EML 4304L    Thermal Fluids Lab

Thermal Conduction

Experiment #3

Teaching Group #3: Christopher Hokes, Ryan Prentiss, Chris Bolyard, Fredrick Davidson, and Siye Baker

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Theoretical Background

 

All temperatures within the bars, the water temperatures and the water flow rates are recorded under equilibrium conditions.  The rate of heat flow at the heat sink is given by                                                                                         (1)

where

mw = mass of cooling water displaced in time Dt

Cp = Specific heat of water at constant pressure

DTw = (Tout - Tin) of cooling water

Dt = time required to displace a volume Vw of water

 

Derivation of Fourier's law

A functional relationship can be established between the rate of heat transfer and the temperature difference, length of travel and the cross-sectional area.  This is the well-known Fourier's law of heat conduction

                                     (2)

where K is the proportionality constant known as the coefficient of thermal conductivity, A is the cross-sectional area, Dx is the distance and q is the heat rate, which is obtained from Equation 1.

 

Thermal Contact Resistance

 

The thermal contact resistance is directly proportional to the temperature gradient and inversely proportional to the heat flux, as indicated by the following equation

                                           (3)

where DT the temperature jumps across the contact point, and q is the heat transfer rate.