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1 17. 2 17.1 Thermal Conduction in Metals and Alloys Classical Approach From the kinetic theory of gases ) where, l is mean free path.

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Presentation on theme: "1 17. 2 17.1 Thermal Conduction in Metals and Alloys Classical Approach From the kinetic theory of gases ) where, l is mean free path."— Presentation transcript:

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2 2 17.1 Thermal Conduction in Metals and Alloys Classical Approach From the kinetic theory of gases ) where, l is mean free path

3 3 Relation between the heat conductivity and, heat conductivity by electrons

4 4 17.2 Thermal Conduction in Metals and Alloys- Quantum Mechanical Considerations Do all the electrons participate in the heat conduction? No, only those electrons which have an energy close to the Fermi energy participate in the heat conduction since, (from previous chapter)

5 5 (Lorentz number) Since,

6 6 17.3 Thermal Conduction in Dielectric Materials Heat conduction in dielectric materials occurs by a flow of phonons. At low temperatures Only a few phonons exist, the thermal conductivity depends mainly on the heat capacity which increases with the low temperatures. At higher temperature The phonon-phonon interactions are dominant, the phonon density increases with increasing T. Thus the mean free path and the thermal conductivity decreases for temperatures

7 7 18

8 8 18 Thermal Expansion : Coefficient of linear expansion The length L of a rod increases with increasing temperature, Atomistic point of view For small temperature : a atom may rest in its equilibrium position As temperature increases the amplitudes of the vibrating atom increases Asymmetric Because potential curve is not symmetric, a atom moves farther apart from its neighbor

9 The End Exam: December 19 th. From 10:00 – 13:00 Part a and Part b A4 paper – summary of the class lecture for your own purpose.


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