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The effect of high pressure on the OH stretch of dilute HOD in D(2)O was examined using high-pressure Fourier transform infrared (FT-IR) spectroscopy. It was found that at pressures directly above the ice VI to ice VII transition, ice VII displays a splitting in the OH absorption indicative of differing hydrogen bonding environments. This result is contrary to published structures of ice VII in which each OH oscillator should experience an identical electronic environment. The anomalous band was found to decrease in absorbance and finally disappear at ∼43.0 kbar. In addition, the pressure response of the amide I' and II' bands of three small model peptides was examined. Analysis of these bands' response to increased pressure indicates significant side-chain dependence of their structural rearrangement, which may play a role in the composition of full length proteins of barophilic organisms.

Type 2 diabetes is characterized by elevated blood glucose levels resulting from a pancreatic β-cell secretory insufficiency combined with insulin resistance, most significantly manifested in skeletal muscle and liver (1). If untreated, diabetic complications develop that cause loss of vision, peripheral neuropathy, impaired kidney function, heart disease, and stroke. The disease has a polygenic basis because numerous genes (the latest count exceeding 20) participate in its pathogenesis, but modern lifestyle characterized by limited physical activity and excessive caloric intake are critical precipitating factors for the current epidemic of type 2 diabetes worldwide (2). It appears that available treatments, including attempts at lifestyle alterations and drug therapies including insulin, are insufficient to stem the tide. Therefore, new approaches, including the development of therapeutic agents with novel mechanisms of action, are needed. Selection of new drug targets to treat type 2 diabetes has to be guided primarily by consideration of established physiological chemistry of glucose homeostasis and of prevailing views about the pathophysiology of type 2 diabetes because the genetics of the disease that could serve as another guiding principle remain prohibitively perplexing. The glucose-phosphorylating enzyme glucokinase (GK) was identified as an outstanding drug target for developing antidiabetic medicines because it has an exceptionally high impact on glucose homeostasis because of its glucose sensor role in pancreatic β-cells and as a rate-controlling enzyme for hepatic glucose clearance and glycogen synthesis, both processes that are impaired in type 2 diabetes (3). Milestones in the 45-year history of GK research are listed in Supplementary Table 1 (Supplementary References S1–S27). In the mid-1990s, Hoffmann La-Roche scientists conducted a high-throughput screen in search of small molecules that could reverse the inhibition of GK by its regulatory protein (GKRP, see further discussion below) and identified a hit molecule that reversed GKRP inhibition by directly stimulating GK (4 …

The stability of bovine lactoperoxidase to denaturation by guanidinium-HCl, urea, or high temperature was examined by differential scanning calorimetry (DSC) and tryptophan fluorescence. The calorimetric scans were observed to be dependent on the heating scan rate, indicating that lactoperoxidase stability at temperatures near Tm is controlled by kinetics. The values for the thermal transition, Tm, at slow heating scan rate were 66.8, 61.1, and 47.2 degrees C in the presence of 0.5, 1, and 2 M guanidinium-HCl, respectively. The extrapolated value for Tm in the absence of guanidinium-HCl is 73.7 degrees C, compared with 70.2 degrees C obtained by experiment; a lower experimental value without a denaturant is consistent with distortion of the thermal profile due to aggregation or other irreversible phenomenon. Values for the heat capacity, Cp, at Tm and Ea for the thermal transition decrease under conditions where Tm is lowered. At a given concentration, urea is less effective than guanidinium-HCl in reducing Tm, but urea reduces Cp relatively more. Both fluorescence and DSC indicate that thermally denatured protein is not random coil. A change in fluorescence around 35 degrees C, which was previously reported for EPR and CD measurements (Boscolo et al. Biochim. Biophys. Acta 1774 (2007) 1164-1172), is not seen by calorimetry, suggesting that a local and not a global change in protein conformation produces this fluorescence change.

