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Thermal Properties of Materials

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Presentation on theme: "Thermal Properties of Materials"— Presentation transcript:

1 Thermal Properties of Materials
Chapter 22: Thermal Properties of Materials Chapter 22: Thermal Properties of Materials © 2011 Cengage Learning Engineering. All Rights Reserved.

2 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Learning Objectives Heat capacity and specific heat Thermal expansion Thermal conductivity Thermal shock © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 2

3 Heat Capacity and Specific Heat
Chapter 22: Thermal Properties of Materials Heat Capacity and Specific Heat Phonons Packets of elastic waves. They are characterized by their energy, wavelength, or frequency, which transfers energy through a material. The energy of the phonon can be expressed in terms of the wavelength or frequency. Specific heat The energy required to raise the temperature of one gram of a material by one degree. © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 3

4 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22.1 Heat capacity as a function of temperature for metals and ceramics. © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 4

5 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22.2 The effect of temperature on the specific heat of iron. Both the change in crystal structure and the change from ferromagnetic to paramagnetic behavior are indicated. © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 5

6 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Thermal Expansion Linear co-efficient of thermal expansion Describes the amount by which each unit length of a material changes when the temperature of the material changes by one degree. © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 6

7 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22.4 The linear coefficient of thermal expansion of iron changes abruptly at temperatures where an allotropic transformation occurs. (b) The expansion of Invar is very low due to the magnetic properties of the material at low temperatures. Thermal stresses are related to the coefficient of thermal expansion, the modulus of elasticity E of the material, and the temperature change T: thermal = ET © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 7

8 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22.5 When one end of a bar is heated, a heat flux Q/A flows toward the cold end at a rate determined by the temperature gradient produced in the bar. The thermal conductivity k is a measure of the rate at which heat is transferred through a material. Q/A = k T/x © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 8

9 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Thermal Conductivity Metals where L is the Lorentz constant - The constant that relates electrical and thermal conductivity. Ceramics The transfer of heat in ceramics occurs primarily by lattice vibrations (or phonons). Semiconductors Heat is conducted in semiconductors by both phonons and electrons. Polymers The thermal conductivity of polymers is very low—even in comparison with silicate glasses. © 2011 Cengage Learning Engineering. All Rights Reserved. 22 - 9

10 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22.6 The effect of temperature on the thermal conductivity of selected materials. Note the log scale on the vertical axis. © 2011 Cengage Learning Engineering. All Rights Reserved.

11 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Thermal Shock Failure of a material caused by stresses introduced by sudden changes in temperature is known as thermal shock. Thermal shock behavior is affected by several factors: Coefficient of thermal expansion: A low coefficient minimizes dimensional changes and reduces the ability to withstand thermal shock. Thermal conductivity: The magnitude of the temperature gradient is determined partly by the thermal conductivity of the material. © 2011 Cengage Learning Engineering. All Rights Reserved.

12 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Thermal Shock Modulus of elasticity: A low modulus of elasticity permits large amounts of strain before the stress reaches the critical level required to cause fracture. Fracture stress: A high stress required for fracture permits larger strains. Phase transformations: Additional dimensional changes can be caused by phase transformations. © 2011 Cengage Learning Engineering. All Rights Reserved.

13 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Figure 22-7 The effect of quenching temperature difference on the modulus of rupture of sialon. The thermal shock resistance of the ceramic is good up to about 950°C. © 2011 Cengage Learning Engineering. All Rights Reserved.

14 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Thermal Shock Thermal shock parameter or where f fracture stress of the material v Poisson’s ratio k thermal conductivity E modulus of elasticity  linear coefficient of thermal expansion © 2011 Cengage Learning Engineering. All Rights Reserved.

15 © 2011 Cengage Learning Engineering. All Rights Reserved.
Chapter 22: Thermal Properties of Materials Key Terms Phonons Heat capacity or specific heat Linear coefficient of thermal expansion Thermal stresses Thermal conductivity Lorentz constant Thermal shock © 2011 Cengage Learning Engineering. All Rights Reserved.


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