The heat transfer science and its basic concepts have already
been discussed in details. This post is about the Conduction phenomena in
detail.
What Is Conduction?
Conduction is the phenomena of transfer of
energy due to the temperature gradient. On the molecular level, conduction
definition can be described as the transfer of kinetic energy between the molecules;
due to the elastic and inelastic collisions between the molecules.
The term conduction is basically used for the
heat transfer between the solids. In liquids and gases pure conduction can not exist.
Fourier’s Law Of Heat Conduction:
Fourier
law is used as the general equation of conduction. Fourier law states that:
“The rate of heat transfer per unit area is
directly proportional to the normal temperature gradient.”
Q = -kA dT
dx
Or
qx = -k
dT
dx
The negative sign of the equation shows the negative
temperature gradient, which ensures that the thermal energy flows in the
direction of decreasing temperature.
Where:
Q
= rate of heat transfer
A
= heat transfer area
k = thermal conductivity of material; W/m.K
q
= heat flux ; W/m2
The above two equations are the equations
for heat conduction in single direction. As per to the Cartesian coordinates system,
the above equations can be simplified as the most general equation of
conduction is:
q = - k ▽T
Thermal
Conductivity Units (k):
Thermal conductivity units
in FPS system : Btu/hr·ft⋅F
Where:
1
W/(m. oC) = 0.5778 Btu/hr·ft⋅F
One Dimensional
Steady State Conduction:
The term steady state conduction describes that
the temperatures at any point are independent of the time factor. The one
dimensional conduction refers to the fact that the temperature gradients exist
along in the single direction only.
- Plane wall:
The
heat transfer rate through a plane wall (made up of single material) is :
Δx
Or
Qx = T1 – T2
Rth
Where Rth is the resistance
to the heat transfer, which is equal to the Δx/ kA
- Composite wall:
The heat transfer rate through
a composite wall made up of more then 1 material is :
Qx = ΔToverall
∑Rth
- Cylinders:
The
heat transfer rate along the cylinder are:
Q= 2πLk (Ti – To)
ln(ro/
ri)
- Spheres
Spherical
systems are also considered as the one dimensional systems. The heat transfer rate
along the sphere is:
Q =
4πk (Ti – To)
1/ri - 1/ro
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