Definition of Heat
Conceptual Overview
Heat: form of energy transfer due to temperature difference. Not a property of a system, but energy in transit. Unit: joule (J). Symbol: Q. Direction: spontaneously from hotter to colder body.
Distinction from Temperature
Heat: energy transfer mechanism. Temperature: measure of average kinetic energy of particles. Heat transfer changes temperature or phase.
Energy Transfer Mode
Occurs via microscopic collisions and electromagnetic waves. Not stored but exchanged between systems or surroundings.
Modes of Heat Transfer
Conduction
Mechanism: direct molecular collision, electron movement in metals. Medium: solids primarily. Rate: governed by Fourier’s law.
Convection
Mechanism: bulk fluid motion carries heat. Types: natural (buoyancy-driven), forced (external source). Requires fluid medium.
Radiation
Mechanism: electromagnetic waves (infrared). Does not require medium. Governed by Stefan-Boltzmann law. All bodies emit radiation proportional to temperature.
Heat and Thermodynamics Laws
First Law of Thermodynamics
Energy conservation: ΔU = Q - W, internal energy change equals heat added minus work done by system.
Second Law of Thermodynamics
Heat flows spontaneously from hot to cold. Entropy of isolated system increases. Defines irreversibility of heat transfer.
Third Law of Thermodynamics
Absolute zero unattainable. Entropy approaches constant minimum as temperature approaches zero. Heat capacity approaches zero near 0 K.
Heat Capacity and Specific Heat
Heat Capacity (C)
Definition: amount of heat to raise system’s temperature by 1 K. Unit: J/K. Extensive property dependent on mass.
Specific Heat Capacity (c)
Heat capacity per unit mass. Unit: J/kg·K. Varies with material and phase. Used for calculating heat transfer in substances.
Calculation Formula
Q = m × c × ΔTQ: heat (J), m: mass (kg), c: specific heat (J/kg·K), ΔT: temperature change (K).
Calorimetry Techniques
Basic Principle
Measure heat transfer by temperature change in known mass and specific heat. Assumes no heat loss to environment.
Types of Calorimeters
Simple coffee-cup calorimeter: constant pressure. Bomb calorimeter: constant volume, measures combustion heat.
Heat Transfer Calculation
Q_lost = - Q_gainedUsed to find unknown heat or specific heat of substances.
Latent Heat and Phase Changes
Definition
Heat absorbed or released during phase change at constant temperature and pressure. Does not change temperature.
Types
Latent heat of fusion: solid-liquid transition. Latent heat of vaporization: liquid-gas transition.
Formula
Q = m × LQ: heat (J), m: mass (kg), L: latent heat (J/kg).
| Substance | Latent Heat of Fusion (kJ/kg) | Latent Heat of Vaporization (kJ/kg) |
|---|---|---|
| Water | 334 | 2260 |
| Ethanol | 104 | 854 |
Microscopic Interpretation of Heat
Particle Motion
Heat corresponds to increased random kinetic energy of atoms and molecules. Vibrations, rotations, translations contribute.
Phonons and Energy Transfer
Phonons: quantized lattice vibrations in solids transfer heat by conduction. Electron transport significant in metals.
Statistical Mechanics
Heat relates to distribution of particle energies. Boltzmann distribution governs energy states occupancy at given temperature.
Measurement of Heat
Calorimeter Use
Measures heat released or absorbed. Requires thermal isolation and precise temperature sensors.
Thermometric Methods
Thermocouples, resistance temperature detectors (RTDs), infrared sensors detect temperature changes linked to heat flow.
Heat Flux Sensors
Direct measurement of heat flow rate per unit area. Used in engineering and material testing.
Practical Applications
Heating and Cooling Systems
Design of HVAC systems relies on heat transfer principles. Insulation to minimize heat loss.
Industrial Processes
Metal processing, chemical reactions, thermal management depend on controlled heat transfer.
Biological Systems
Metabolism generates heat. Thermoregulation maintains organism temperature via heat exchange.
Heat Engines and Efficiency
Basic Principle
Convert heat energy into mechanical work. Operate cyclically between hot and cold reservoirs.
Efficiency Limits
Maximum efficiency defined by Carnot efficiency: η = 1 - (T_cold / T_hot). Real engines have lower efficiencies.
Examples
Steam engines, internal combustion engines, refrigerators (reverse heat engines).
Thermal Conductivity and Insulation
Thermal Conductivity (k)
Material property: ability to conduct heat. Units: W/m·K. High in metals, low in insulators.
Heat Transfer Rate
Q/t = k × A × (ΔT / d)Q/t: heat transfer rate (W), A: cross-sectional area (m²), ΔT: temperature difference (K), d: thickness (m).
Insulating Materials
Low k value materials reduce heat flow. Examples: foam, fiberglass, air gaps.
| Material | Thermal Conductivity (W/m·K) |
|---|---|
| Copper | 401 |
| Aluminum | 237 |
| Glass Wool | 0.04 |
| Air | 0.025 |
Radiative Heat Transfer
Emission and Absorption
All bodies emit and absorb thermal radiation. Emissivity (ε) quantifies efficiency (0 to 1).
Stefan-Boltzmann Law
P = εσAT⁴P: power radiated (W), ε: emissivity, σ: Stefan-Boltzmann constant (5.67×10⁻⁸ W/m²K⁴), A: area (m²), T: absolute temperature (K).
Applications
Solar radiation, thermal imaging, radiative cooling, spacecraft thermal control.
References
- Halliday, D., Resnick, R., & Walker, J. Fundamentals of Physics, 10th Edition. Wiley, 2014, pp. 512-557.
- Çengel, Y. A., & Boles, M. A. Thermodynamics: An Engineering Approach, 8th Edition. McGraw-Hill Education, 2015, pp. 300-350.
- Tipler, P. A., & Mosca, G. Physics for Scientists and Engineers, 6th Edition. W. H. Freeman, 2007, pp. 450-490.
- Incropera, F. P., & DeWitt, D. P. Fundamentals of Heat and Mass Transfer, 6th Edition. Wiley, 2006, pp. 120-180.
- Feynman, R. P., Leighton, R. B., & Sands, M. The Feynman Lectures on Physics, Vol. 1. Addison-Wesley, 1963, pp. 39-78.