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Solvent separated methane

Adsorption of solvent with activated charcoal. This is the most modern method of solvent recovery. It was introduced after World War I and immediately attracted attention by the exceptionally high recovery obtained, amounting to approximately 98% of the solvent entering the plant. The first plants using activated charcoal were used extensively in the oil industry for separating methane from heavier fractions in natural gas. [Pg.604]

Figure 15.4. Potential of mean force (PMF) between two methane molecules in water. This shows a first deeper minimum corresponding to the contact geometry of the two methane molecules. Another second (less deep) minimum is also observed in the PMF, corresponding to the solvent separated minimmn. Adapted from thesis entitled Molecular dynamics simulations of hydrophobic solutes in hquid water by Andy Hsu, Institute of Atomic and Molecular Sciences, Academia Sinica. (http //w3.iams.sinica.edu.tw/lab/jlli/thesis andy/%5d.)... Figure 15.4. Potential of mean force (PMF) between two methane molecules in water. This shows a first deeper minimum corresponding to the contact geometry of the two methane molecules. Another second (less deep) minimum is also observed in the PMF, corresponding to the solvent separated minimmn. Adapted from thesis entitled Molecular dynamics simulations of hydrophobic solutes in hquid water by Andy Hsu, Institute of Atomic and Molecular Sciences, Academia Sinica. (http //w3.iams.sinica.edu.tw/lab/jlli/thesis andy/%5d.)...
In the same figure we also show the distance dependence of the effective interaction energy between the two spheres. The results have been obtained by eomputer simulations where the spheres are methane molecules. Note the pronounced minimum between the two spheres at contact and then the maximum at intermediate distances. The interaction energy falls off to zero as the two spheres move away. In some cases, one finds a second minimum at a distance beyond the maximum [10]. Such a minimum at a larger separation is referred to as a solvent separated pair and arises due to the structuring around the hydrophobic spheres. [Pg.223]

In the solvent-separated configuration shown in Fig. 4.24a, the distance between the methane groups is about 7 A. On... [Pg.487]

For water to form the solvent-separated pair, let l , be the minimum distance to be accommodated in the aqueous core region of the reverse micelle. From the pair correlation function between methane and the oxygen, the location of the first minima is observed (Rao et al. 2007) at a distance of Iso = 5.6 k. Fet Ir be the distance between atomic centers of the solute atoms in the solvent-separated configuration, hence the minimum distance, l , = l, + 24. For the case of methane in the solvent-separated configuration in free water, 1 = 1 k and = 18.2 A. For the contact pair, 4 = 3.95 A and the corresponding value of = 15.15 A. From the water density distributions in the reverse micelle. [Pg.198]

Upon going to solution in methane (w = 9)—a model of nonpolar and nonpolarizable solvent—the minima on the PES, which are associated with the ion pairs, vanish. The effect of the solvent is felt only in some lowering of the calculated dissociation energy. So as to assess the role of a nonpolar but readily polarizable solvent, the authors of Ref. [67] chose H2(n = 11). The calculation revealed, apart from solvated undissocated CH3F, only one additional minimum at r p = 2.92 A, = 5, /c = 6. In this structure, one H2 molecule is incorporated into the cavity between the ions, and this sytem may be represented as a solvent-separated ion pair in which one solvent molecule is shared by two solvation shells formed upon ionic dissociation. [Pg.131]

The most noteworthy prediction of the PC theory was the potential of mean force for model methane pairs in water (Figure 5). This was the first molecularly realistic prediction of a potential of mean force between hydrophobic spheres in water. It showed structural oscillations that are natural features of these functions in simpler liquids a solvent-separated minimum free energy configuration, a thermally substantial barrier to desolvation, and a free energy minimum at contact of the two methane molecules. These qualitative features of the potential of mean force between spherical hydrophobic solutes have subsequently been observed in simulation many times. The result shown in Figure 5 was produced with the two-moment ITM, is substantially the same as the prediction of PC, and is in good agreement with the available computer simulation data. [Pg.1292]

Condensable hydrocarbons are removed from natural gas by cooling the gas to a low temperature and then by washing it with a cold hydrocarbon hquid to absorb the condensables. The uncondensed gas (mainly methane with a small amount of ethane) is classified as natural gas. The condensable hydrocarbons (ethane and heavier hydrocarbons) are stripped from the solvent and are separated into two streams. The heavier stream, which largely contains propane with some ethane and butane, can be Hquefied and is marketed as Hquefied petroleum gas (LPG) (qv). The heavier fractions, which consist of and heavier hydrocarbons, are added to gasoline to control volatihty (see Gasoline and other motor fuels). [Pg.399]

The quantity measured in the experimental work on the methane derivatives was the rotation of the Na D-line in ethanol solution (sometimes it was necessary to use another solvent, in which case a correction was applied). The sum (5), as well as its separate terms, was evaluated for 13 different choices of the set of ligands a,b,c,d,x. For eleven of these, the observed sum was less in absolute value than its statistical average calculated from the absolute values of the separate terms. For the other two (as well as for some of the eleven), the mixture contained molecules for which one would expect large deviations from T,rsymmetry, and/or dimerization. For those mixtures for which the sum (5) was small, a least-square fit was made to the data with a function of the form (2). This best fit was interpreted as the T -component, the remainder as the result of deviation from T -symmetry for each molecule. A fit was also made with functions of the form (1), with less quantitative success. [Pg.75]

To Fmoc 0-glycosyl threonine (erf-butyl ester 20 (290 mg, 0.4 mmol) dissolved in dry dichloromethane (5 mL) is added dry trifluoroacetic acid (3 mL) at 0°C. The mixture is allowed to warm to room temperature, and the reaction is monitored by TLC (dichloro-methane-ethanol 10 1). After 3 h, the conversion is complete. The solvent is evaporated in vacuo. Toluene (10 mL) is codistilled in vacuo from the remainder. Small amounts of an unpolar impurity are separated by flash chromatography on silica gel (20 g) in dichloro-methane-ethanol (15 1) yield 230 mg (90%) [a]D 69.7° (c 1, CHC13) Rf 0.32 (CH -ethanol 10 1). [Pg.275]

Some time s(especi ally when only a few compds are in a mixt), it is more convenient not to extrude the column, but instead to subject it to a more prolonged washing directly in the tube. This treatment, called elution, will usually separate the components more efficiently into wider bands and these may then be removed(together with solvents) and collected separately in clean receivers as the percolation thru the column continues. Solvents used in washing the column are called eluents or elution agents and they may be ales, eth, acet, dichloroethane, dichloro-methane, chlf, et acetate or petr ether(Refs 58 78)... [Pg.74]

The porous platinum/Teflon electrodes separate the electrolytic cell from the gaseous reference chamber on one side and the sample chamber on the working electrode side. The applied voltage is controlled by a potentiostat. The sample enters into the electrolytic cell through the porous electrodes, the pore size of which also needs to be closely controlled in order to prevent their flooding with the solvent. An example of an electrochemical reaction of interest is oxidation of methane under conditions of humid air. [Pg.232]


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See also in sourсe #XX -- [ Pg.73 ]




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