Water is a highly polar molecule, consisting of a very electronegative atom, oxygen, bonded to two weakly electropositive hydrogen atoms with two lone pairs of electrons. These features give water remarkable physical properties, some of which are anomalous, such as its lower density in the solid phase compared with the liquid phase. Its ability to serve as both a hydrogen bond donor and hydrogen bond acceptor governs its role as a solvent, a role that is of central interest for biological chemists. In this Account, we focus on water's properties as a solvent. Water dissolves a vast range of solutes with solubilities that range over 10 orders of magnitude. Differences in solubility define the fundamental dichotomy between polar, or hydrophilic, solutes and apolar, or hydrophobic, solutes. This important distinction plays a large part in the structure, stability, and function of biological macromolecules. The strength of hydrogen bonding depends on the H-O...O H-bond angle, and the angular distribution is bimodal. Changes in the width and frequency of infrared spectral lines and in the heat capacity of the solution provide a measure of the changes in the strength and distribution of angles of the hydrogen bonds. Polar solutes and inorganic ions increase the population of bent hydrogen bonds at the expense of the more linear population, while apolar solutes or groups have the opposite effect. We examine how protein denaturants might alter the solvation behavior of water. Urea has very little effect on water's hydrogen bond network, while guanidinium ions promote more linear hydrogen bonds. These results point to fundamental differences in the protein denaturation mechanisms of these molecules. We also suggest a mechanism of action for antifreeze (or thermal hysteresis) proteins: ordering of water around the surface of these proteins prior to freezing appears to interfere with ice formation.

The recently discovered glycine-rich snow flea antifreeze protein (sfAFP) has no sequence homology with any known proteins. No experimental structure has been reported for this interesting protein molecule. Here we report the total chemical synthesis of the mirror image forms of sfAFP (i.e., L-sfAFP, the native protein, and D-sfAFP, the native protein's enantiomer). The predicted 81 amino acid residue polypeptide chain of sfAFP contains Cys residues at positions 1, 13, 28, and 43 and was prepared from four synthetic peptide segments by sequential native chemical ligation. After purification, the full-length synthetic polypeptide was folded at 4 degrees C to form the sfAFP protein containing two disulfides. Chemically synthesized sfAFP had the expected antifreeze activity in an ice recrystallization inhibition assay. Mirror image D-sfAFP protein was prepared by the same synthetic strategy, using peptide segments made from d-amino acids, and had an identical but opposite-sign CD spectrum. As expected, D-sfAFP displays the same antifreeze properties as L-sfAFP, because ice presents an achiral surface for sfAFP binding. Facile synthetic access to sfAFP will enable determination of its molecular structure and systematic elucidation of the molecular basis of the antifreeze properties of this unique protein.

Chemical protein synthesis and racemic protein crystallization were used to determine the X-ray structure of the snow flea antifreeze protein (sfAFP). Crystal formation from a racemic solution containing equal amounts of the chemically synthesized proteins d-sfAFP and l-sfAFP occurred much more readily than for l-sfAFP alone. More facile crystal formation also occurred from a quasi-racemic mixture of d-sfAFP and l-Se-sfAFP, a chemical protein analogue that contains an additional -SeCH2- moiety at one residue and thus differs slightly from the true enantiomer. Multiple wavelength anomalous dispersion (MAD) phasing from quasi-racemate crystals was then used to determine the X-ray structure of the sfAFP protein molecule. The resulting model was used to solve by molecular replacement the X-ray structure of l-sfAFP to a resolution of 0.98 A. The l-sfAFP molecule is made up of six antiparallel left-handed PPII helixes, stacked in two sets of three, to form a compact brick-like structure with one hydrophilic face and one hydrophobic face. This is a novel experimental protein structure and closely resembles a structural model proposed for sfAFP. These results illustrate the utility of total chemical synthesis combined with racemic crystallization and X-ray crystallography for determining the unknown structure of a protein.

In this study, we examine the coupling of a complex ring vibration to solvent through hydrogen-bonding interactions. We compare phenylalanine, tyrosine, l-dopa, dopamine, norepinephrine, epinephrine, and hydroxyl-dl-dopa, a group of physiologically important small molecules that vary by single differences in H-bonding substitution. By examination of the temperature dependence of infrared absorptions of these molecules, we show that complex, many-atom vibrations can be coupled to solvent through hydrogen bonds and that the extent of that coupling is dependent on the degree of both on- and off-ring H-bonding substitution. The coupling is seen as a temperature-dependent frequency shift in infrared spectra, but the determination of the physical origin of that shift is based on additional data from temperature-dependent optical experiments and ab initio calculations. The optical experiments show that these small molecules are most sensitive to their immediate H-bonding environment rather than to bulk solvent properties. Ab initio calculations demonstrate H-bond-mediated vibrational coupling for the system of interest and also show that the overall small molecule solvent dependence is determined by a complex interplay of specific interactions and bulk solvation characteristics. Our findings indicate that a full understanding of biomolecule vibrational properties must include consideration of explicit hydrogen-bonding interactions with the surrounding microenvironment.

