Page 129 - Hydrocarbon Exploration and Production Second Edition
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116                                                          Reservoir Fluids


                                                 compressed
                                                    liquid
                                                               critical
                                                               point
                     P c


                                                               superheated
                                          curve                  vapour
                                                                 or gas
                             SOLID            LIQUID
                      Pressure           Melting  point  A  B






                                                  VAPOUR
                                              A'
                                          triple
                                          point

                                         Temperature         T
                                                             c
                           sublimation curve         vapor pressure curve
          Figure 6.17  Pressure^temperature phase diagram.

             Figure 6.17 shows the phase boundaries between the component in the solid,
          liquid and gas (vapour) states. Starting with the liquid (water) at point A, as the
          temperature is increased the boiling point is approached until the boiling point curve
          is reached, at which point the water boils and turns to steam (gas). Starting from the
          situation of the gaseous phase at point B, if the temperature is reduced the dew point
          curve is approached, and when the dew point is reached, the component changes
          from the gaseous phase to the liquid phase. For a single component, the boiling
          point curve and the dew point curve are coincident, and are known as the vapour
          pressure curve. Of course the phase boundary between the liquid and solid phases is
          the melting point curve.
             At the triple point all three phases can co-exist, and this point is a unique property
          of pure substances. At the critical point, defined by the critical temperature (T c )and
          pressure (P c ), it becomes impossible to distinguish between the gaseous and liquid
          phases; the highly compressed gas has the same density and appearance as a high-
          temperature liquid. The effect of the increased pressure and attractive forces between
          molecules is to move molecules together and increase the density (as when a gas
          becomes a liquid), but the increasing temperature increases the kinetic energy of the
          molecules and tends to drive them apart, thus reducing the density (as when a liquid
          becomes a gas). At the critical point, the phases become indistinguishable, and beyond
          the critical point just one state exists, and is usually referred to as a supercritical fluid.
             In the production of hydrocarbon reservoirs, the process of isothermal depletion
          is normally assumed, that is reducing the pressure of the system whilst maintaining
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