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34     Chapter 2  Structure of  Thermodynamics


                                           Thus we have demonstrated  the remarkable fact that equation 2.8-1 makes it
                                       possible to calculate all the thermodynamic  properties for a rnonotomic ideal gas
                                       without  electronic  excitation.  Here we  have considered  an ideal  monatomic  gas.
                                       but this illustrates  the general conclusion  that if  any thermodynamic potential  of
                                       a one-component  system can be determined as a function of  its natural variables,
                                       all of  the thermodynamic  properties of  the system can be calculated.
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