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Coupling constant first-order

It is fortunate that most applications devolve into one of two camps small molecules or proteins. In the former case, the size of these molecules has stayed fairly constant and the inexorable rise in magnetic fields has meant that the number of incidences of second-order spectra has decreased (although complications will always exist with virtual couplings). It is therefore pertinent to examine methods, which are not only designed to extract couplings from first-order spectra, but are also amenable to automation. [Pg.223]

Figure 5.7. First-order constant-volume batch plots for two coupled parallel first-order steps. Top left very fast isomerization top right very slow isomerization bottom left comparable rates with kn > k21 > kIp > k2Q and initial charge of A, (schematic). Figure 5.7. First-order constant-volume batch plots for two coupled parallel first-order steps. Top left very fast isomerization top right very slow isomerization bottom left comparable rates with kn > k21 > kIp > k2Q and initial charge of A, (schematic).
Most spectrometers today contain software that can calculate spectra for up to seven spins. The first step is a trial-and-error procedure of approximating the chemical shifts and coupling constants in order to match the observed spectrum through computer simulation. Chemical shifts are varied until the widths and locations of the observed and calculated mul-tiplets approximately agree. Then the coupling constants or their sums and differences are varied systematically until a reasonable match is obtained. This method is relatively successful for three and four spins, but is difficult to employ with larger systems. [Pg.116]

Lumped Kinetic or Pseudokinetic Modeis. Lumped kinetic models have some predictive ability outside their original existing data set. Some rate constants are derived and used in a set of coupled, linear, first-order rate equations. Forward and reverse reactions can be included. The set kinetic equations may be used to evaluate variations of feedstock, hydrogen partial pressure, etc. These models require the use of computers to formulate and to use. They do provide additional levels of detail in return. Most current published models have some degree of lumping (36,37). [Pg.1987]

The problems discussed in this section have been restricted to reversible electron transfer processes coupled with first-order chemical reactions (for the most part). The current responses are usually expressed as functions of the dimensionless kinetic parameters (cf. Table 2) involving the life-time of mercury drop, For the estimation of the chemical rate constants of reversible reactions the equilibrium constants K should be known. As in other voltammetric methods (see below), the experimental data are transformed into normalized quantities. Kinetic... [Pg.172]

The systematic derivation of implicit correlation functionals is discussed in Sect. 2.4. In particular, perturbation theory based on the Kohn-Sham (KS) Hamiltonian [16,17,18] is used to derive an exact relation for l xc- This expression is then expanded to second order in the electron-electron coupling constant in order to obtain the simplest first-principles correlation functional [18]. The corresponding OPM integral equation as well as extensions like the random phase approximation (RPA) [19,20] and the interaction strength interpolation (ISI) [21] are also introduced. [Pg.57]

The C-H spin couplings (Jen) have been dealt with in numerous studies, either by determinations on samples with natural abundance (122, 168, 224, 231, 257, 262, 263) or on samples specifically enriched in the 2-, 4-, or 5-positions (113) (Table 1-39). This last work confirmed some earlier measurements and permitted the determination for the first time of JcH 3nd coupling constants. The coupling, between a proton and the carbon atom to which it is bonded, can be calculated (264) with summation rule of Malinovsky (265,266), which does not distinguish between the 4- and 5-positions, and by use of CNDO/2 molecular wave functions the numerical values thus - obtained are much too low, but their order agrees with experiment. The same is true for Jch nd couplings. [Pg.79]

First-order spectra (mulliplels) are observed when the eoupling constant is small compared with the frequency difference of chemical shifts between the coupling nuclei This is referred to as an A n spin system, where nucleus A has the smaller and nucleus X has the considerably larger chemical shift. An AX system (Fig. 1.4) consists of an T doublet and an X doublet with the common coupling constant J x The chemical shifts are measured from the centres of eaeh doublet to the reference resonance. [Pg.3]

Rather large HH coupling constants in the aliphatics range (72.5 and 15.0 Hz) indicate geminal methyl protons in rings. In order to establish clearly the relevant AB systems, it makes sense first to interpret the CH COSY diagram (Table 52.1). From this, the compound contains two methylene groups, A and B. [Pg.240]

The spin Hamiltonian operates only on spin wavefunctions, and all details of the electronic wavefunction are absorbed into the coupling constant a. If we treat the Fermi contact term as a perturbation on the wavefunction theR use of standard perturbation theory gives a first-order energy... [Pg.308]

The first step was found to be a fast pre-equilibrium (Scheme 12-8). The dependence of the measured azo coupling rate constants on the acidity function and the effect of electron-withdrawing substituents in the benzenediazo methyl ether resulting in reduced rate constants are consistent with a mechanism in which the slow step is a first-order dissociation of the protonated diazo ether to give the diazonium ion (Scheme 12-9). The azo coupling proper (Scheme 12-10) is faster than the dissociation, since the overall rate constant is found to be independent of the naphthol con-... [Pg.313]

Due to this aggregation effect, the measured rate constants for the second coupling reaction are not truly first-order with respect to the diazo component. Gloor and... [Pg.362]

Remes et al. (1976) also investigated the kinetics of the N-azo coupling of nine a-amino acids. They are aware of earlier investigations in which the major products were pentaz-1,4-dienes, but they claim that under their reaction conditions (pH 8.00-10.25, thirty-fold excess of amino acid) only the triazenes are formed. The rates were found to be first-order with respect to diazonium ion which is consistent with their conclusion however, in the opinion of the present author the results suggest a significant (say, 10%) contribution of pentazdiene formation to the total rate process. No significant correlation was found between the rate constants and the acidity constants of the nine amino acids. [Pg.392]

First order multiplet First order multiplets are those in which the difference in chemical shifts of the coupled protons, in hertz (Hz), divided by the coupling constant between them is about 8 or more (Av/y>8). These multiplets have a symmetrical disposition of the lines about their midpoints. The distance between the two outermost peaks of a first order multiplet is the sum of each of the coupling constants. [Pg.415]

The complete reaction scheme is shown in Fig. 5.3-7, while Fig. 5.4-51 gives a simplified representation. 1-naphthol (A) is primarily coupled with diazotized sulphanilic acid (B) to form monoazo dyes coupled in para and ortho positions (p-R and o-R, respectively). This reaction is first order in both A and B. Each of the primary products can react with diazotized sulphanilic acid to form bisazo dye (5). Rate constants at 298 K and pH 10 are ku = 10600 m mof s k2i = 1 22 = 1.7 m mor s (see Fig. 5-4-51). [Pg.341]


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See also in sourсe #XX -- [ Pg.145 ]

See also in sourсe #XX -- [ Pg.145 ]

See also in sourсe #XX -- [ Pg.145 ]




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