SOME CLASSICAL THERMODYANMICS RESULTS

John W. Dooley, Physics Department, Millersville University

MATHEMATICS GENERAL EXPERIMENTAL RESULTS THERMODYNAMIC CONSEQUENCES   IDEAL GAS CONSEQUENCES IDEAL GAS EXPERIMENTAL RESULTS
           
  Temperature can be measured. Absolute temperature scale is special and n is the proper measure of quantity.      
    n is evidence for the existence of microscopic structure     PV =nRT
  Adiabatic work is path-independent First Law: Internal energy exists and is a state variable.      
  Dissipative work is equivalent to heat Heat flow is energy transfer. dU=dQ-dW      
Identities based on the existence of an equation of state       PV^gamma = constant on adiabat gamma is constant for an ideal gas
        U is a function of T only. Free expansion of ideal gas has Delta T=0
    S IS A STATE VARIABLE   Integral dS round a Carnot cycle is zero  
  Heat flows from hot to cold Second Law of Thermodyanmics      
    No engine is more efficient than Carnot   Carnot engine efficiency  
    First Law for states      
Identities based on the existence of an equation of state, and the path-   MAXWELL RELATIONS      
independence of state variables   n is evidence for the existence of microscopic structure   Cp-Cv=nR (IDEAL) and Cp and Cv are constants gamma temperature independent
  Values for gamma for different gas species fall in clusters gamma variation is evidence for the existence of microscopic structure   Correct calculate of speed of sound in a gas allows determination of gamma  
    agrees with a particular microscopic model   U=3/2 nRT  
  u=sigma T^4 for black body radiation Prad = u/3 (RAD PRESS AGREES WITH EM THEORY)      
    Cv ~ T^3 (AGREES WITH HEAT CAP IN SOLIDS)      

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Last Updated on 5/18/98
By john w dooley