Page 54 - Characterization and Properties of Petroleum Fractions - M.R. Riazi
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         34 CHARACTERIZATION AND PROPERTIES OF PETROLEUM FRACTIONS
         As discussed in Section 1.7.18, kinematic viscosity is ex-
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         pressed in cSt, SUS, and SFS units. Values of kinematic vis-  flash point greater than 80 C (ASTM D 92 or ISO 2592 test
                                                              methods). Flash point should not be mistaken with fire point,
         cosity for pure liquid hydrocarbons are usually measured and  which is defined as the minimum temperature at which the
         reported at two reference temperatures of 38 C (100 F) and  hydrocarbon will continue to burn for at least 5 s after being
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         99 C (210 F) in cSt. However, other reference temperatures  ignited by a flame.
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         of 40 C (104 F), 50 C (122 F), and 60 C (140 F) are also used
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         to report kinematic viscosities of petroleum fractions. Liq-  2.1.11 Autoignition Temperature
         uid viscosity decreases with an increase in temperature (see
         Section 2.7). Kinematic viscosity, as it is shown in Chapter 3,  This is the minimum temperature at which hydrocarbon va-
         is a useful characterization parameter, especially for heavy  por when mixed with air can spontaneously ignite without
         fractions in which the boiling point may not be available.  the presence of any external source. Values of autoignition
                                                              temperature are generally higher than flash point, as given
                                                              in Table 2.2 for some pure hydrocarbons. Values of autoigni-
         2.1.9 Freezing and Melting Points
                                                              tion temperature for oils obtained from mineral sources are
         Petroleum and most petroleum products are in the form of a  in the range of 150–320 C (300–500 F), for gasoline it is about
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         liquid or gas at ambient temperatures. However, for oils con-  350 C (660 F), and for alcohol is about 500 C (930 F) [7].
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         taining heavy compounds such as waxes or asphaltinic oils,  With an increase in pressure the autoignition temperature
         problems may arise from solidification, which cause the oil  decreases. This is particularly important from a safety point
         to lose its fluidity characteristics. For this reason knowledge  of view when hydrocarbons are compressed.
         of the freezing point is important and it is one of the ma-
         jor specifications of jet fuels and kerosenes. For a pure com-  2.1.12 Flammability Range
         pound the freezing point is the temperature at which liquid
         solidifies at 1 atm pressure. Similarly the melting point, T M ,  To have a combustion, three elements are required: fuel (hy-
         is the temperature that a solid substance liquefies at 1 atm.  drocarbon vapor), oxygen (i.e., air), and a spark to initiate the
         A pure substance has the same freezing and melting points;  combustion. One important parameter to have a good com-
         however, for petroleum mixtures, there are ranges of melting  bustion is the ratio of air to hydrocarbon fuel. The combustion
         and freezing points versus percent of the mixture melted or  does not occur if there is too much air (little fuel) or too lit-
         frozen. For a mixture, the initial melting point is close to the  tle air (too much fuel). This suggests that combustion occurs
         melting point of the lightest compound in the mixture, while  when hydrocarbon concentration in the air is within a certain
         the initial freezing point is close to the freezing point (or melt-  range. This range is called flammability range and is usually
         ing point) of the heaviest compound in the mixture. Since the  expressed in terms of lower and upper volume percent in the
         melting point increases with molecular weight, for petroleum  mixture of hydrocarbon vapor and air. The actual volume per-
         mixtures the initial freezing point is greater than the initial  cent of hydrocarbon vapor in the air may be calculated from
         melting point. For petroleum mixtures an equivalent term of  Eq. (2.11) using vapor pressure of the hydrocarbon. If the cal-
         pour point instead of initial melting point is defined, which  culated vol% of hydrocarbon in the air is within the flamma-
         will be discussed in Chapter 3. Melting point is an important  bility range then the mixture is flammable by a spark or flame.
         characteristic parameter for petroleum and paraffinic waxes.
                                                              2.1.13 Octane Number
         2.1.10 Flash Point
                                                              Octane number is a parameter defined to characterize an-
         Flash point, T F , for a hydrocarbon or a fuel is the minimum  tiknock characteristic of a fuel (gasoline) for spark ignition
         temperature at which vapor pressure of the hydrocarbon is  engines. Octane number is a measure of fuel’s ability to re-
         sufficient to produce the vapor needed for spontaneous igni-  sist auto-ignition during compression and prior to ignition.
         tion of the hydrocarbon with the air with the presence of an  Higher octane number fuels have better engine performance.
         external source, i.e., spark or flame. From this definition, it is  The octane number of a fuel is measured based on two ref-
         clear that hydrocarbons with higher vapor pressures (lighter  erence hydrocarbons of n-heptane with an assigned octane
         compounds) have lower flash points. Generally flash point  number of zero and isooctane (2,2,4-trimethylpentane) with
         increases with an increase in boiling point. Flash point is  assigned octane number of 100. A mixture of 70 vol% isooc-
         an important parameter for safety considerations, especially  tane and 30 vol% n-heptane has an octane number of 70.
         during storage and transportation of volatile petroleum prod-  There are two methods of measuring octane number of a fuel
         ucts (i.e., LPG, light naphtha, gasoline) in a high-temperature  in the laboratory. The methods are known as motor octane
         environment. The surrounding temperature around a storage  number (MON) and research octane number (RON). The MON
         tank should always be less than the flash point of the fuel  is indicative of high-speed performance (900 rpm) and is mea-
         to avoid possibility of ignition. Flash point is used as an in-  sured under heavy road conditions (ASTM D 357). The RON
         dication of the fire and explosion potential of a petroleum  is indicative of normal road performance under low engine
         product. Estimation of the flash point of petroleum fractions  speed (600 rpm) city driving conditions (ASTM D 908). The
         is discussed in Chapter 3, and data for flash points of some  third type of octane number is defined as posted octane num-
         pure hydrocarbons are given in Table 2.2. These data were ob-  ber (PON), which is the arithmetic average of the MON and
         tained using the closed cup apparatus as described in ASTM  RON [PON = (MON + RON)/2]. Generally isoparaffins have
         D 93 (ISO 2719) test method. There is another method of  higher octane number than do normal paraffins. Naphthenes
         measuring flash point known as open cup for those oils with  have relatively higher octane number than do corresponding
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