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Saturation behavior

As described above, mechanism-based inactivation conforms to a two-step reaction and should therefore display saturation behavior. The value of should be a rectangular hyperbolic function of [/]. This was described in detail above in Section 8.1. [Pg.229]

The saturation behavior of a spectrum - the variation of integrated intensity with microwave power - is related to the spin-lattice relaxation time, a measure of the rate of energy transfer between the electron spin and its surroundings. Saturation often depends on the same structural and dynamic properties as line widths. [Pg.18]

The phenomenological equations proposed by Felix Bloch in 19462 have had a profound effect on the development of magnetic resonance, both ESR and NMR, on the ways in which the experiments are described (particularly in NMR), and on the analysis of line widths and saturation behavior. Here we will describe the phenomenological model, derive the Bloch equations and solve them for steady-state conditions. We will also show how the Bloch equations can be extended to treat inter- and intramolecular exchange phenomena and give examples of applications. [Pg.92]

As a simple model for the enzyme penicillinase, Tutt and Schwartz (1970, 1971) investigated the effect of cycloheptaamylose on the hydrolysis of a series of penicillins. As illustrated in Scheme III, the alkaline hydrolysis of penicillins is first-order in both substrate and hydroxide ion and proceeds with cleavage of the /3-lactam ring to produce penicilloic acid. In the presence of an excess of cycloheptaamylose, the rate of disappearance of penicillin follows saturation kinetics as the cycloheptaamylose concentration is varied. By analogy to the hydrolysis of the phenyl acetates, this saturation behavior may be explained by inclusion of the penicillin side chain (the R group) within the cycloheptaamylose cavity prior to nucleophilic attack by a cycloheptaamylose alkoxide ion at the /3-lactam carbonyl. The presence of a covalent intermediate on the reaction pathway, although not isolated, was implicated by the observation that the rate of disappearance of penicillin is always greater than the rate of appearance of free penicilloic acid. [Pg.231]

There may, however, be specific reasons to study a signal over an extended temperature range. For one, a linear increase in EPR amplitude with the inverse of the temperature (Curie s law) is proof that a spin system is a two-level system, i.e., an S = 1/2 or an effective S = 1/2 system. More importantly, in complex multicenter metalloproteins, overlapping spectra may be deconvoluted by virtue of their Tu value being different if two centers, a and b, have rMa < TMb then at TMb the spectrum of center a is broadened and that of center b is not. It is once more emphasized that these types of studies require determination of (anisotropic) saturation behavior at all relevant temperatures. [Pg.57]

For a binding reaction we can pick whether we show the reaction as favorable or unfavorable by picking the substrate concentration we use. Association constants have concentration units (M-1)- The equilibrium position of the reaction (how much ES is present) depends on what concentration we pick for the substrate. At a concentration of the substrate that is much less than the dissociation constant for the interaction, most of the enzyme will not have substrate bound, the ratio[ES]/[E] will be small, and the apparent equilibrium constant will also be small. This all means that at a substrate concentration much less than the dissociation constant, the binding of substrate is unfavorable. At substrate concentrations higher than the dissociation constant, most of the enzyme will have substrate bound and the reaction will be shown as favorable (downhill). (See also the discussion of saturation behavior in Chap. 8.)... [Pg.103]

SUBSTRATE CONCENTRATION affects the velocity of an enzyme-catalyzed reaction. Almost all enzyme-catalyzed reactions show saturation behavior. At a high enough substrate concentration, the reaction just won t go any faster than Tmax. The substrate concentration required to produce a velocity that is one-half of is called the Km. [Pg.118]

In the meantime temperature-dependent stopped-flow measurements were conducted on the latter complex in order to determine the activation parameters of the N-N cleavage reaction (24). Plots of the absorption intensity at 418 nm vs. time at T — —35 to +15°C indicate biphasic kinetics with two rate constants 0bs(p and obs(2)> in analogy to our measurements of the tungsten complex. This time, however, both rates depended upon the acid concentration. Interestingly much smaller rate constants 0bs(i) and 0bs(2)> were found for all acid concentrations than given by Henderson et al. for his (single) rate constant kobs (up to 1 order of magnitude). Furthermore plots of 0bs(i) and kohs(2) vs. the acid concentration showed no saturation behavior but linear dependencies with slopes k and k and intercepts k und k, respectively (s — acid dependent and i — acid independent), Eq. (2) ... [Pg.376]

Fig. 22 A plot of kohs for methanolysis of 4 x 10 5M methyl /j-nitrophcnyl phosphate (MNPP) vs. [35 2Zn(II)] in the presence of 1 equivalent of CH-jO per ligand showing a saturation behavior, pH = 9.5, T = 25+0.1 °C. Line through the data calculated by NLLSQ fits to a Michaelis-Mentin equation corrected for complex dissociation95 giving a binding constant of A M = 0.37 mmol dm-3 and a maximum rate constant for reaction of the MNPP [(CH3CT) 35 2Zn(II)] complex of kmAK — (4.1 0.1) x 10 2s Reproduced with permission from ref. 95. Fig. 22 A plot of kohs for methanolysis of 4 x 10 5M methyl /j-nitrophcnyl phosphate (MNPP) vs. [35 2Zn(II)] in the presence of 1 equivalent of CH-jO per ligand showing a saturation behavior, pH = 9.5, T = 25+0.1 °C. Line through the data calculated by NLLSQ fits to a Michaelis-Mentin equation corrected for complex dissociation95 giving a binding constant of A M = 0.37 mmol dm-3 and a maximum rate constant for reaction of the MNPP [(CH3CT) 35 2Zn(II)] complex of kmAK — (4.1 0.1) x 10 2s Reproduced with permission from ref. 95.
An external electric field induces a change in the dipole moment known as polarization. However, the induced dipole moment has a saturation behavior which makes the polarization deviate for the linear response to the external L-field. and the total polarization p of the chromophore in an external electric field can be written as... [Pg.25]

