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192    PHASE EQUILIBRIA

                      of the gas is possible. We say that there cannot be any CO 2(l) at temperatures above
                      T (critical) .
                        Furthermore, supercritical CO 2 does not behave as merely a mixture of liquid
                      and gaseous CO 2 , but often exhibits an exceptional ability to solvate molecules in
                      a specific way. The removal of caffeine from coffee relies on the chromatographic
                      separation of caffeine and the other organic substances in a coffee bean; supercritical
                      fluid chromatography is a growing and exciting branch of chemistry.


              5.3     Quantitative effects of pressure
                      and temperature change
                      for a single-component system


                       Why is ice so slippery?

                      Effect of p and T on the position of a solid–liquid equilibrium


                                      We say something is ‘as slippery as an ice rink’ if it is has a tiny
              The coefficient of fric-  coefficient of friction, and we cannot get a grip underfoot. This is
              tion µ (also called
              ‘friction factor’) is the  odd because the coefficient of friction µ for ice is quite high – try
              quotient of the fric-   dragging a fingernail along the surface of some ice fresh from the
              tional force and the    ice box. It requires quite a lot of effort (and hence work) for a
              normal force. In other  body to move over the surface of ice.
              words, when we apply a    At first sight, these facts appear to represent a contradiction in
              force, is there a resis-  terms. In fact, the reason why it is so easy to slip on ice is that ice
              tance to movement       usually has a thin layer of liquid water covering its surface: it is
              or not?                 this water–ice combination that is treacherous and slippery.
                                        But why does any water form on the ice if the weather is
                      sufficiently cold for water to have frozen to form ice? Consider the ice directly
                      beneath the blade on a skater’s ice-shoe in Figure 5.9: the edge of the blade is
                      so sharp that an enormous pressure is exerted on the ice, as indicated by the grey
                      tints.
                                        We now look at the phase diagram for water in Figure 5.10.
              The sign of dp/dT for   Ice melts at 0 C if the pressure is p  O  (as represented by T 1 and
                                                   ◦
              the liquid–solid line   p 1 respectively on the figure). If the pressure exerted on the ice
              on a phase diagram      increases to p 2 , then the freezing temperature decreases to T 2 .(The
              is almost always posi-  freezing temperature decreases in response to the negative slope
              tive. Water is the only
                                      of the liquid–solid phase boundary (see the inset to Figure 5.10),
              common exception.
                                      which is most unusual; virtually all other substances show a posi-
                                      tive slope of dp/dT .)
                        If the temperature T 2 is lower than the freezing temperature of the water – and it
                      usually is – then some of the ice converts to form liquid water; squeezing decreases
                      the freezing temperature of the water. The water-on-ice beneath the skater’s blade is
                      slippery enough to allow effortless skating.
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