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Separation absorption

The reaction occurs in two steps ammonium carbamate is formed first, followed by a decomposition step of the carbamate to urea and water. The first reaction is exothermic, and the equilibrium is favored at lower temperatures and higher pressures. Higher operating pressures are also desirable for the separation absorption step that results in a higher carbamate solution concentration. A higher ammonia ratio than stoichiometric is used to compensate for the ammonia that dissolves in the melt. The reactor temperature ranges between 170-220°C at a pressure of about 200 atmospheres. [Pg.146]

The ability of the stable carbene 218 to deprotonate acidic hydrocarbons was examined by NMR in (CD3)2S0.153 Indene (pJta = 20.1) was completely converted to its anion whereas 9-phenylxanthene (pAfa = 27.7) was not measurably deprotonated. The NMR spectra of 1 1 mixtures of 218 with fluorene (pXa = 22.9) and 2,3-benzofluorene (pA"a = 23.5) showed separate absorptions for the hydrocarbons and their anions. From the integration of these spectra, P a = 24.0 for 218 was derived. In THF, 218 failed to deprotonate fluorene but almost completely deprotonated indene. The proton transfer from hydrocarbons to 218 creates ions (ion pairs) from neutral species, which will be less favorable in solvents of lower polarity. [Pg.42]

Triisopropylthiobenzophenone 20a and its p-methoxy derivative 20b were chosen for study (Scheme 11). Like thiobenzophenone, thiones 20 show well-separated absorption maxima in the visible (600 nm, nTi" ) and UV (320 nm, Tm" ) regions of the spectrum. In contrast, photolysis of freeze-pump-thaw-deoxygenated solutions of thiones 20a and 20b in benzene through Pyrex (>290 nm) afforded excellent chemical yields (ca. 70%) of the benzocyclo-butenethiol derivatives 21a and 21b. The same photoreaction could be brought about in the crystalline state at a much-reduced rate. [Pg.18]

Deuteration of one end of the allyl moiety in these compounds removes the equivalence of the two positions and in place of the single line for the terminal position, two separate absorptions should appear (W). One, in the normal decoupled spectrum, is a singlet for the hydrogen substituted carbon, and the other a weak quintet for the deuterated end which would be difficult to observe. These two signals would bracket the normal singlet. If a mixture of deuterated and undeuterated allyl compound is used, therefore, two easily observable peaks should appear, one in the normal position, the other shifted. In the spectra of allyllithium and allylsodium the line from the deuterated compound appeared I and 11 Hz upfield respectively, at 0°C, of the normal lines. The potassium compound only showed a somewhat broadened line. At -80°C the separation for allyllithium was 22 Hz. [Pg.90]

HP IR measurements have recently been reported by workers at Sasol for cobalt-catalysed 1-dodecene hydroformylation reactions using bicyclic phosphines (4) derived from (R)-(+)-limonene [68]. Using Fourier deconvolution to separate absorptions due to [HCo(CO)4] and [Co2(CO)7(phosphine)], it was possible to estimate the ratio of modified [HCo(CO)3(phosphine)] to un-modified [HCo(CO)4] in the catalytic mixture, using peak areas. Values of this ratio ranged from ca. 2-20, depend-... [Pg.124]

Photochromism is a chemical process in which a compound undergoes a reversible change between two states having separate absorption spectra, i.e. different colours. The change in one direction occurs under the influence of electromagnetic radiation. [Pg.7]

Figure 3.3 shows some of these possible transitions for HCI. Those with A7 = +1 are known as the R branch and occur at the high-energy side of the hypothetical transition At = 1, A7 = 0 (this is not allowed because of the selection rule, A7 = +1). Those with A7 = — 1 on the low-frequency side of the hypothetical transition form the P branch. Figure 3.4 shows the absorption spectrum of HCI at room temperature, with the rotational transitions responsible for each line. The relative intensities of the lines reflect the relative populations of the absorbing rotational levels the peaks are doublets due to the separate absorptions of the two chlorine isotopes, that is, H35C1 and H37C1, which have different reduced masses and hence values of the rotational constant B. [Pg.46]

Up to now we have been able to observe 13 separate absorption bands in the ultraviolet region of the spectrum between 220 and 400 m/. The shift in the Amax of polyenyl free radicals to longer wavelengths with increasing n would be expected to be linear with n, similar to the... [Pg.47]

At two different concentrations isomerisation experiments have been carried out with lactose as well as with lactulose. The results are shown in table 3, together with the initial catalyst condition data as calculated from separate absorption and ionisation measurements (refs.8,9). It appears that a higher selectivity can be obtained at higher initial concentrations. [Pg.219]

The principle involved in combustion is the complete oxidation of C and H in the compound to C02 and H20 by means of air or 0. By the separate absorption of these two substances the percentages of C and H can be calculated. For many years the macro method in general use has been that originally due to Liebig, in which 0-15—0-25 gm. of substance is required for the analysis. [Pg.446]

A hysteresis loop can formally be drawn for the interconversion of a photo-chromic substance between two states A and B characterized by two well separated absorption bands as shown in Figure 26 sweeping the frequency up from vc to Va converts the system from state A to B when vc reaches the absorption band of A the system remains in state B if Va goes back to v0 sweeping vc to Vb converts the system from state B to A, where it remains when V goes back to VQ. Such state interconversion curves are also characterized by the non-linearity of the response with respect to scanning the triggering stimulus. [Pg.125]

