f): Number of cycles per unit time.
Units: hertz (Hz)
Relationship: f = 1/T
Period: T = 2π √m/k
m: Mass attached to the spring (kg)
k: Spring constant (N/m)
Period: T = 2π √L/g
L: Length of the pendulum (m)
g: Acceleration due to gravity (9.81 m/s²)
The period of SHM is independent of amplitude (for ideal systems).
In a mass-spring system, increasing mass mmm increases the period T.
In a pendulum, increasing length L increases the period T.
Displacement: x(t) = A cos(ωt+ϕ)
Velocity: v(t) = −Aω sin(ωt+ϕ)
Acceleration: a(t) = −Aω²cos(ωt+ϕ)
A: Amplitude (maximum displacement)
ω: Angular frequency = 2π f
ϕ: Phase constant (depends on initial conditions)
Displacement-Time Graph: Cosine wave starting at maximum displacement.
Velocity-Time Graph: Sine wave, 90° out of phase with displacement.
Acceleration-Time Graph: Cosine wave, 180° out of phase with displacement.
Velocity is 90° out of phase with displacement.
Acceleration is 180° out of phase with displacement
Kinetic Energy (KE): Energy due to motion.
KE = ½ mv²
Potential Energy (PE): Energy stored in the system.
For springs: PE = ½ kx²
In ideal SHM (no damping), total energy EEE remains constant:
E = KE + PE = ½ kA²
At maximum displacement (x = ±A):
KE = 0
PE = Maximum
At equilibrium position (x = 0):
KE = Maximum
PE = 0
KE and PE vary sinusoidally over time, with total energy remaining constant.
A mass attached to a spring oscillates horizontally or vertically.
The restoring force is provided by the spring's elasticity.
A mass (bob) suspended from a string swings back and forth.
For small angles (<15°), the motion approximates SHM.
Vibrating guitar strings.
Tuning forks.
Air columns in wind instruments.
Understand the derivations of period formulas for different systems.
Be able to analyze energy transformations within SHM.
Practice interpreting and sketching displacement, velocity, and acceleration graphs
Apply SHM concepts to real-world systems and identify approximations made