The OH stretch mode from water and organic hydroxyl groups have strong infrared absorption, the position of the band going to lower frequency with increased H-bonding. This band was used to study water in trehalose and glycerol solutions and in genetically modified yeast cells containing varying amounts of trehalose. Concentration-dependent changes in water structure induced by trehalose and glycerol in solution were detected, consistent with an increase of lower-energy H-bonds and interactions at the expense of higher-energy interactions. This result suggests that these molecules disrupt the water H-bond network in such a way as to strengthen molecule-water interactions while perturbing water-water interactions. The molecule-induced changes in the water H-bond network seen in solution do not translate to observable differences in yeast cells that are trehalose-deficient and trehalose-rich. Although comparison of yeast with low and high trehalose showed no observable effect on intracellular water structure, the structure of water in cells is different from that in bulk water. Cellular water exhibits a larger preference for lower-energy H-bonds or interactions over higher-energy interactions relative to that shown in bulk water. This effect is likely the result of the high concentration of biological molecules present in the cell. The ability of water to interact directly with polar groups on biological molecules may cause the preference seen for lower-energy interactions.

The heme in horseradish peroxidase (HRP) was replaced by phosphorescent Pt-mesoporphyrin IX (PtMP), which acted as a phosphorescent marker of oxygen quenching and allowed comparison with another probe, Pd-mesoporphyrin IX (Khajehpour et al. (2003) Proteins 53, 656-666). Benzohydroxamic acid (BHA), a competitive inhibitor of the enzyme, was also used to monitor its effects on phosphorescence quenching. With the addition of BHA, in the presence of oxygen, the phosphorescence intensity of the protein increased. In contrast, the addition of BHA, in the absence of oxygen, reduced the phosphorescence intensity of the protein. K(d) = 18 microM when BHA binds to PtMP-HRP. The effect of BHA can be explained by two factors: (1) BHA reduces the accessibility of O(2) to the protein interior and (2) BHA itself quenches the phosphorescence. Consistent with this, the oxygen quenching of the phosphorescence of PtMP-HRP gave a quenching constant of k(q) = 234 mm Hg(-1) s(-1) in the absence of BHA and k(q) = 28.7 mm Hg(-1) s(-1) in the presence of BHA. The quenching rate of BHA is 4000 s(-1). The relative quantum yield of the phosphorescence of the Pt derivative is about six times that of the Pd derivative, whereas the phosphorescence lifetime is approximately eight times shorter. The high quantum yield and suitable lifetime make Pt-porphyrins appropriate as sensors of O(2) diffusion and flexibility in heme proteins.

Fluorescence imaging of cells and tissue can be used to evaluate beta-NADH redox and location. At low temperature, beta-NADH fluorescence intensity increases and therefore sensitivity of imaging increases. In this paper, the temperature dependence of fluorescence was evaluated for beta-NADH in glycerol/water solution and in trehalose/sucrose glass. The average fluorescence lifetime for NADH in glycerol/water is 0.66 ns, compared with 5.3 ns in trehalose/ sucrose at 20 degrees C. Emission spectra were recorded from 290 to 12 K. The fluorescence of beta-NADH in glycerol/water increases approximately 16 fold and the emission shifts about 35 nm to the blue as temperature decreases. Much smaller change is seen for fluorescence of beta-NADH in sugar glass. Below 77 K, the beta-NADH spectral features did not change significantly with temperature change, and so no increase in sensitivity is obtained by going to very low temperatures. It is suggested that the sensitivity of beta-NADH fluorescence is related to water relaxation around the excited state molecule. Differences in water in various tissues may contribute to beta-NADH fluorescence changes when cells are altered.

We present a series of different spectral hole burning experiments, such as aging and waiting time experiments and thermal cycling experiments to gain information on features of the EL of proteins and the associated physics. We focus on heme proteins. Spectral diffusion dynamics in proteins follow a power law in waiting time. If the protein is unfolded the dynamics change to a logarithmic time law as widely observed in glasses. Thermal cycling experiments with proteins show, in addition to random features, also discrete features. There are severe solvent effects demonstrating that the EL is strongly influenced by the solvent. We demonstrate that the hole recovery reaction may strongly depend on protein relaxation, and finally, we link features of the EL to characteristic properties of the folding–unfolding transition.

