Oscillations and waves describe periodic motion and energy transfer without matter transport.
Overview
graph TD
A[Oscillations & Waves] --> B[SHM]
A --> C[Wave Motion]
B --> B1[Simple Pendulum]
B --> B2[Spring System]
C --> C1[Transverse]
C --> C2[Longitudinal]
C --> C3[Standing Waves]Simple Harmonic Motion (SHM)
Interactive Demo: Spring-Mass Oscillation
Watch how a mass on a spring oscillates. Adjust amplitude and frequency to see how they affect the motion:
Definition
Motion in which acceleration is proportional to displacement and directed towards mean position:
$$\boxed{a = -\omega^2 x}$$Equations of SHM
$$x = A\sin(\omega t + \phi)$$or
$$x = A\cos(\omega t + \phi)$$ $$v = A\omega\cos(\omega t + \phi) = \omega\sqrt{A^2 - x^2}$$ $$a = -A\omega^2\sin(\omega t + \phi) = -\omega^2 x$$Key Relations
$$\boxed{\omega = \frac{2\pi}{T} = 2\pi f}$$ $$\boxed{v_{max} = A\omega}$$(at mean position)
$$\boxed{a_{max} = A\omega^2}$$(at extreme position)
Energy in SHM
$$KE = \frac{1}{2}m\omega^2(A^2 - x^2)$$ $$PE = \frac{1}{2}m\omega^2 x^2$$ $$\boxed{E_{total} = \frac{1}{2}m\omega^2 A^2 = \frac{1}{2}kA^2}$$Properties:
- KE maximum at mean position
- PE maximum at extreme position
- Total energy constant
Simple Pendulum
$$\boxed{T = 2\pi\sqrt{\frac{L}{g}}}$$For small oscillations (θ < 10°)
Factors Affecting T
- T increases with L
- T decreases with g
- T independent of mass and amplitude
Spring-Mass System
$$\boxed{T = 2\pi\sqrt{\frac{m}{k}}}$$Combinations of Springs
Series:
$$\frac{1}{k_{eq}} = \frac{1}{k_1} + \frac{1}{k_2}$$Parallel:
$$k_{eq} = k_1 + k_2$$Wave Motion
Types of Waves
| Type | Particle Motion | Examples |
|---|---|---|
| Transverse | Perpendicular to propagation | Light, string waves |
| Longitudinal | Parallel to propagation | Sound, spring waves |
Wave Equation
$$\boxed{y = A\sin(kx - \omega t + \phi)}$$where:
- $k = \frac{2\pi}{\lambda}$ (wave number)
- $\omega = 2\pi f$ (angular frequency)
- $v = f\lambda = \frac{\omega}{k}$ (wave velocity)
Wave Velocity
On string:
$$v = \sqrt{\frac{T}{\mu}}$$where T = tension, μ = mass per unit length
Sound in gas:
$$v = \sqrt{\frac{\gamma P}{\rho}} = \sqrt{\frac{\gamma RT}{M}}$$Superposition of Waves
Principle
When two waves overlap, the resultant displacement is the sum of individual displacements.
Interactive Demo: Wave Superposition
See how two waves combine. Adjust frequencies and phase difference to observe interference and beats:
Interference
Constructive: Phase difference = 0, 2π, 4π… (Path difference = 0, λ, 2λ…)
$$A_{max} = A_1 + A_2$$Destructive: Phase difference = π, 3π… (Path difference = λ/2, 3λ/2…)
$$A_{min} = |A_1 - A_2|$$Beats
When two waves of slightly different frequencies superpose:
$$\boxed{f_{beat} = |f_1 - f_2|}$$Standing Waves
Formed by superposition of two waves of same frequency traveling in opposite directions.
Equation
$$y = 2A\sin(kx)\cos(\omega t)$$Nodes and Antinodes
- Nodes: Points of zero amplitude (destructive interference)
- Antinodes: Points of maximum amplitude (constructive interference)
Distance between consecutive nodes = λ/2
Standing Waves in Strings
Fixed at Both Ends
$$\lambda_n = \frac{2L}{n}$$ $$\boxed{f_n = \frac{n}{2L}\sqrt{\frac{T}{\mu}} = nf_1}$$n = 1, 2, 3… (harmonics)
Standing Waves in Organ Pipes
Closed Pipe (One end closed)
Only odd harmonics:
$$\boxed{f_n = \frac{(2n-1)v}{4L}}$$n = 1, 2, 3… (1st, 3rd, 5th harmonics)
Open Pipe (Both ends open)
All harmonics:
$$\boxed{f_n = \frac{nv}{2L}}$$n = 1, 2, 3… (all harmonics)
Doppler Effect
Apparent change in frequency due to relative motion between source and observer.
General Formula
$$\boxed{f' = f\left(\frac{v \pm v_o}{v \mp v_s}\right)}$$Sign convention:
- Upper signs: approaching
- Lower signs: receding
Practice Problems
A particle executes SHM with amplitude 4 cm and time period 4 s. Find maximum velocity.
A spring of constant 400 N/m has a 0.1 kg mass attached. Find time period.
A string of length 1 m vibrates in its third harmonic. If tension is 100 N and mass per unit length is 0.01 kg/m, find frequency.
A train approaches a platform at 20 m/s blowing a whistle of 500 Hz. Find frequency heard by observer on platform. (v = 340 m/s)