2. Fig 1.16 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

3. Fig 1.17 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

4. MOLAR HEAT CAPACITY C m monatomic diatomic solid

5. Fig 1.18 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

6. Fig 1.21 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

7. Fig 1.22 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) Mawell- Boltzmann Distribution

8. # of atoms per unit volume per unit energy at an energy E  

9. Fig 1.23 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) The mean energy is (3/2) kT  monatomic gas with three degrees of freedom

10. N = total number of molecules, n E dE = the fraction of the particles in the range E to (E + dE) then we can answer the question: “What is the probability, given a molecule, that its energy is in the range from E to (E+dE)?”

11. Fig 1.24 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

12. Fig 1.25 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005)

13. Fig 1.26 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) Random motion of conduction electrons in a conductor results in electrical noise.

14. Fig 1.27 From Principles of Electronic Materials and Devices, Third Edition, S.O. Kasap (© McGraw-Hill, 2005) Charging and discharging of a capacitor by a conductor due to the random thermal motions of the conduction electrons.