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                                           2. CHARACTERIZATION AND PROPERTIES OF PURE HYDROCARBONS 57
                                                         API Gravity









                                    Kinematic Viscosity at 100°F , cSt                Kinematic Viscosity at 210°F , cSt  Molecular Weight
             --`,```,`,``````,`,````,```,,-`-`,,`,,`,`,,`---







































                              FIG. 2.5—Estimation of molecular weight from Eq. (2.52). Taken from Ref. [67] with per-
                            mission.


            2.4.1.5 Goossens Correlation                          Eq. (2.38) but with a variable b and c =−1. Parameter b is
            Most recently Goossens [61] correlated M to T b and d 20 in the  considered as a function of T b , while SG in Eq. (2.38) is re-
                                                                           20
                                                                                                        20
                                                                                                    ◦
            following form using the data on 40 pure hydrocarbons and  placed by d 4  the specific gravity at 20/4 C(d 4  is the same
                                                                              3
            23 petroleum fractions:                               as d 20 in g/cm ). The data bank used to develop this equa-
                                                                  tion covers the carbon range of C 5 –C 120 (M ∼ 70–1700, T b ∼
                                         β
            (2.55)           M = 0.01077T /d 20                   300–1000 K, and d ∼ 0.63–1.08). For the same 63 data points
                                        b   4
                                                                  used to obtain the constants of Eq. (2.55), the average error
            where β = 1.52869 + 0.06486 ln[T b /(1078 − T b )]. Inspection  was 2.1%. However, practical application of Eq. (2.55) is lim-
            of this equation shows that it has the same structure as  ited to much lower molecular weight fractions because heavy











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