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





                               16                   Elementary Physical Chemistry



                                 Note: U is a state function, meaning it is independent of the previous
                                 history of the system but depends only on the current state and not
                                 on the way the state was formed. The quantities q and w are not state
                                 functions.
                                 There are other state functions, to be introduced later. All will be
                                 denoted by capital letters in contrast to the concepts of work and
                                 heat, which are denoted by small letters.



                               2.8. Exact and Inexact Differentials
                               The First Law is frequently expressed in differential form:

                                                         dU =dq +dw                        (2.9)
                               There is a difference between the differentials dU on the one hand and
                               dq and dw on the other hand. dU is an exact differential — its integral
                               depends only on the initial and final states of the system and not on the
                               path of integration. The differentials dq and dw are generally not exact.
                               Their integrated values depend on the path of integration.
                                  As an illustration of the meaning of exact and inexact differentials,
                               consider the integration of ydx (the horizontally shaded area) between the
                               limits A and B. Obviously, the value depends on the path of integration. The
                               same is true for the integral xdy. But the sum of these two is independent
                               of the path. This shows that individual integrals may be path-dependent,
                               but their sum could be path-independent (see Fig. 2.2).


















                                         Graphical representation of the sum of the integrals ∫ydx + ∫xdy.
                                Fig. 2.2
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