
CHAPTER
CONDUCTION 2

Conduction
Conduction is the mode of energy transfer as heat due to temperature
difference in a solid or any phase of material where the mass is
contiguous and in thermal contact. Microscopically this mode of
energy transfer is attributed to free electron flow from higher to lower
energy levels, lattice vibration and molecular collision. However no
macroscopic mass movement is involved.
The temperature in the body will be a function of location and time.
In the popular cartesian coordinates : T = T(x, y, z, τ)
How temperature varies with position within the body :
The temperature field is obtained by deriving and solving the differential
equation based on energy balance relations for the volume.

Conduction
qxthe conducted heat rate in the x-direction has
phenomenologically been found to be adequately
represented by:
insulator
T1T2 < T1
A
q
x
x
d T
q k A
d x
Temperature gradient
Conductivity

Fourier’s Law
''
T T T
q k T k i j k
x y z
insulator
T1T2 < T1
A
q
x
'' x
x
q
dT
q k
A dx
Baron Jean Baptiste
Joseph Fourier
(1768-1830)
del operator

Thermal conductivity
The equation of heat conduction in one direction
Thermal conductivity k of a material (W/mK) can be defined as the rate
of heat transfer Jun/sec through a unit thickness of the material (m) per
unit area (1m2)per unit temperature difference (1K)
The constant of proportionality k is the thermal conductivity of material,
which is a measure of the ability of a material to conduct heat .
Thermal Conductivity of Gases
Thermal Conductivity of Liquids
Thermal Conductivity of Solids
+ Metals and alloys;
+ Solid dielectrics (non-metals);
'' x
x
q
dT
q k
A dx

