1991
DOI: 10.1021/ja00021a002
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An experimentally based family of potential energy surfaces for hydride transfer between NAD+ analogs

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Cited by 100 publications
(136 citation statements)
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“…For computational simplicity, therefore, we base our calculations on the hypothetical symmetric transfer of H − from reduced to oxidized nicotinamide moieties, in a manner similar to a model for symmetric H-transfer in solution. 53 The donor and acceptor moieties are analogous to the ubiquitous nicotinamide biological cofactor NAD(P) + . A hydrogen truncates the nicotinamide rings where they normally link to the ribosyl moiety of NAD(P) + , so the system contains a total of 33 atoms (Figure 3) and an overall charge of +1.…”
Section: Methodsmentioning
confidence: 99%
“…For computational simplicity, therefore, we base our calculations on the hypothetical symmetric transfer of H − from reduced to oxidized nicotinamide moieties, in a manner similar to a model for symmetric H-transfer in solution. 53 The donor and acceptor moieties are analogous to the ubiquitous nicotinamide biological cofactor NAD(P) + . A hydrogen truncates the nicotinamide rings where they normally link to the ribosyl moiety of NAD(P) + , so the system contains a total of 33 atoms (Figure 3) and an overall charge of +1.…”
Section: Methodsmentioning
confidence: 99%
“…93 In many respects, this theory is similar to TST with a transmission coefficient based on large-curvature tunneling. 147,236,[260][261][262][346][347][348][349][350][351][352][353] In both cases, the TST rate constant is multiplied by a factor that reflects the "interplay between donor-acceptor configuration and nuclear tunneling". Their general expression for the transition probability takes account of all possible paths averaged over energy 305,307 and in this respect is similar to the large-curvature tunneling coefficient that involves, 260,347,[351][352][353][354] for each energy, a convolution of the probability of a given nuclear configuration and the tunneling probability at that configuration, followed by a Boltzmann average over energies.…”
Section: Modelsmentioning
confidence: 99%
“…The first factor f 1 is assumed to arise from protein dynamics, and it is sometimes assumed to be independent of m ; this first factor is the free energy to bring the donor and acceptor into a tunneling‐ready configuration. That concept is reminiscent of the “work term” in Marcus theory 35, 81, 84, 85, 171–173. The work term is the part of the free energy of activation that brings the reactants together without distorting them along the chemical reaction coordinate.…”
Section: Tunneling In Enzymatic Reactionsmentioning
confidence: 99%