🌊 1. Wave Motion
A wave is a continuous transfer of disturbance from one part of a medium to another through successive vibrations of the particles of the medium about their mean positions.
The wave carries energy and transports momentum but not matter when it propagates in a medium.
📌 Mechanical Wave
The waves which require a material medium for their propagation are called mechanical waves.
📌 Transverse Wave
The wave in which the particles vibrate perpendicularly to the direction of propagation is called a transverse wave.
📌 Longitudinal Wave
The wave in which particles vibrate along the direction of propagation is called a longitudinal wave.
Examples sound wave in air, wave in a spring (compression & release), sea waves, seismic waves.
📐 2. Important Wave Parameters
Distance between two nearest particles vibrating in same phase. Equals distance travelled during one complete vibration.
Number of waves/crests passing a point per second. f = 1/T (T = time period).
Time for one complete wave to pass a point.
Maximum displacement from equilibrium position.
Distance travelled by crest in one second.
Position of wave relative to reference (measured in angles).
Velocity of vibrating particles.
🎵 3. Standing Waves (Superposition)
When two waves of same frequency & amplitude travel in opposite directions → standing wave.
Represents SHM with amplitude A = 2a cos(kx).
✨ Condition for Maximum Amplitude (Antinodes)
Maximum amplitude when |cos(kx)| = 1 → cos(2πx/λ) = cos(nπ)
Antinodes occur at: x = 0, λ/2, λ, 3λ/2, … nλ/2
Phase difference φ = 0, π, 2π, …
Path difference = nλ/2
✅ Distance between two consecutive antinodes = λ/2
🔥 4. Second Law of Thermodynamics
⚙️ 5. Heat Engine
Device converting heat energy into mechanical work. 3 parts: Source (hot body at T₁), Working substance, Sink (cold body at T₂).
📈 Efficiency of Heat Engine
🌀 6. Carnot Engine (Ideal Heat Engine)
Carnot engine has maximum efficiency; works on Carnot cycle consisting of two isothermal and two adiabatic processes.
📌 Carnot Cycle Steps (P-V diagram)
- a. Isothermal Expansion (A→B): Absorbs Q₁ at T₁ → W₁ = nRT₁ ln(V₂/V₁)
- b. Adiabatic Expansion (B→C): Temperature drops T₁→T₂, W₂ = nR(T₁-T₂)/(γ-1)
- c. Isothermal Compression (C→D): Rejects Q₂ to sink at T₂, W₃ = nRT₂ ln(V₃/V₄)
- d. Adiabatic Compression (D→A): Temperature rises T₂→T₁, W₄ = nR(T₁-T₂)/(γ-1)
Net work = area enclosed by cycle ABCDA.
📊 7. Efficiency of Carnot Cycle
From isothermal processes: Q₁ = nRT₁ ln(V₂/V₁), Q₂ = nRT₂ ln(V₃/V₄)
From adiabatic conditions: V₂/V₁ = V₃/V₄ → logarithms cancel.
❄️ 8. Refrigerator (Reverse Carnot Cycle)
Transfers heat Q₂ from cold body to hot body by doing external work W.
📘 Key Formulae Summary — Wave velocity: v = fλ | Particle velocity: vp = -v(dy/dx) | Carnot η = 1 – T₂/T₁ | Engine η = 1 – Q₂/Q₁