Heat transfer is one of the subjects in thermal engineering, which is primarily concerned with the exchange, use, and conversion of heat or, in other words, thermal energy between physical bodies. Exchange of thermal energy due to the difference in temperatures. This heat transfer takes place when there is a temperature difference. Let’s discuss this topic in detail with relevant examples for better understanding. Transfer of thermal energy from more energetic to less energetic particles due to their interaction is called conduction heat transfer.
There are three forms to transfer heat.
There are two types of conduction: steady-state conduction and transient conduction.
Material is steady when the temperature at its cross sections on any position remains constant with time. The steady-state is different from a state of thermal equilibrium in which temperature at any position should be the same. The temperature of the material in a steady-state varies with position. There is zero absorption or emission of heat at the cross-sections during this state. The extreme ends of the material are steady at specific temperatures, and all other surfaces are covered with insulators so that heat cannot escape through any wall. This also enables the same amount of heat to flow through the cross-sections at particular time intervals.
During transient or non-steady-state conduction, the temperature changes or varies along any part of the material at any given point in time. The primary determinant of the conduction, in this case, is the material’s time-dependent temperature. Transient conduction generally occurs when a temperature change is newly introduced on either the outer edges of the material or inside. Thus, the temperature change is brought about by the sudden entry of a new source of heat within a particular material or object.
Quantitatively, thermal conduction can be described as the rate of time at which heat flows in a given material while set at a particular temperature. It is also possible to maintain parts of an object at different temperatures. It is inversely proportional to the length of the bar. The formula denotes this:
H = KATL
Here H is the amount of transferred heat
K is thermal conductivity
A is the area of the surface
L is the distance
T is the difference in temperature
The greater the value for K is for a given material, the more rapidly it will conduct heat. The thermal conductivities for various materials are listed in the table below. These values are constant at a normal temperature range but may vary slightly with higher or lower temperatures.
MATERIAL | THERMAL CONDUCTIVITY (J/m-K) |
Metals | |
Silver | 406 |
Copper | 385 |
Aluminium | 205 |
Brass | 109 |
Steel | 50.2 |
Lead | 34.7 |
Mercury | 8.3 |
Non-metals | |
Insulating brick | 0.15 |
Concrete | 0.8 |
Body fat | 0.20 |
Felt | 0.04 |
Glass | 0.8 |
Ice | 1.6 |
Glass wool | 0.04 |
Wood | 0.12 |
Water | 0.8 |
Gases | |
Air | 0.024 |
Argon | 0.016 |
Hydrogen | 0.14 |
Heat transfer refers to the phenomenon of transferring energy from one point to another. This specific mechanism includes heat conduction, heat convection, and radiation heat transfer. Conduction is the transfer of heat during the heat conduction process, which is a slow process. For instance, if one end of a metal rod is held above a flame, the other end, which has not been in contact with the flame, will soon turn hot as well. This is due to conduction, enabling the heat to travel through the entirety of the rod. The molecules in hotter regions have more kinetic energy than those not desirable.