We shall see further (in Sections VI, VII, and IX) that there exists also another important cause stipulating appearance of the second separate absorption band in the FIR spectral region. In terms of our approach, such a band originates due to vibration of the hydrogen-bonded molecules. [Pg.120]

For this low-temperature and -pressure range, any gas density may quickly be calculated. Error here is less than 3% in every case checked. What about higher temperatures and pressures Aren t these higher values where all concerns rest Yes, most all process unit operations, such as fractionation, separation, absorption stripping, chemical reaction, and heat exchange generate and apply these higher-temperature... [Pg.9]

If the absorption is multicomponent, the average equilibrium constant mave is determined for each of the solute components at the average temperature and pressure of the absorber, and a separate absorption factor Aave is defined for each component. These absorption factors can be used in Eq. (28) to define the absorbed fraction of the component. [Pg.16]

E> can be measured directly by membrane or vapor pressure osmometry. The application of an alternative method was described recently [64, 65]. It is based on an analysis of the sedimentation equilibrium in an analytical ul-tracentrifuge, where the solution contains the polyelectrolyte as well as a small concentration of an inert salt. In sedimentation equilibrium, the concentration gradients of both components are coupled via a Donnan-type equilibrium, which is governed by the effective charge number zeff of the polyion. Both concentration gradients can be determined in one experiment, when the polyion and the coion of the salt have sufficiently separated absorption bands in the UV or visible range. [Pg.44]

The first method [87,88] uses a matrix form of the Beer-Lambert absorption law in a transmission mode. A 2-D material sample is raster-scanned by a pulsed, tunable THz source to generate an N rows x L columns image matrix [/] where N is the number of THz frequencies used and L is the number of pixels. The values of [/] are the measured total absorbance at each pixel. Separate absorption experiments with known materials of interest establish the THz spectra both graphically and through the N x M spectra matrix [S], where M is the number of components. The collection of species can include non-agent materials that can affect the absorptions for example, barrier materials with spectra that are typically weakly frequency dependent. The spatial patterns of the agents are contained in the M x L matrix [P], The values of [P] effectively contain agent concentration information. [Pg.357]

Sometimes separate absorptions can be found for crystalline and amorphous regions in such a case the dichroism of this band gives information about orientation in both regions. [Pg.479]

The similar distinct absorption peak shown for yff-D-fructopyranose is associated with a weakly bonding 0(4)H group forming a two-center H 0 bond of 2.07 A (Fig. 13.25). A similar separate absorption peak should also be observed for the very weakly bonded 0(4)H group in the / -D-glucopyranose (Fig. 13.27) and /1-lactose (Fig. 13.43) crystal structures, but hitherto these have not been reported. [Pg.204]

Figure 10. Top liquid-phase absorbance spectrum of each component of a typical photorefractive polymer composite. Each component, A -vinylcarbazole (PVK), 2,4,7-trinitro-9-fluorenone (TNF), and typical chromophore (EHDNPB), is diluted in dichloromethane separately. (Absorption due to the solvent has been subtracted.) Bottom the absorbance of light in a solid sample due to the charge transfer complexation between PVK and TNF. The sample was prepared from a 9 1 ratio of PVK/ TNF. The extension of absorption to longer wavelengths is clear. Figure 10. Top liquid-phase absorbance spectrum of each component of a typical photorefractive polymer composite. Each component, A -vinylcarbazole (PVK), 2,4,7-trinitro-9-fluorenone (TNF), and typical chromophore (EHDNPB), is diluted in dichloromethane separately. (Absorption due to the solvent has been subtracted.) Bottom the absorbance of light in a solid sample due to the charge transfer complexation between PVK and TNF. The sample was prepared from a 9 1 ratio of PVK/ TNF. The extension of absorption to longer wavelengths is clear.
A related proposal based on presumed change of the potential function is the double minimum explanation. The presence of the base introduces the possibility that a second minimum energy position exists with the proton nearer B than A. Such a double minimum would have a complicated set of energy levels for in extreme cases giving two rather widely separated absorptions for Vg, Detoni and Hadii have so assigned absorptions in the spectra of aromatic selenates and of selenic acid (520). Barrow and Yerger made a systematic search for such cases and concluded that acetic acid-alkyl amines may have such potential functions (143, 2221). It is quite reasonable that some acid-base pairs may have double minimum potential functions. Yet, it does not seem... [Pg.246]


See other pages where Separation absorption is mentioned: [Pg.369]    [Pg.800]    [Pg.566]    [Pg.588]    [Pg.46]    [Pg.13]    [Pg.334]    [Pg.202]    [Pg.14]    [Pg.230]    [Pg.176]    [Pg.213]    [Pg.369]    [Pg.199]    [Pg.112]    [Pg.521]    [Pg.127]    [Pg.224]    [Pg.89]    [Pg.134]    [Pg.43]    [Pg.17]    [Pg.23]    [Pg.228]    [Pg.233]    [Pg.152]    [Pg.50]    [Pg.13]    [Pg.400]    [Pg.306]   
See also in sourсe #XX -- [ Pg.291 ]




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