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August 25, 2010 9:36      9in x 6in     b985-ch02      Elementary Physical Chemistry





                               14                   Elementary Physical Chemistry

                               2.5. Reversible Process

                               When the internal pressure P is equal to the external one P ext, the system
                               is said to be in a state of equilibrium. An infinitesimal increase in P ext will
                               result in an increase in compression and an infinitesimal decrease in P ext
                               will result in an increase in expansion. A reversible process is a process
                               which proceeds through a succession of equilibrium states.
                                  If an ideal gas is in equilibrium with its surroundings, then P ext = P
                               and, for an ideal gas, P = nRT/V . Therefore, the work (done by the
                               surrounding on the system) in a reversible change is

                                             w PV = −∫(nRT/V )dV = −nRT ln V f /V i        (2.4)
                               Note again that the work is positive in a compression (V f <V i ) and negative
                               in an expansion (V f >V i ).

                               2.6. Measurement of Heat
                               The traditional way to discuss the concepts of temperature and heat is
                               to define one of these and deduce the other from it. Attempts to define
                               temperature in terms of heat are bound to cause difficulties since normally
                               heat is not observed directly but inferred from changes in temperature.
                               Statements such as radiant energy, thermal heat flow, are sometimes used
                               in defining heat. Using such descriptions of heat to define temperature is
                               obviously not very satisfactory and will be avoided here.


                                 Comment: The concept of heat is most conveniently described in
                                 terms of the heat capacity, which is the heat divided by the
                                 temperature change (Section 10). Here, we introduce the concept by
                                 focusing directly on temperature changes of two systems in thermal
                                 equilibrium.


                                  Consider a system, A, initially at a temperature T A in equilibrium with
                               a system, B, whose initial temperature is T B . If the equilibrium temperature
                               is T , small changes in temperature of the two systems can be written as
                               dT A = T − T A and dT B = T − T B . The ratio of these quantities defines the
                               ratio of the heat capacities,thatis

                                                      dT A /dT B = −C A /C B               (2.5)
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