Pyrene-1-carboxylic acid has a pK of 4.0 in the ground state and 8.1 in the singlet electronic excited state. In the pH range of physiological interest (pH approximately 5-8), the ground state compound is largely ionized as pyrene-1-carboxylate, but protonation of the excited state molecule occurs when a proton donor reacts with the carboxylate during the excited state lifetime of the fluorophore. Both forms of the pyrene derivatives are fluorescent, and in this work the protonation reaction was measured by monitoring steady-state and time-resolved fluorescence. The rate of protonation of pyrene-COO(-) by acetic, chloroacetic, lactic, and cacodylic acids is a function of DeltapK, as predicted by Marcus theory. The rate of proton transfer from these acids saturates at high concentration, as expected for the existence of an encounter complex. Trihydrogen-phosphate is a much better proton donor than dihydrogen- and monohydrogen-phosphate, as can be seen by the pH dependence. The proton-donating ability of phosphate does not saturate at high concentrations, but increases with increasing phosphate concentration. We suggest that enhanced rate of proton transfer at high phosphate concentrations may be due to the dual proton donating and accepting nature of phosphate, in analogy to the Grotthuss mechanism for proton transfer in water. It is suggested that in molecular structures containing multiple phosphates, such as membrane surfaces and DNA, proton transfer rates will be enhanced by this mechanism.

Molecular dynamics simulations and infrared spectroscopy were used to determine the hydrogen bond patterns of glycerol and its mixtures with water. The ability of glycerol/water mixtures to inhibit ice crystallization is linked to the concentration of glycerol and the hydrogen bonding patterns formed by these solutions. At low glycerol concentrations, sufficient amounts of bulk-like water exist, and at low temperature, these solutions demonstrate crystallization. As the glycerol concentration is increased, the bulk-like water pool is eventually depleted. Water in the first hydration shell becomes concentrated around the polar groups of glycerol, and the alkyl groups of glycerol self-associate. Glycerol-glycerol hydrogen bonds become the dominant interaction in the first hydration shell, and the percolation nature of the water network is disturbed. At glycerol concentrations beyond this point, glycerol/water mixtures remain glassy at low temperatures and the glycerol-water hydrogen bond favors a more linear arrangement. High glycerol concentration mixtures mimic the strong hydrogen bonding pattern seen in ice, yet crystallization does not occur. Hydrogen bond patterns are discussed in terms of hydrogen bond angle distributions and average hydrogen bond number. Shift in infrared frequency of related stretch and bend modes is also reviewed.

Infrared (IR) spectroscopy is used for studying the carbohydrate moieties of glycosylated proteins. IR spectra of mono- and disaccharides in the fingerprint region are specific to each sugar and to the environment of the sugar molecules (i.e., aqueous solution or anhydrous glass phase). The IR spectra of glycosylated proteins (mucin, soybean peroxidase, collagen IV, and avidin) were compared with those of the constituent sugars and cytochrome c (a protein with no glycosylation). Our results demonstrate that the IR absorption spectra of glycosylated proteins show distinct absorption bands for the sugar moiety, the protein amide group, and water. Therefore, IR can be used to detect glycosylation.

Molecular dynamics (MD) simulations combined with water-water H-bond angle analysis and calculation of solvent accessible surface area and approximate free energy of solvation were used to determine the influence of hydroxyl orientation on solute hydration and surrounding water structure for a group of chemically identical solutes-the aldohexopyranose sugars. Intramolecular hydrogen bond cooperativity was closely associated with changes in water structure surrounding the aldohexopyranose stereoisomers. The OH-4 group played a pivotal role in hydration as it was able to participate in a number of hydrogen bond networks utilizing the OH-6 group. Networks that terminated within the molecule (OH-4 --> OH-6 --> O-5) had relatively more nonpolar-like hydration than those that ended in a free hydroxyl group (OH-6 --> OH-4 --> OH-3). The OH-2 group modulated the strength of OH-4 networks through syndiaxial OH-2/4 intramolecular hydrogen bonding, which stabilized and induced directionality in the network. Other syndiaxial interactions, such as the one between OH-1 and OH-3, only indirectly affected water structure. Water structure surrounding hydrogen bond networks is discussed in terms of water-water hydrogen bond populations. The impact of syndiaxial versus vicinal hydrogen bonds is also reviewed. The results suggest that biological events such as protein-carbohydrate recognition and cryoprotection by carbohydrates may be driven by intramolecular hydrogen bond cooperativity.