Figure 3. ARUPS energy distribution curves taken with Hel radiation at normal incidence and an electron emission angle of 52" shown as a function of copper coverage. The intensity of the various curves has been normalized at the Fermi level Ef The individual curves are matched to their corresponding copper coverages in monolayers by the solid lines and the saturation behavior of the interface state at approximately —1.5 eV is identified by the dashed lines. (Data from ref. 8.) (Reprinted with permission from ref. 43. Copyright 1987 American Association for the Advancement of Science.)... Figure 3. ARUPS energy distribution curves taken with Hel radiation at normal incidence and an electron emission angle of 52" shown as a function of copper coverage. The intensity of the various curves has been normalized at the Fermi level Ef The individual curves are matched to their corresponding copper coverages in monolayers by the solid lines and the saturation behavior of the interface state at approximately —1.5 eV is identified by the dashed lines. (Data from ref. 8.) (Reprinted with permission from ref. 43. Copyright 1987 American Association for the Advancement of Science.)...
In Fig. 20 is given the proton saturation behavior of a SA sample with an... [Pg.72]

Fig. 20. Saturation behavior of NMR absorption (x") and dispersion derivative at resonance (axV Ho) for proton resonance of silica-alumina (sample of area 425 meter / gram) dehydrated at 500°. The audio modulation frequency was 40 c.p.s. Arrows on abscissa indicate values of Hi for which saturation of x" and dx / Ho occurs (17S). Fig. 20. Saturation behavior of NMR absorption (x") and dispersion derivative at resonance (axV Ho) for proton resonance of silica-alumina (sample of area 425 meter / gram) dehydrated at 500°. The audio modulation frequency was 40 c.p.s. Arrows on abscissa indicate values of Hi for which saturation of x" and dx / Ho occurs (17S).
As shown in Fig. 7.20, the burning rate of the AP composite propellant is increased approximately twofold by the addihon of 1 % BEFP. In general, the degree of the burning rate increase is proportional to the amount of catalyst added when the catalyst conshtutes less than about 3 % of the total mass, and the effect of the catalyst addihon shows saturation behavior at about 5% by mass. Fig. 7.23 shows the burning rates of AP-HTPB composite propellants composed of ap(0-80) and... [Pg.195]

An alkylating agent (ICH2COO ) that acts as a potent irreversible inhibitor of enzymes containing reactive thiol, e-amino, and/or imidazole side-chain groups within their active sites. The carboxymethylation reaction with enzymes is typically a bimolecular process that takes place without rate-saturation behavior ... [Pg.374]

Scatchard plots for ligand saturation behavior of an oligomeric protein exhibiting positive cooperativity, negative cooperativity, or independent binding behavior. For addition details, See Monod-Wyman-Changeux Cooperativity Model Scatchard Plot... [Pg.411]

Net carrier transport can be examined whenever a transportable substrate is present on both sides of a membrane. Again for the case of a single class of carriers, the inward transport rate and outward transport rates show rate-saturation behavior ... [Pg.448]

Figure 2. Top Effect of the magnitude of the allosteric constant on ligand saturation behavior of a dimer obeying the MWC model. Bottom Fraction of total dimeric protein present in various T- and R-species. Figure 2. Top Effect of the magnitude of the allosteric constant on ligand saturation behavior of a dimer obeying the MWC model. Bottom Fraction of total dimeric protein present in various T- and R-species.
PULSE-CHASE EXPERIMENTS RATE OF REACTION CHEMICAL KINETICS Rate processes in aqueous solutions, CHEMICAL KINETICS RATE SATURATION BEHAVIOR RAY-ROSCELLI TREATMENT ISOMERIZATION ISO MECHANISMS RE-... [Pg.777]

From the last column of the table, we see that the ratio of the parallel-spin to the total correlation energy is remarkably independent of the size of the basis set. Contrary to expectation, the parallel-spin correlation contribution appears to be about as difficult to account for within a finite basis-set approach as the antiparallel-spin correlation. Our investigation does not provide a careful study of the basis-set saturation behavior in MP2 calculations, such as is given in Refs. [74,72,75,33]. However, our results show that, with small- and moderate-sized basis sets which are sufficiently flexible for most purposes and computationally tractable in calculations on larger systems, there is no evidence that the parallel-spin correlation contribution converges more rapidly than the antiparallel-spin contribution. A plausible explanation for this effect is that, for small interelectronic separations, the wavefunction becomes a function of the separation, which is difficult to represent in a finite basis-set approach for either spin channel. The cusp condition of Eq. (19) is a noticeable manifestation of this dependence, but does not imply that the antiparallel-spin channel is more difficult to describe with a moderate-sized basis set than the parallel channel. In fact, in the parallel correlation hole, there is a higher-order cusp condition, relating the second and third derivatives with respect to u [76]. [Pg.26]


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See also in sourсe #XX -- [ Pg.26 ]

See also in sourсe #XX -- [ Pg.217 ]




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