Heat Transfer

Definitions

  • System: what we want to study
  • Surroundings: external to system
  • Boundary: region between system and surroundings where interactions happen

  • Property: macroscopic characteristic of system
  • State: condition of system described by properties
  • Process: transformation from one state to another

  • Steady state: when a certain property does not change with time
  • Extensive property: overall value is sum of its parts (e.g. mass, volume, energy)
  • Intensive property: values are independent of size, extent (e.g. pressure, temperature)

Thermodynamic Systems

  1. Isolated system
    • No exchange of energy
    • No exchange of matter
  2. Closed system
    • Exchange of energy
    • No exchange of matter
  3. Open system/Control volume
    • Exchange of energy
    • Exchange of matter

Work Done and Heat Transfer

Work Done, W

  • W > 0: Work done BY system
  • W < 0: Work done ON system

Warning

Work done is NOT a property of the system.

Heat Transfer, Q

  • Q > 0: Heat transfer TO system
  • Q < 0: Heat transfer FROM system

Warning

Heat transfer is NOT a property of the system.

Rate of heat transfer

Q = \int_{t_{1}}^{t_{2}}\dot{Q} \ dt\\ \text{Units: }W\text{ or }Js^{-1}

Heat flux

  • Rate of heat transfer per unit area \dot{q}
\dot{Q} = \int_{A}\dot{q} \ dA\\ \text{Units: }Wm^{-2}\text{ or }Js^{-1}m^{-2}

Adiabatic process

  • Thermodynamic process involving no heat transfer with the surroundings

Conduction

  • Occurs within the same medium
  • Happens in solids, liquids, gases
  • Transfer of energy from energetic to less energetic particles

Fourier's Law

\text{Heat transfer due to conduction, }\dot{Q}_{x} = -\kappa A\frac{dT}{dx}

where:

  • \kappa is the thermal conductivity of the material;
  • A is the surface area of the material;
  • \frac{dT}{dx} is the temperature gradient across the x-direction.

\textbf{Assuming linear temperature gradient:}

\text{Heat transfer due to conduction, }\dot{Q}_{x} = -\kappa A\left(\frac{T_{2}-T_{1}}{L}\right)

where:

  • \kappa is the thermal conductivity of the material;
  • A is the surface area of the material;
  • T_{1}, T_{2} are the respective temperatures at two ends of the material;
  • L is the length of the material.

Radiation

  • Happens in solids, liquids, gases
  • Emission due to changes in electronic configuration of material

Stefan-Boltzmann Law

\text{Heat transfer due to radiation, }\dot{Q}_{e} = \epsilon\sigma AT_{b}^{4}

where:

  • \epsilon is the emissivity (radiation proportionality) of the material; 0\leq\epsilon\leq1
  • \sigma is the Stefan-Boltzmann constant
  • A is the surface area of the material;
  • T_{b} is the temperature of the emitting surface.

\textbf{As such, net heat transfer due to radiation:}

\text{Net heat transfer due to radiation, }\dot{Q}_{e} = \epsilon\sigma A(T_{h}^4-T_{c}^4), \text{where }T_{h} > T_{c}

where:

  • \epsilon is the emissivity (radiation property) of the material; 0\leq\epsilon\leq1
  • \sigma is the Stefan-Boltzmann constant
  • A is the surface area of the material;
  • T_{h}, T_{c} are the temperature of the hot and cold surfaces respectively.

Convection

  • Occurs between solid and liquid; solid and gas

Newton's law of cooling

\dot{Q}_{c} = hA(T_{h}-T_{c})

where:

  • h is the heat transfer coefficient;
  • A is the surface area of the material;
  • T_{h}, T_{c} are the temperature of the hot and cold surfaces respectively.

Heat transfer coefficient, h

  • Empirical parameter
  • Depends on flow pattern, fluid property, geometry

  • Forced convection
    • Caused by external device (e.g. fan, pump)
    • Larger h (more efficient)
  • Free/natural convection
    • Caused by buoyancy effects (difference in air density)
    • Smaller h (less efficient)

Laws of Thermodynamics

First Law of Thermodynamics

  • Energy is conserved.
\Delta E = E_{2} - E_{1} = Q - W\\ \frac{dE}{dt} = \dot{Q}-\dot{W}\\ dE = \delta Q - \delta E

Microscopic and Macroscopic Energy

\Delta E = \Delta KE + \Delta PE + \delta U

where:

  • \Delta KE is the change in kinetic energy;
  • \Delta PE is the change in potential energy;
  • the change in the above two energies happens at the macroscopic scale, i.e. changes in KE and PE can be seen;
  • \Delta U is the change in internal energy;
  • the change in internal energy happens at the microscopic scale, i.e. changes in U cannot be seen.

Energy Balance

\dot{E}_{in} + \dot{E}_{gen} -|\dot{E}_{out}| = \dot{E}_{st}

where:

  • \dot{E}_{in} is the rate of energy transfer in;
  • \dot{E}_{gen} is the rate of energy generated;
  • \dot{E}_{out} is the rate of energy transfer out;
  • \dot{E}_{st} is the rate of energy stored.

Surface Energy Balance

  • No heat is generated or stored.
\dot{E}_{in}-|\dot{E}_{out}| = 0