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Vapor-liquid crude mixture

Distillation may be defined as the separation of the constituents of a liquid mixture by partial vaporization of the mixture, followed by separate recovery of the vapor and liquid residue. Since crude petroleum is the most complex mixture of liquids found in nature, it is not surprising that distillation is one of the most important processes in modem petroleum refining. [Pg.70]

Figure 10. Vapor-liquid equilibria for an argon-krypton mixture (modeled as a Lennard-Jones mixture) for the bulk fluid (R = >) and for a cylindrical pore of radius R = / /Oaa = 2.5. The dotted and dashed lines are from a crude form of density functional theory (the local density approximation, LDA). The points and solid lines are molecular dynamics results for the pore. Reprinted with permission from W. L. Jorgensen and J. Tirado-Rives, J. Am. Chem. Soc. Figure 10. Vapor-liquid equilibria for an argon-krypton mixture (modeled as a Lennard-Jones mixture) for the bulk fluid (R = >) and for a cylindrical pore of radius R = / /Oaa = 2.5. The dotted and dashed lines are from a crude form of density functional theory (the local density approximation, LDA). The points and solid lines are molecular dynamics results for the pore. Reprinted with permission from W. L. Jorgensen and J. Tirado-Rives, J. Am. Chem. Soc.
Distillation is a unit operation that separates by vaporization liquid mixtures of miscible and volatile substances into individual components or groups of components. The separation of water and alcohol into the respective components of liquid air into nitrogen, oxygen, and argon and the separation of crude petroleum into gasoline, oil, and kerosene are examples of the distillation unit operation. [Pg.434]

Many specially designed arc apparatus have been patented for the plasma treatment of petroleum fractions146- 151 Some of these permit cracking gas-liquid mixtures or gas-solid mixtures in continuous process with recycling of undecomposed petroleum. In one such device147 crude oil is mixed with an energy transfer medium (rare gas, alkali metal vapor) and the mixture formed into particles which are fed through the hollow cathode of an electrical arc sustained in the transfer medium. [Pg.19]

Consequently, the continuous variation of specific volume of the vapor-liquid mixture at fixed temperature and pressure is a result of the continuous change in the fraction of the mixture that is vapor. The conclusion, then, is that an isotherm such as that shown in Fig. 7.3-2 is an approximate representation of the real phase behavior (shown in Fig. 7.3-3) by a relatively simple analytic equation of state. In fact, it is impossible to represent the discontinuities in the derivative dP/dV)T that occur at and v with any analytic equation of state. By its sigmoidal behavior in the two-phase region, the van der Waals equation of state is somewhat qualitatively and crudely exhibiting the essential features of vapor-liquid phase equilibrium historically, it was the first equation of state to do so. [Pg.286]

Prior to using the Peng-Robinson Equation of State for vapor-liquid equilibria calculations, the Equation of State parameters for each component were tuned using PVT data for oil. Once the Equation of State has been tuned, the mixture of crude oil and solvent is flashed at desired pressure and temperature to determine the composition of liquid phase. Coat s PVT simulator was used for this purpose. [Pg.18]

As far as the oil phase is concerned, it is, with rare exception, always a mixture, sometimes an awkward one like a crude oil. Also in this case, it has been recently understood that there can exist some individual behavior among oil molecules and that a mixture would not behave as a pure component provided that there is an opportunity to do so [60]. This behavior is not exceptional but rather the normal one. For instance, in the well-known vapor-liquid equilibrium, the difference in composition between the two phases is the fundamental concept underlying the distillation processes. Such a situation could be found also in liquid-liquid phase equilibria. [Pg.270]

As already mentioned, there are two general approaches to cooling the cell, immersion in the coolant and pumping coolant through the cell jacket. The simplest approach [21,27] for immersion is to use standard slush baths or salt-ice mixtures that are available for temperatures down to -160°C [28]. Crude but effective control of temperature can be achieved by cooling the cell in liquid nitrogen followed by slow warm-up in the vapor above the boiling liquid [5]. [Pg.502]

