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is uniform. Once again, the sorted condition (fast molecules on one side,
             slow  on  the  other)  is  a  state  of  low  probability,  and  the-  uniform
             distribution  is  a  state  of  high  probability.  Upon  contact,  the  system
             evolves  spontaneously  from  a  state  of  low  probability  to  one  of  high

             probability.
             3. A stirred cup of coffee. Suppose that you stir a cup of coffee and then
             remove the spoon. Over time, the circulation of the liquid decreases and

             viscosity causes the energy of the rotating fluid to be dissipated as internal
             energy of the molecules. In the initial state there is an ordered motion of
             the  swirling  coffee.  In  the  final  equilibrium  state  there  is  a  random
             molecular motion. Once again, the ordered circulation of the molecules is

             a state of low probability, while the random disordered motion is a state of
             high probability. In this natural process, the system has gone from a state
             of low probability to a state of high probability.

               In all three cases above, the system has gone spontaneously from a state
             of low probability to one of high probability. All three of these situations
             are irreversible natural processes that are characterized by an increase in

             the  entropy  of  the  system.  It  is,  therefore,  reasonable  to  conclude  that
             there is a quantitative relationship between probability and entropy. This
             relationship, which was proposed by Boltzmann, is

                                                       S        k ln  P
            Here k is the Boltzmann constant, and S is the entropy of the system. P, to
            define it loosely, is the number of different molecular arrangements that
            correspond  to  the  same  macroscopic  state.  If,  for  example,  the

            circumstances are so special that only one arrangement is possible, then P
            = 1 and S (= k In P) = 0, and we have a completely ordered state. Larger
            values of P, such as that corresponding to the more uniform distribution

            of molecules in the container, give larger values of the entropy. When we
            say that state A of a system is more probable than state B, we simply mean
            that state A has a larger value of P.
               An increase in entropy has also been said to be a measure of the increase

             in the disorder of a system, and, thus, entropy is a measure of disorder.
             The term "disorder" does not have a precise mathematical definition, but
             it is qualitatively related to the probability. A state of low disorder is a

             state  in  which  the  components  of  a  system  have  been  carefully  sorted,
             such  as  by  placing  all  the  molecules  with  low  speeds  in  one  part  of  a
             system. A state of high disorder is a random state in which no sorting has

             occurred. The increase in entropy of a system in natural processes can,
             thus,  also  be  regarded  to  as  an  increase  in  the  level  of  disorder  of  the



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