Fluorescent analogues of the potent and highly selective delta-opioid antagonist TIPP (H-Tyr-Tic-Phe-Phe-OH) and TIP (H-Tyr-Tic-Phe-OH) containing the exceptionally environmentally sensitive fluorescent amino acid beta-(6'-dimethylamino-2'-naphthoyl)alanine (Aladan [Ald]) in place of Phe3 were synthesized. The Ald3- and D-Ald3 analogues of TIPP and TIP all retained delta-opioid antagonist properties. The most potent analogue, [Ald3]TIPP, showed a K(e) value of 2.03 nM in the mouse vas deferens assay and five times higher delta vs. mu selectivity (K(i)mu/K(i)delta = 7930) than the TIPP parent peptide in the opioid receptor binding assays. Theoretical conformational analyses of [Ald3]TIPP and [Ald3]TIP using molecular mechanics calculations resulted in a number of low-energy conformers, including some showing various patterns of aromatic ring stacking and others with the Ald side chain and a carbonyl group (fluorescence quencher) in close proximity. These ensembles of low-energy conformers are in agreement with the results of steady-state fluorescence experiments (fluorescence emission maxima and quantum yields) and fluorescence decay measurements (fluorescence lifetime components), which indicated that the fluorophore was either engaged in intramolecular hydrophobic interactions or in proximity of a fluorescence quencher (e.g., a carbonyl group). These fluorescent TIP(P) delta-opioid antagonists represent valuable pharmacological tools for various applications, including studies on membrane interactions, binding to receptors, cellular uptake and intracellular distribution, and tissue distribution.

Phosphorescence of single protein molecules has been directly observed by laser confocal microscopy. The native horseradish peroxidase (HRP) has been converted into a phosphorescent analog (Pt-HRP) by replacing the heme prosthetic group with platinum mesoporphyrin IX (Pt-MP). Oxygen quenching of the triplet state emission of single Pt-HRP molecules has been directly detected and the oxygen quenching constant could be estimated at the single molecule level. The method lays a foundation for experimental studies of the pathways of oxygen diffusion in proteins.

Infrared absorption spectra for liquid and ice H2O and D2O and for protonated and deuterated glycerol/water glasses are compared in the spectral range of 1000−4000 cm-1 and the temperature range of 295−12 K. As temperature decreases, the absorbance bands of the OH and OD stretching modes of glycerol/water solution shift to lower frequency and the band intensifies and narrows. The center of the absorption band for OH stretch for glycerol/D2O/H2O solution (60/32/8 v/v) is at 3364 cm-1 at 295 K and at 3277 cm-1 at 25 K. The full width at half-maximum (fwhm) of the band is 259 cm-1 at 295 K and 186 cm-1 at 25 K. The width of the OH stretch band for D2O that is doped with H2O is 193 cm-1 in liquid (295 K) and 24 cm-1 in ice (12 K). The broader width for the OH stretch at 12 K for glycerol/water relative to that seen in ice is consistent with inhomogeneous broadening due to the glassy nature of glycerol/water solutions. The HOH and DOD bending (scissoring) bands for water in glycerol shift to higher frequency, ...

We present results of a hole burning study with thermal cycling and waiting time spectral diffusion experiments on a modified cytochrome - c protein in its native as well as in its denatured state. The experiments show features which seem to be characteristic for the protein state of matter and its associated dynamics at low temperature. The properties responsible for the observed patterns are organisation paired with randomness and, in addition, the finite size which gives rise to surface and solvent effects. We discuss some general model approaches which might serve as guide lines for understanding these features., To Appear in the Journal of Low Temperature Physics, 2004

The heme of horseradish peroxidase is buried in the protein, but a channel from the protein surface connects the aqueous solution to the heme site. Ferric horseradish peroxidase has an absorption band at 640 nm that is attributed to a charge-transfer (CT) transition between the a 2u HOMO of ﷿ electrons of the porphyrin ring and the dxy/dyz orbital of the ferric ion. Because the water channel extends to the Fe, it seems likely that the CT band will be sensitive to the hydration of the protein. To study this premise, the protein was incorporated into trehalose/sucrose glasses and the hydration of the sugar glasses was varied. Absorption spectra of HRP in sugar glasses and in glycerol/water were taken in the range 10-300 K. The CT absorption band shows vibronic fine structure. The peak positions are the same in hydrated sugar and glycerol/water but the peak positions change in desiccated sugar glass. The data suggest that in hydrated, but not desiccated, sugar glass, water is retained in the heme pocket. Binding of the competitive inhibitor benzohydroxamic acid to the protein increases the CT absorption and resolution. The effect of benzohydroxamic acid on the Fe as calculated using a combination of density functional theory and molecular mechanics is to stabilize the spin state 3 /2 with respect to 5 /2. At low temperature the widths of the lines in the CT band are narrower for the protein in glycerol/water (glass transition at 150 K) than in trehalose/sucrose (glass formation at 65 °C). This indicates that the CT band is inhomogeneously broadened and sensitive to the solvent. The spectral narrowing of the CT absorption occurs as the temperature decreases over the temperature range studied. Water, as indicated by the OH stretch, also shifts in this range. The findings are discussed in terms of how buried water and nearby charges can modulate the activity of the heme.

