Intramolecular electron transfer in azurin in water and deuterium oxide has been studied over a broad temperature range. The kinetic deuterium isotope effect, k H͞kD, is smaller than unity (0.7 at 298 K), primarily caused by the different activation entropies in water (؊56.5 J K ؊1 mol ؊1 ) and in deuterium oxide (؊35.7 J K ؊1 mol ؊1 ). This difference suggests a role for distinct protein solvation in the two media, which is supported by the results of voltammetric measurements: the reduction potential (E 0 ) of Cu 2؉͞؉ at 298 K is 10 mV more positive in D2O than in H2O. The temperature dependence of E 0 is also different, yielding entropy changes of ؊57 J K ؊1 mol ؊1 in water and ؊84 J K ؊1 mol ؊1 in deuterium oxide. The driving force difference of 10 mV is in keeping with the kinetic isotope effect, but the contribution to ⌬S ‡ from the temperature dependence of E 0 is positive rather than negative. Isotope effects are, however, also inherent in the nuclear reorganization Gibbs free energy and in the tunneling factor for the electron transfer process. A slightly larger thermal protein expansion in H 2O than in D2O (0.001 nm K ؊1 ) is sufficient both to account for the activation entropy difference and to compensate for the different temperature dependencies of E 0 . Thus, differences in driving force and thermal expansion appear as the most straightforward rationale for the observed isotope effect. K inetic deuterium or tritium isotope effects (KIE) have long been recognized to reflect crucial mechanistic features in proton and hydrogen atom transfer processes (see, for example, refs. 1-6). KIE were also introduced early as a mechanistically diagnostic tool in hydrolytic metalloenzyme catalysis (7-8). Studies of KIE in metalloenzyme catalysis during the last decade have incorporated increasingly detailed theoretical notions (7-11), for example: proton͞deuteron tunneling and multiphonon environmental vibrational excitation (4-6, 12-16); gated proton͞deuteron transfer (6,(12)(13)(14); proton͞deuteron transfer and shallow barriers (17-20); coupled multiproton transfer (17, 21); and stochastic molecular (13-15) and bulk environmental control (12,22).Theoretical frames for proton tunneling and KIE are most straightforward when the barriers for proton transfer are high, yielding large values of the KIE (Ͼ Ͼ1), measured as the ratio between the rate constant for proton and deuteron (or triton) transfer. Proton͞deuteron tunneling is here strongly conspicuous. This partially adiabatic limit (4, 6), applies particularly to proton or hydrogen atom transfer between C-donor or -acceptor atoms. Proton transfer between O-and N-donor or -acceptor atoms mostly displays small values (KIE ϭ 1-2.5), reflecting strong hydrogen bond interactions, facile mutual approach between the donor and acceptor groups, and shallow barriers. These barriers correspond to the fully adiabatic limit (4), where the dominating effect of the KIE is reflected in isotopedependent splitting in the crossing region of the appropriate potential surfaces (6)...