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X at low concentrations

Each end product, I and X, inhibits Ei. At saturating levels of either one, the velocity can be driven to zero. Mixtures of I and X at low concentrations are more inhibitory than the same total specific concentration of I or X alone. That is, if 35% inhibition is observed at [I] = 6 Kj and [X] = 0 and if 35% inhibition is observed at [X] = 6 Kx and [I) = 0, then at [I] = 3 Ki plus [X] = 3 Kx, the inhibition will be greater than 35%. Cooperative inhibition implies that I and X are not mutually exclusive. Both end products can combine with Ei simultaneously to form dead-end EIX and/or EIXS complexes. [Pg.267]

For a binary mixture, the composition is completely specified by x , which is the mole fraction of component A in the liquid in equilibrium. In this case, the partial pressure of component A will be a function of pressure, temperature, and x . If the properties of the liquid are pressure-independent, and if the gases behave as ideal gases, then the partial pressure of component A at constant temperature can be written as a function of only x . If the liquid phase consists of only one component, the partial pressure of A equals the vapor pressure of pure A. The partial pressure of component A, Pa, is described as a function of x by Henry s law. It states that Pa is directly proportional to x at low concentrations of component A ... [Pg.176]

As an example we show in Fig, 1 the solubility data of D in 0.80 90.20 obtained during heating the Pdg 80 90.20 x sample between 60 and 500 °C in 20 K steps. The experimental values of x and p are plotted according to Eq, 1 taking N = 1. The circles represent the experimental values. These data can be fitted very well by straight lines (solid lines in Fig. 1) u/hich means that Ap is a linear function of x at low concentrations. From the intersections of the straight lines with the y axis we obtain the equilibrium constants at infinite dilution which... [Pg.388]

Fig. 10 Effect of dispersion on X at low concentrations in liquid phase 33j. Reprinted with permission Chem. Engng. Sci., 31, Copyright (1976) Pergamon Press. Fig. 10 Effect of dispersion on X at low concentrations in liquid phase 33j. Reprinted with permission Chem. Engng. Sci., 31, Copyright (1976) Pergamon Press.
One important characteristic of polymers is their shear thinning behavior the viscosity decreases with increasing rate of deformation (Figure 13.23). This behavior at 7 is attributed to the partial disentanglement of the chains as they get extended in the flow direction. Since the relaxation time increases with molecular weight [for example, X at low concentrations Eqs. (12), (15)] and with polymer concentration, shear thinning begins at lower shear rates for polymers with... [Pg.702]

Minerals generally present difficult problems in chemical analysis, and these problems grow more serious when the elements being determined are as difficult to separate as are those named above. The time and effort that x-ray emission spectrography can save are therefore great, but there are obstacles to be surmounted. Among these are (1) Absorption and enhancement effects are often serious. (2) The element of interest may be present at low concentration in a matrix that is unknown and variable. (3) Satisfactory standards are not always easy to obtain. (4) Simple equipment sometimes does not resolve important analytical lines- completely. (5) Sample preparation and particle size often influence the intensities of analytical lines Class II deviations (7.8) can be particularly serious with minerals. [Pg.199]

The simplicity mentioned above exists for various kinds of samples that meet the fundamental requirements laid down in Chapters 6 and 7. Examples are a thin film on a suitable substrate, a sample dissolved at low concentration in a solvent transparent to x-rays, or a sample uniformly dispersed in a similarly transparent medium. In all cases, scattered x-rays should be at a minimum to keep the background low. From the point of view taken here, a trace is thus regarded as a major constituent in a sample if sensible absorption and enhancement effects are absent—if, that is, Equation 7-3 is valid. [Pg.226]