Oxygen and other molecules of similar size take part in a variety of protein reactions. Therefore, it is critical to understand how these small molecules penetrate the protein matrix. The protein system studied in this case is horseradish peroxidase (HRP). We have converted the native HRP into a phosphorescent analog by replacing the heme prosthetic group by Pd-mesoporphyrin. Oxygen readily quenches the phosphorescence of Pd porphyrins, and this can be used to characterize oxygen diffusion through the protein matrix. Our measurements indicate that solvent viscosity and pH modulate the accessibility of the heme pocket relative to small molecules. The binding of the substrate benzohydroxamic acid (BHA) to the protein drastically impedes oxygen access to the heme pocket. These results indicate that, first, the penetration of small molecules through the protein matrix is a function of protein dynamics, and second, there are specific pathways for the diffusion of these molecules. The effect of substrate and pH on protein dynamics has been investigated with the use of molecular dynamics calculations. We demonstrate that the model of a "fluctuating entry point," as suggested by Zwanzig (J Chem Phys 1992;97:3587-3589), properly describes the diffusion of oxygen through the protein matrix.

We examined the hydration of amides of alpha(3)D, a simple, designed three-helix bundle protein. Molecular dynamics calculations show that the amide carbonyls on the surface of the protein tilt away from the helical axis to interact with solvent water, resulting in a lengthening of the hydrogen bonds on this face of the helix. Water molecules are bonded to these carbonyl groups with partial occupancy ( approximately 50%-70%), and their interaction geometries show a large variation in their hydrogen bond lengths and angles on the nsec time scale. This heterogeneity is reflected in the carbonyl stretching vibration (amide I' band) of a group of surface Ala residues. The surface-exposed amides are broad, and shift to lower frequency (reflecting strengthening of the hydrogen bonds) as the temperature is decreased. By contrast, the amide I' bands of the buried (13)C-labeled Leu residues are significantly sharper and their frequencies are consistent with the formation of strong hydrogen bonds, independent of temperature. The rates of hydrogen-deuterium exchange and the proton NMR chemical shifts of the helical amide groups also depend on environment. The partial occupancy of the hydration sites on the surface of helices suggests that the interaction is relatively weak, on the order of thermal energy at room temperature. One unexpected feature that emerged from the dynamics calculations was that a Thr side chain subtly disrupted the helical geometry 4-7 residues N-terminal in sequence, which was reflected in the proton chemical shifts and the rates of amide proton exchange for several amides that engage in a mixed 3(10)/alpha/pi-helical conformation.

The reactive site structure and CO IR spectral signature of horseradish peroxidase complexed with CO were studied using a combination of density functional theory and molecular modeling. The quantum chemical model used included the proximal His170, the distal amino acids His42 and Arg38, and the crystallographic water molecule that interacts with CO, His42, and Arg38. The mutant H42L was simulated by removing distal histidine from the cluster and the mutant R38L by removing the arginine. In the models where the Arg38 is present a hydrogen bond interaction is found between the He of Arg and the oxygen of adduct -CO. When both His42 and Arg38 are present they interact with the CO moiety, but they also interact with each other so their effect is not simply additive. The effect of a change in pH was modeled by removing potentially titratable hydrogen atoms identified by molecular mechanics and Poisson-Boltzmann pK a calculations on the active site. Previously observed IR spectral features of CO as a function of pH and active site mutations could be interpreted primarily in terms of changes in CO and Fe-CO bond lengths produced by changes in active site composition and charge state. The effect of the charge relay due to the possible second deprotonation (assuming that the first deprotonation took place in the His42) from the Arg38 or H Φ in the proximal His170 gives a decrease of the CO stretching frequency.

