Equilibrium Statistical Physics, Plischke ex. 1.2

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SUMMARY

The forum discussion centers on solving a problem from Plischke's "Equilibrium Statistical Physics," specifically example 1.2. The key equation derived is the integral of heat capacity over temperature, expressed as $$C_M \ln T$$. Participants clarify that the integration of $$\frac{C_M}{T}$$ leads to this logarithmic relationship, emphasizing the importance of understanding the limits of integration from initial temperature $$T_i$$ to final temperature $$T_f$$. The discussion highlights the necessity of recognizing the mathematical steps involved in this derivation.

PREREQUISITES
  • Understanding of integral calculus, particularly logarithmic integrals.
  • Familiarity with concepts of heat capacity in thermodynamics.
  • Knowledge of statistical mechanics principles as outlined in "Equilibrium Statistical Physics."
  • Ability to interpret mathematical expressions and equations in physics.
NEXT STEPS
  • Review the derivation of logarithmic integrals in calculus.
  • Study the relationship between heat capacity and temperature in thermodynamic systems.
  • Explore additional examples from Plischke's "Equilibrium Statistical Physics" for deeper understanding.
  • Investigate the applications of statistical mechanics in real-world physical systems.
USEFUL FOR

This discussion is beneficial for physics students, educators, and researchers focusing on statistical mechanics and thermodynamics, particularly those working with concepts from "Equilibrium Statistical Physics."

percolator
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Homework Statement



See: attached imageHow do we get the final equation? I'm obviously missing out on something..
 

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$$
\int_{T_i}^{T_f} dT \left( \frac{C_M}{T} \right) = C_M \int_{T_i}^{T_f} \frac{dT}{T} = C_M \ln T
$$
Can you take it from there?
 
yeah, thanks!
 

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