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Callister - An introduction - 8th edition

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Summary • 795<br />

• Coefficient-of-thermal-expansion values for polymers are typically greater than<br />

for metals, which in turn are greater than for ceramic materials.<br />

Thermal Conductivity<br />

• The transport of thermal energy from high- to low-temperature regions of a material<br />

is termed thermal conduction.<br />

• For steady-state heat transport, flux may be determined using Equation 19.5.<br />

• For solid materials, heat is transported by free electrons and by vibrational lattice<br />

waves, or phonons.<br />

• The high thermal conductivities for relatively pure metals are due to the large numbers<br />

of free electrons and the efficiency with which these electrons transport thermal<br />

energy. By way of contrast, ceramics and polymers are poor thermal conductors<br />

because free-electron concentrations are low and phonon conduction predominates.<br />

Thermal Stresses<br />

• Thermal stresses, which are introduced in a body as a consequence of temperature<br />

changes, may lead to fracture or undesirable plastic deformation.<br />

• One source of thermal stresses is the restrained thermal expansion (or contraction)<br />

of a body. Stress magnitude may be computed using Equation 19.8.<br />

• The generation of thermal stresses resulting from the rapid heating or cooling of<br />

a body of material result from temperature gradients between the outside and<br />

interior portions and accompanying differential dimensional changes.<br />

• Thermal shock is the fracture of a body resulting from thermal stresses induced<br />

by rapid temperature changes. Because ceramic materials are brittle, they are especially<br />

susceptible to this type of failure.<br />

Equation Summary<br />

Equation<br />

Page<br />

Number Equation Solving for Number<br />

19.1 C dQ<br />

dT<br />

Definition of heat capacity 782<br />

19.3a<br />

19.3b<br />

l f l 0<br />

l 0<br />

a l 1T f T 0 2<br />

¢l<br />

l 0<br />

a l ¢T<br />

Definition of linear coefficient of thermal<br />

expansion<br />

785<br />

19.4<br />

¢V<br />

V 0<br />

a y ¢T<br />

Definition of volume coefficient of thermal<br />

expansion<br />

786<br />

19.5 q k dT<br />

dx<br />

Definition of thermal conductivity 789<br />

19.8<br />

s Ea l 1T 0 T f 2<br />

Ea l ¢T<br />

Thermal stress 792<br />

19.9<br />

s f k<br />

TSR <br />

Ea l<br />

Thermal shock resistance parameter 794

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