The effects of nitroprusside and S-nitrosocysteine, compounds that generate nitric oxide (NO), on synaptosomal energy-producing pathways and energy level were investigated. The decrease in respiration was much faster and more pronounced with S-nitrosocysteine than with nitroprusside. S-Nitrosocysteine, at 10 microM, inhibited by 80% respiration with glucose and succinate (plus rotenone) in intact synaptosomes and with ascorbate/cytochrome c in broken preparations. Oxygenated hemoglobin reversed and/or prevented the inhibition, whereas glutathione (GSH) prolonged it. Under aerobic conditions, the synaptosomal energy level (creatine phosphate/creatine and ATP/ADP ratios) was reduced by the presence of S-nitrosocysteine, whereas lactate generation was enhanced. The effects on energy parameters were greater at 5 min than at 15 min of incubation and were more pronounced in the presence of GSH. Under strictly anaerobic conditions, lactate production was reduced by the NO-generating compounds in a concentration-dependent manner. It is concluded that (a) inhibition of oxidative phosphorylation by NO leads to a fall in the synaptosomal energy level, which in turn stimulates glycolysis; (b) glycolysis can be inhibited by higher concentrations of the radical; and (c) inhibitory effects on the energy-generating pathway and ATP level could contribute to NO toxicity under some in vivo situations.

The spectral diffusion dynamics of free base cytochrome c (H2-Cc) in a dry trehalose film is tremendously enhanced as compared to a glycerol/water glass. We show that relaxation as well as fluctuation processes contribute to the spectral diffusion dynamics. Relaxation shows up in aging phenomena which can be measured in a separate fashion. In both solvents, the spectral diffusion as well as the aging dynamics follow power laws in time. The respective exponents are quite different, yet the influence of the solvent on them is only marginal. The large difference in the magnitude of the spectral diffusion dynamics in the two solvents can be traced back to a correspondingly large difference in the inhomogeneous width which itself seems to come from the much higher glass transition temperature in trehalose, which is close to the unfolding temperature of cytochrome c.

Porphyrin electronic transitions in heme proteins provide a useful tool for probing the protein environment, since the surrounding protein affects the porphyrin π-electron cloud. Perturbations can arise from structural distortions of the porphyrin ring, from the internal electric field generated by charged and polar groups, or from axial ligation to the heme iron. In this work, cytochrome c in aqueous solution or in glasses of trehalose or glycerol/water was examined as a function of temperature to evaluate the effect of fluctuations on the heme. The amide I band of cytochrome c in trehalose remains constant over a wide temperature excursion, indicating that interactions between the protein and the matrix do not change with temperature. The width of the Q(0,0) optical transition measured at low temperature (i.e.

The formation of chemisorbed monolayers of yeast cytochrome c on both uncharged polar and nonpolar soft surfaces of organic self-assembled monolayers (SAM) on solid inorganic substrates was followed in situ by polarized total internal reflection fluorescence. Two types of nonpolar surfaces and one type of uncharged polar surface were used. The first type of nonpolar surface contained only thiol endgroups, while the other was composed of a mixture of thiol and methyl endgroups. The uncharged polar surface was provided by the mixture of thiol and hydroxyl endgroups. The thiol endgroups were used to form a covalent disulfide bond with the unique surface-exposed cysteine residue 102 of the protein. The mean tilt angle of the protein's zinc-substituted porphyrin was found to be 41 degrees and 50 degrees for the adsorption onto the nonpolar and uncharged polar surfaces, respectively. The distribution widths for the pure thiol and the thiol/methyl and thiol/hydroxyl mixtures were 9 degrees, 1 degrees, and 18 degrees, respectively. The high degree of the orientational order and good stability achieved for the protein monolayer on the mixed thiol/methyl endgroup SAM makes this system very attractive for studies of both intramolecular and intermolecular electron transfer processes.

We have recently demonstrated that metalloporphyrins are potent inhibitors of both human immunodeficiency virus type 1 (HIV-1) and human immunodeficiency virus type 2 (HIV-2) reverse transcriptases (RTs) [Argyris, E.G., Vanderkooi, J.M., Venkateswaran, P.S., Kay, B.K., and Paterson, Y. (1999) J. Biol. Chem.274, 1549–1556]. In addition, by screening a phage peptide library we discovered that a peptide with sequence similarity to residues 398–407 from the connection subdomain of HIV RTs binds heme. These findings suggested that this highly conserved region may be the binding site for metalloporphyrins and a novel site for inhibition of enzymatic activity. Our most recent data presented here confirm this suggestion. Screening of HIV-1 RT 398–407 peptide analogs by fluorescence assays demonstrates that Trp residues at positions 401 and 402 are important for heme binding. Furthermore, site-directed mutagenesis of these residues verified these findings and indicated that heme inhibits HIV-1 RT by binding on the connection subdomain of the p66 subunit of the enzyme but not on the p51 subunit. This was also confirmed by analyzing the binding affinities of heme for mutant HIV-1 RT heterodimers, using intrinsic fluorescence assays. The clear identification of the connection domain as a novel inhibition site is crucial in understanding the mechanism of heme binding and enzymatic inhibition and will facilitate the generation of novel porphyrin-based inhibitors of RT.

