Page 28 - Bruno Linder Elementary Physical Chemistry
P. 28

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





                                              The First Law of Thermodynamics              13

                            2.4. Measurement of Work

                            Work is distance times force. Force is mass times acceleration.
                            The following are examples of work:

                            a) When lifting an object, a force must be applied in the direction away
                              from the earth, which is equal to the mass times the gravitational
                              acceleration, i.e. m × g. If the object moves a distance h,the work
                              done by the surrounding on the system is

                                                        w = h × mg                      (2.1)
                            b) When a gas in a cylinder (see Fig. 2.1) is compressed, the piston, acted
                              on by the external force f ext ,moves a distance dx in the direction
                               of f ext. The external pressure on the piston of area A is P ext =
                               f ext /A. The piston is displaced a distance dx in the direction of the
                              force, f ext.

                               The change in the volume of the system is dV = −Adx.(The
                            negative sign is introduced because the final volume V f is smaller than
                            the initial volume V i .) Accordingly, the work done by the surrounding on
                            the system is

                                              dw PV =(f ext/A)Adx = −P extdV            (2.2)

                               For constant P ext the integrated value is

                                                     w PV = −P ext∆V                    (2.3)

                            where ∆V = V f − V i . Obviously, the maximum work is obtained when the
                            internal gas pressure is infinitesimally less than the external. If greater,
                            compression cannot occur.













                                                    Compression of a gas by piston.
                                           Fig. 2.1
   23   24   25   26   27   28   29   30   31   32   33