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Intermediate chemical exchange

Intermediate chemical exchange is the most difficult type of exchange to recognize because it often goes completely unnoticed. Intermediate exchange typically involves the extreme broadening of the resonance in question. In many cases, the broad peak may not be recognized for what it is, especially if automated baseline correction procedures are used to process the spectrum. [Pg.154]

If there is the potential for chemical exchange, we should examine the frequency spectmm before we apply baseline correction. Increasing the vertical scale (how big the biggest peaks in the spectrum are relative to the maximum peak height that can be accommodated in the computer display) by several orders of magnitude can often reveal the presence of a broad peak. [Pg.154]

Mathematical fitting of observed line shapes can he used to extract the activation energy, E, for dynamic exchange processes hy using an Arrhenius plot wherein the slope of the logK (K is the rate of exchange) versus inverse absolute temperature is proportional to activation barrier. [Pg.155]

If we wish to assign the resonances to the atomic sites of a molecule, the indication that exchange is complicating our spectra is normally not welcome. Carrying out NMR studies at higher frequencies or at lower temperatures are two ways in which exchange broadening can be reduced. [Pg.155]

Coalescence point. The moment in time or the temperature at which two resonances merge to become one resonance. Mathematically, coalescence occurs when the curvature of the middle of the observed spectral feature changes sign from positive to negative. [Pg.155]


Figure B2.4.1 shows the lineshape for intermediate chemical exchange between two equally populated sites without scalar coupling. For more complicated spin systems, the lineshapes are more complicated as well, since a spin may retain its coupling information even though its chemical shift changes in the exchange. Figure B2.4.1 shows the lineshape for intermediate chemical exchange between two equally populated sites without scalar coupling. For more complicated spin systems, the lineshapes are more complicated as well, since a spin may retain its coupling information even though its chemical shift changes in the exchange.
In the intermediate chemical exchange condition, the total relaxation frequency is given by the sum of the spin-spin relaxation, as above, together with the relaxation owing to chemical exchange, r, given by. [Pg.57]

Pharmaceutical. Ion-exchange resins are useful in both the production of pharmaceuticals (qv) and the oral adrninistration of medicine (32). Antibiotics (qv), such as streptomycin [57-92-17, neomycin [1404-04-2] (33), and cephalosporin C [61-24-5] (34), which are produced by fermentation, are recovered, concentrated, and purified by adsorption on ion-exchange resins, or polymeric adsorbents. Impurities are removed from other types of pharmaceutical products in a similar manner. Resins serve as catalysts in the manufacture of intermediate chemicals. [Pg.387]

In this chapter, we discuss NMR methods for rate measurements in all three regimes. First we discuss a new way of looking at the coalescing lineshapes in intermediate exchange. Then we cover standard and alternative NMR methods for studies of slow and fast chemical exchange. For many... [Pg.233]

In many of these descriptions of lineshapes, chemical exchange line-shapes are treated as a unique phenomenon, rather than simply another example of relaxation effects on lineshapes. This is especially true for line-shapes in the intermediate time scale, where severe broadening or overlapping of lines may occur. The complete picture of exchange lineshapes can be somewhat simplified, following Reeves and Shaw [13], who showed that for two sites, the lineshape at coalescence can always be described by two NMR lines. This fact can be exploited to produce a clarified picture of exchange effects on lineshapes and to formulate a new method for the calculation of exchange lineshapes [16, 23]. This method makes use of the fact that lineshapes, even near coalescence, retain Lorentzian characteristics [13] (fig. 3). These lines, or coherences, are each defined by an intensity, phase, position, and linewidth, and for each line in the spectrum, the contribution of that particular line to the overall free induction decay (FID) or spectrum can be calculated. [Pg.235]

Takeda, T., Kunitomi, K., Horie, T., Iwata, K., Feasibility study on the applicability of a diffusion-welded compact intermediate heat exchanger to next-generation high temperature gas-cooled reactor, Nucl. Eng. Des. 1997, 168,11-21. Bier W., Keller W., Linder G., Seidel, D., Schubert, K., Martin, H., Gas-to-gas heat transfer in micro heat exchangers, Chem. Eng. Process. 1993, 32, 33-43. Schubert, K., Brandner J., Fichtner M., Linder G., Schygulla, U., Wenka, A., Microstructure devices for applications in thermal and chemical process engineering, Microscale Therm. Eng. 2001, 5,17-39. www.fzk.de, Forschungszentrum Karlsruhe, 17 July 2004. [Pg.407]

In general, there are two alternatives for coupling the S-I process to a VHTR. In the first, secondary helium is initially used to supply heat to the MT/HT1 sulphuric acid decomposition steps. LT helium heat is then consumed by the HI decomposition section before the helium return to the intermediate heat exchanger. In the second alternative, heat integration between the chemical process steps allows for helium heat supply solely to the MT/HT sulphuric acid decomposition steps. Residual process LT heat recovered there is utilised in the HI decomposition section. [Pg.182]

In a coupled nuclear hydrogen generation system, the reactor loop will be coupled to the chemical loop via an intermediate heat exchanger (IHX). This coupling is illustrated in Figure 1. [Pg.378]

The existence of the Black Sea bottom convective layer (BCL) has important implications for the physical and chemical exchange at the sediment/water interface and at the interface between intermediate and bottom water masses. Two-fold increased vertical gradients of dissolved sulphide at the upper boundary of the BCL suggest the presence of the anoxic interface separating entire anoxic water mass dominated by turbulent diffusion from underlying waters of the BCL where double diffusion is the main mixing mechanism. [Pg.445]

Line shape analysis may be complemented or verifled by measuring chemical exchange by NMR by relaxation dispersion experiments. Relaxation dispersion is based on measuring a series of CPMG-based relaxation rates at different temperatures. Excited state intermediates in folding reactions or ligand-accessible intermediates can thereby be probed, even when they constitute as little as 1% of the entire population (34, 98). [Pg.1281]


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