2) It can be proven that the multiplicity of a large Einstein solid in the low-temperature limit (q <<< N) is 'eN\9 given by = For convenience we write the internal energy as U = qe, where e is the size of each energy unit (measured in eV or Joules). Use the definition of entropy, and then the definition of temperature to solve for the internal energy as a function of temperature. HINT: If you didn't get U Nee-/KT the first time, try again. Answers: U = Nee¯€/kT¸
2) It can be proven that the multiplicity of a large Einstein solid in the low-temperature limit (q <<< N) is 'eN\9 given by = For convenience we write the internal energy as U = qe, where e is the size of each energy unit (measured in eV or Joules). Use the definition of entropy, and then the definition of temperature to solve for the internal energy as a function of temperature. HINT: If you didn't get U Nee-/KT the first time, try again. Answers: U = Nee¯€/kT¸
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Transcribed Image Text:2) It can be proven that the multiplicity of a large Einstein solid in the low-temperature limit (q <<< N) is
'eN\9
given by =
For convenience we write the internal energy as U = qe, where e is the size of
each energy unit (measured in eV or Joules). Use the definition of entropy, and then the definition of
temperature to solve for the internal energy as a function of temperature.
HINT: If you didn't get U
Nee-/KT the first time, try again.
Answers:
U = Nee¯€/kT¸
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