Figure 4.29. Back-calculated results for files VALIDX.dat. The data are presented sequentially from left to right. The ordinate is in % of the nominal concentration. Numbers X = 1,2, and 3 indicate the data file. Each bracket indicates a day s worth of results (sorted by concentration). The log/log format tends to produce positive deviations at low concentrations, while the lin/lin format does the opposite, to the point of suggesting negative concentrations The reason is that the low concentration values are tightly clustered at the left end of the lin/lin depiction whereas the values are evenly spread in the log/log depiction, with commensurate effects on the position of Xmean, the sum Sxx< and the influence each coordinate has on the slope. The calibration design was optimized for the log/log format. Figure 4.29. Back-calculated results for files VALIDX.dat. The data are presented sequentially from left to right. The ordinate is in % of the nominal concentration. Numbers X = 1,2, and 3 indicate the data file. Each bracket indicates a day s worth of results (sorted by concentration). The log/log format tends to produce positive deviations at low concentrations, while the lin/lin format does the opposite, to the point of suggesting negative concentrations The reason is that the low concentration values are tightly clustered at the left end of the lin/lin depiction whereas the values are evenly spread in the log/log depiction, with commensurate effects on the position of Xmean, the sum Sxx< and the influence each coordinate has on the slope. The calibration design was optimized for the log/log format.
Espenson has shown that the reaction of c/j-Co(en)2(N3)2 with takes place by an inner-sphere mechanism. This Co(III) complex was selected for investigation because it is particularly reactive towards and also the dissociation of monoazido vanadium(lll) is relatively slow. At low concentrations (2-20 X 10 M) the second-order rate coefficient is 32.9 l.mole . sec at 25 °C, [H ] = 0.10 M and [i = 1.0 M. At higher concentrations ( 0.1 M), using a stopped-flow apparatus, the kinetics are apparently first order at 520 mfi, a wavelength where shows negligible absorbance. The rate coefficient under... [Pg.203]

It will be observed that the chemical potentials depend appreciably on the chain length, represented by x only at low concentrations. The influence of the chain length vanishes with increase in concentration of... [Pg.513]

A plug-flow, liquid-liquid, extraction column is represented in Fig. 4.19. For convenience, it is assumed that the column operates under low concentration conditions, such that the aqueous and organic flow rates, L and G, respectively are constant. At low concentration, mole fraction x and y are identical to mole ratios X and Y, which are retained here in the notation for convenience. This however leads to a more complex formulation than when concentration quantities are used, as in the example AXDISP. [Pg.202]

The surface active agents (surfactants) may be cationic, anionic or non-ionic. Surfactants commonly used are cetyltrimethyl ammonium bromide (CTABr), sodium lauryl sulphate (NaLS) and triton-X, etc. The surfactants help to lower the surface tension at the monomer-water interface and also facilitate emulsification of the monomer in water. Because of their low solubility surfactants get fully dissolved or molecularly dispersed only at low concentrations and at higher concentrations micelles are formed. The highest concentration where in all the molecules are in dispersed state is known as critical micelle concentration (CMC). The CMC values of some surfactants are listed in table below. [Pg.16]

Li generally occupies octahedral sites in these compounds at low concentrations. But there is only one octahedral site per transition metal in a compound like VScj, and so beyond x = 1 at least some of the Li must occupy tetrahedral sites. Since the tetrahedral sites are above and below the planes of the octahedral sites, the Li-Li repulsion is reduced if the Li already in octahedral sites shift to tetrahedral sites beyond x = 1. Thus the structure goes from AbC(b)AbC at x = 1 to AbC(a,c)AbC at X = 2. That is one way to rationalise why all the Li occupy tetrahedral... [Pg.171]

If a straight hne is obtained when is plotted against x/m at low concentrations, the Langmuir equation is applicable. However, due to the restrictive assumptions, Langmuir isotherms usually are of miuor importance in heterogeneous media... [Pg.98]


See other pages where X at low concentrations is mentioned: [Pg.79]    [Pg.295]    [Pg.79]    [Pg.295]    [Pg.83]    [Pg.349]    [Pg.437]    [Pg.335]    [Pg.98]    [Pg.362]    [Pg.9]    [Pg.842]    [Pg.254]    [Pg.187]    [Pg.192]    [Pg.1167]    [Pg.443]    [Pg.335]    [Pg.458]    [Pg.374]    [Pg.52]    [Pg.366]    [Pg.56]    [Pg.216]    [Pg.247]    [Pg.364]    [Pg.51]    [Pg.277]    [Pg.159]    [Pg.171]    [Pg.185]    [Pg.339]    [Pg.68]    [Pg.132]    [Pg.262]    [Pg.315]    [Pg.180]    [Pg.205]    [Pg.76]   
See also in sourсe #XX -- [ Pg.442 ]




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Low Concentration

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