Page 123 - Physical chemistry understanding our chemical world
P. 123

90    ENERGY AND THE FIRST LAW OF THERMODYNAMICS

                      Alternatively, we could consider inflating the tyre with a series of, say, 100 short
                      steps – each separated by a short pause. The difference in pressure before and after
                      each of these small steps would be so slight that the gas within the tyre would be
                      allowed to reach equilibrium with its surroundings after adding each increment, and
                      before the next. Stated a different way, the difference between the pressure of the gas
                      in the hand pump and in the tyre will always be slight.
                                        We can take this idea further. We need to realize that if there is
              ‘Infinitesimal’ is the   no real difference in pressure between the hand pump and the gas
              reciprocal of infinite,  within the tyre, then no work would be needed to inflate because
              i.e. incredibly small.  there would never be the need to pump against a pressure. Alter-
                                      natively, if the inflation were accomplished at a rate so slow that it
                      was infinitesimally slow, then there would never be a difference in pressure, ensuring
                      w was always zero. And if w was zero, then U would stay constant per increment. (We
                      need to be aware that this argument requires us to perform the process isothermally.)
                        It should be clear that inflating a tyre under such conditions is never going to occur
                      in practice, because we would not have the time, and the inflation would never be
                      complete. But as a conceptual experiment, we see that working at an infinitesimally
                      slow rate does not constitute work in the thermodynamic sense.
                                        It is often useful to perform thought experiments of this type,
              A thermodynamic pro-    changing a thermodynamic variable at an infinitely slow rate: we
              cess is reversible if an  say we perform the change reversibly. (If we perform a process in a
              infinitesimal change in  non-reversible manner then we say it is ‘irreversible’.) As a simple
              an external variable    definition, a process is said to be reversible if the change occurs
              (e.g. pressure) can     at an infinitesimal rate, and if an infinitesimal change in an exter-
              change the direction    nal variable (such as pressure) could change the direction of the
              in which the process    thermodynamic process. It is seen that a change is only reversible
              occurs.
                                      if it occurs with the system and surroundings in equilibrium at
                                      all times. In practice this condition is never attained, but we can
                                      sometimes come quite close.
              The amount of work        Reversibility can be a fairly difficult concept to grasp, but it
              that can be performed   is invaluable. In fact, the amount of work that can be performed
              during a thermody-      during a thermodynamic process is maximized when performing
              namic process is maxi-  it reversibly.
              mized by performing it    The discussion here has focused on work done by changes in
              reversibly.             pressure, but we could equally have discussed it in terms of volume
                                      changes, electrical work (see Chapter 7) or chemical changes (see
                                      Chapter 4).



                       How fast does the air in an oven warm up?


                      Absorbing energy

                      The air inside an oven begins to get warm as soon as we switch it on. We can
                      regard the interior of the oven as a fixed system, so the internal energy U of the
   118   119   120   121   122   123   124   125   126   127   128