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296                             MIDSTREAM AND DOWNSTREAM OPERATIONS


                                             Fraction   Components  B.P. Range (°F)

                      Distillation        Gases           C 1 –C 4
                        tower


                                          Light naphtha   C 5 –C 6   90–190
                 Crude
                  oil                     Heavy naphtha  C 6 –C 12  190–330
                                          Kerosene       C 10 –C 16  330–480
                                          Diesel oils    C 14 –C 20  480–610

                                          Lubricants     C 20 –C 50  480–610
                     Furnace              Fuel oil       C 20 –C 70  610–700


                                          Residue         > C 70


           FIguRE 15.5  Typical distillation tower fractions and components. (Source: © energy.fanchi.
           com (2015).)

           lowermost section of the tower to approximately 90°F in the uppermost section of the
           tower as the vapor rises in the distillation tower. Each type of hydrocarbon compo-
           nent condenses from the vapor to the liquid state in a temperature range that depends
           on the boiling point of the molecule.
              The boiling point for a hydrocarbon molecule typically increases as the number of
           carbons in the molecule increases. The normal boiling points (measured at pressure
           equal to 1.00 atm) for straight chain, or normal, alkanes are shown in Figure 15.6
           starting with methane and ending with normal triacontane, n‐C H . Crude distilla-
                                                                 62
                                                              30
           tion towers typically operate near 30 psig, so the normal boiling points in Figure 15.6
           do not precisely reflect volatility for the conditions in the tower, but they do reflect
           relative volatility.
              The decline in temperature from the lowermost section of the tower to the
           uppermost section of the tower establishes sections of the tower with temperature
           ranges that are suitable for collecting hydrocarbons that condense in the tempera-
           ture range of a particular section. The liquid mixture collected at each section is
           the product stream for that section. Product streams vary from high molecular
           weight, viscous liquids at the base of the tower to low molecular weight gases at
           the top of the tower.
              We can model the separation of components that occurs in each section of the
           tower with the flash calculation explained in Chapter 11. The flash calculation starts
           with specification of feed composition and k‐values. The next step is the two‐phase
           check, which determines if the feed will separate to gas and liquid phases for the
           given k‐values. The final step is the flash calculation. These three steps are presented
           for a five‐component system in the following examples.
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