Introduction to Conduction
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Chapter 2 Page 1
Introduction to Conduction
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Chapter 2 Page 2
Fourier's Law of Heat Conduction
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Chapter 2 Page 3
Sample Problem
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Chapter 2 Page 4
Sample Problem
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The Conduction Rate Equation
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Chapter 2 Page 6
The Conduction Rate Equation
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Chapter 2 Page 7
Thermal Properties of Matter
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Chapter 2 Page 8
Thermal Properties of Matter
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To a first approximation, ke is inversely proportional to the
electrical resistivity.
For pure metals, which are of low resistivity, ke is much
larger than kph.
In contrast, for alloys, which are of substantially resistivity,
the contribution of kph to k is no longer negligible.
For nonmetallic solids, k is determined primarily by kph.
The regularity of the lattice arrangement has an important
effect on kph, with crystalline (well-ordered) materials like
quartz having a higher thermal conductivity than
amorphous materials like glass.
In fact, for crystalline, nonmetallic solids such as diamond
and beryllium oxide, kph can be quite large, exceeding
values of k associated with good conductors, such as
aluminum and copper.
Values for selected materials of technical importance
are also provided in Table A.1 (metallic solids) and Tables
A.2 and A.3 (nonmetallic solids).
Chapter 2 Page 9
Thermal Properties of Matter
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Chapter 2 Page 10
Thermal Properties of Matter
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Chapter 2 Page 11