The materials of construction of the radiant coil are highly heat-resistant steel alloys, such as Sicromal containing 25% Cr, 20% Ni, and 2% Si. Triethyl phosphate [78-40-0] catalyst is injected into the acetic acid vapor. Ammonia [7664-41-7] is added to the gas mixture leaving the furnace to neutralize the catalyst and thus prevent ketene and water from recombining. The crude ketene obtained from this process contains water, acetic acid, acetic anhydride, and 7 vol % other gases (mainly carbon monoxide [630-08-0], carbon dioxide [124-38-9], ethylene [74-85-1], and methane [74-82-8]). The gas mixture is chilled to less than 100°C to remove water, unconverted acetic acid, and the acetic anhydride formed as a liquid phase (52,53). [Pg.475]

A somewhat more complicated situation occurs if a liquid process fluid made up of several components (e.g., crude oil) is to be partially vaporized, possibly as a feed to a distillation column. The liquid heats up sensibly until it reaches the temperature at which the first bubble of vapor is formed this temperature is the bubble point (see Fig. lc). The bubble is richer than the liquid in the more volatile components of the mixture. As heating continues, more vapor is formed and the temperature continues to... [Pg.306]

A mixture of hydrocarbons such as petroleum does not boil at a single, sharply defined temperature. Instead, as such a mixture is heated, the compounds with lower boiling points (the most volatile) boil off first, and as the temperature increases, more and more of the material vaporizes. The existence of a boiling-point range permits components of a mixture to be separated by distillation (see discussion in Section 11.6). The earliest petroleum distillation was a simple batch process The crude oil was heated in a still, the volatile fractions were removed at the top and condensed to gasoline, and the still was cleaned for another batch. Modern petroleum refineries use much more sophisticated and efficient distillation methods, in which crude oil is added continuously and fractions of different volatility are tapped off at various points up and down the distillation column (Fig. 7.5). To save on energy costs, heat exchangers capture the heat liberated from condensation of the liquid products. [Pg.278]

To separate important components of petroleum using fractional distillation, petroleum or hot crude oil is heated in a furnace. The liquid alkanes are vaporized and allowed to rise In the fractionating tower. Gases that were dissolved in the petroleum are removed at the top of the tower and condensed into liquids that are sold In cylinders. Gasoline is part of the next-lower group of materials drawn off. Below the gasoline fraction come mixtures of heavier hydrocarbons, such as kerosene, fuel and lubricating oils, and asphalt. [Pg.638]

Crude tall oil is a mixture of fatty acids, resin acids, and neutrals (i.e., no carboxylic acid functionality). The background section relates that neutrals interfere with the separation of the fatty acids from the resin acids and in industrial practice the neutrals are removed by molecul distillation. However, it is difficult to separate the neutrals from the other components because of vapor pressure similarity considerations. Tall oil soap, the precursor to crude tall oil, is a pasty emulsion of the neutrals and the sodium salts of the fatty and resin acids. The patent states that it is possible to extract neutrals from the soap with a liquid hydrocarbon solvent, but the prior art discussion relates that subsequent liquid hydrocarbon solvent recovery steps are relatively difficult. The neutrals can be separated from the soaps by a hydrocarbon solvent, incidentally, because the neutrals are lipophiles whereas the soaps are ionic and do not dissolve in the hydrocarbon. Similarly the neutrals will dissolve in a supercritical fluid like ethylene, or propane, or the chlorofluorocarbons, and the use of these gases in the supercritical state is the invention. Like the case of liquid hydrocarbon solvents, the ionic soap compounds will not dissolve in the supercritical gases. CO2 is specifically not listed among the gases, and we shall discuss the case of CO2 extraction of the emulsion later which is the subject of the next patent. [Pg.438]

Four fractions of pseudo-compounds are obtained by solution analysis of crude oil residue or its cracked product. During solution analysis of the cracking product from thermal treatment of vacuum residue or mixtures of vacuum residue and plastics (such mixtures were used in our investigation), a first step of solution analysis is soxhlet extraction. In the soxhlet extractor, the liquid/solid product is extracted with fresh warm solvent (THF) that does not contain the extract. This can increase the extraction rate, as the sample is contacting fresh warm solvent. The sample is placed inside a cellulose thimble and placed in the extractor. The extractor is connected to a flask containing the extraction solvent, and a condenser is connected above the extractor. The solvent is boiled, and the extractor has a bypass arm that the vapor passes through to reach the condenser, where it condenses and drips into the sample in the thimble. Once the solvent reaches the top of the siphon arm, the solvent and extract are siphoned back into the lower flask. The solvent reboils, and the cycle is repeated until the sample is completely extracted, and the extract is in the lower flask. [Pg.343]


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