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Heat, Thermodynamics and Sound
4.1 Temperature and Heat Transfer
Temperature scales:
- Celsius (°C): 0°C (melting ice), 100°C (boiling water at 1 atm)
- Fahrenheit (°F): °F = (9/5)°C + 32
- Kelvin (K): K = °C + 273.15 (absolute zero = 0 K = −273.15°C — lowest possible temperature; molecules cease all motion)
Heat Transfer Mechanisms:
| Mechanism | Medium Required | How it works | Examples |
|---|---|---|---|
| Conduction | Required (solids best) | Molecule-to-molecule energy transfer | Metals cooling, cooking |
| Convection | Required (fluids) | Bulk movement of heated fluid | Sea breezes, room heaters, ocean currents |
| Radiation | Not required | EM wave (infrared) emission | Sun's heat reaching Earth, thermos flask |
Specific Heat Capacity: Amount of heat needed to raise 1 kg by 1°C.
Water has exceptionally high SHC (4,186 J/kg·K). This is why oceans moderate coastal climates and why water is used as coolant in engines.
4.2 Laws of Thermodynamics
| Law | Statement | Implications |
|---|---|---|
| Zeroth | If A is in thermal equilibrium with C, and B is in equilibrium with C, then A and B are in equilibrium | Defines temperature as a measurable property |
| First | Energy cannot be created or destroyed; Q = ΔU + W | Refrigerators, heat engines obey energy conservation |
| Second | Heat does not spontaneously flow from cold to hot; entropy of universe always increases | No heat engine is 100% efficient; refrigerator needs external work |
| Third | As T → 0 K, entropy → constant (minimum) | Absolute zero is unattainable |
Carnot Efficiency: Maximum theoretical efficiency of a heat engine = 1 − (T_cold/T_hot). The larger the temperature difference, the more efficient the engine.
4.3 Sound Waves
Sound is a longitudinal mechanical wave — particles oscillate parallel to wave propagation direction. It requires a material medium and cannot travel in vacuum.
Speed of sound:
- In air at 0°C = 332 m/s; at 25°C ≈ 346 m/s
- In water ≈ 1,500 m/s; in steel ≈ 5,100 m/s
- Sound travels faster in denser media because particles are closer together
Frequency ranges:
- Infrasound: < 20 Hz — earthquakes, elephant communication, weather
- Audible range: 20 Hz – 20,000 Hz (human hearing)
- Ultrasound: > 20,000 Hz
Applications of ultrasound:
- Medical USG: 2–15 MHz sound pulses reflect from organ boundaries — images of foetus, kidney stones, cardiac function.
- Sonar (Sound Navigation and Ranging): Used by submarines and bats (echolocation) — measures depth/distance by time of echo.
- Industrial NDT: Detects internal cracks in metal castings without cutting.
- Lithotripsy: High-intensity ultrasound pulses break kidney stones non-surgically.
Doppler Effect: When source and observer move relative to each other, observed frequency changes.
- Apparent frequency increases when approaching, decreases when receding.
- Applications: radar speed guns, weather Doppler radar, redshift in astronomy (universe expansion evidence), Doppler ultrasound in cardiology.
