The world of thermodynamics
 
  Fundamentals
Temperature
Heat and Thermodynamics
The Kinetic Theory
Thermal Radiation
The First Law
The Second Law
The Third Law
Black Hole Thermodinamics
 
 
 

    The third law of thermodynamics states that the entropy of a pure perfect crystal is 0 at 0 K: ? S(0K) = 0. At 0K the atoms in a pure perfect crystal are aligned perfectly and do not move. Moreover, there is no entropy of mixing since the crystal is pure. For a mixed crystal containing the atomic or molecular species A and B, there are many possible arrangements of A and B and there is therefore entropy associated with the arrangement of the atoms/molecules.

    As with any good scientific law, there are exceptions. The following are exceptions to the third law of thermodynamics:

  • C=O: carbon monoxide molecules can align in various ways in a crystal, so there is entropy associated with C=O crystals at 0K. In this case, A and B are equally probable and the following equation can be used to calculate the entropy (called residual energy): S = nR [ 1/2 ln(1/2) + 1/2 ln (1/2) ] = -nRln2
  • Glasses: glass is actually disorded microscopically, so it's not a pure perfect crystal.

    It's useful to know the temperature dependence of S (along with other thermodynamic parameters) so you can do experiments at a few temperatures and calculate the S for any temperature.

 
 

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