A combination of simulations and Fourier transform infrared spectroscopy was used to examine the effect of three ionic solutes (KCl, NaCl, and KSCN), the polar solute urea, and the osmolyte trimethylamine-N-oxide (TMAO) on a water structure. The ionic solutes increase the mean water–water H-bond angle in their first hydration shell concomitantly shifting the OH stretching mode to higher frequency, and shifting the HOH bending mode to lower frequency. TMAO decreases the mean water–water H-bond angle in its first hydration shell, shifts the OH stretching mode frequency down, and shifting the HOH bending mode frequency up. Urea has no effect on the mean H-bond angle, OH stretch, and HOH bend frequencies. These results can be explained in terms of changes in the relative proportions of two H-bond angle populations: Ionic solutes increase the population of more distorted (larger angle) H bonds relative to the less distorted population, TMAO has the reverse effect, while urea does not affect the H-bond angle probability distribution. The negligible effect of urea on water structure supports the direct binding model for urea-induced protein denaturation.

We present in this work low-temperature visible absorption spectra for recombinant Thermus thermophilus cytochrome c552. The Q-band presents a remarkable splitting at low temperature. We performed quantum chemical calculations to evaluate quantitatively the effect of heme conformation, axial ligand, peripheral substituents and local electric fields on the electronic spectra. In an attempt to find correlation between protein structure and spectral splitting, we carried out the same calculations on three other cytochrome c's: horse heart, tuna heart, and yeast. The quantum chemical calculations were performed at the INDO level with extensive configuration interaction. The electric field at the heme pocket was included in the calculations through a set of point charges fitting the actual electric field. The results obtained show clearly that all mentioned effects contribute to the observed spectral splitting in a complex nonadditive way.

Infrared spectral frequencies of amide vibrational modes are sensitive to secondary structure. In this work, evidence is presented that accessibility to water additionally affects spectral positions. The dimeric α-helical coiled-coil GCN4-P1‘ was 13C labeled in the amide carbonyl groups of buried Leu or exposed Ala. At 20 °C, the amide I‘ peak for 13C Ala amide is at 1585 cm-1, whereas the position for 13C Leu is at 1606 cm-1. These shifts permit the distinction of solvent-exposed and buried amide groups. Lowering temperature increases H-bond strength, producing a shift to lower frequency. In the temperature range from 10 to 273 K in aqueous glycerol, the amide transitions assigned to solvent-exposed regions of the helices undergo the strongest temperature-dependent shifts, similar to that of the peptide bond model compound, N-methylacetamide, in the same aqueous solvent. In addition, spectral shifts of the amide bands for N-methylacetamide and the solvent-exposed component of the proteins follow the glas...

Low-temperature UV−vis absorption and Stark-effect hole-burning spectra of Zn substituted cytochrome c are studied experimentally and theoretically using quantum mechanical and Poisson−Boltzmann el...

We report on a comparative investigation of the heme pocket fields of two Zn-substituted c -type cytochromes—namely yeast and horse heart cytochromes c —using a combination of hole burning Stark spectroscopy and electrostatic calculations. The spectral hole burning experiments are consistent with different pocket fields experienced at the hemes of the respective cytochromes. In the case of horse heart Zn-cytochrome c , two distinguishable electronic origins with different electrostatic properties are observed. The yeast species, on the other hand, displays a single electronic origin. Electrostatic calculations and graphics modeling using the linearized finite-difference Poisson-Boltzmann equation performed at selected time intervals on nanosecond-molecular dynamics trajectories show that the hemes of the respective cytochromes sample different potentials as they explore conformational space. The electrostatic potentials generated by the protein matrix at the heme show different patterns in both cytochromes, and we suggest that the cytochromes differ by the number of "electrostatic substates" that they can sample, thus accounting for the different spectral populations observed in the two cytochromes.

Resonance Raman and UV-visible absorption spectra show that nickel(II) microperoxidase-11 (NiMP-11) is four-coordinate in aqueous solution in the pH range from 1.0 to 13.0. In aqueous solutions of NiMP-11 in the absence of cetyltrimethylammonium bromide (CTAB), NiMP-11 is aggregated. In CTAB micellar solutions, where aggregation of NiMP-11 does not occur, the Raman spectra of NiMP-11 are similar to that of nickel(II) cytochrome c (NiCyt-c). The presence of the peptide segment shifts the equilibrium heavily in favor of the nonplanar form, just as does the entire protein component in the case of NiCyt-c. This further elucidates the structural mechanism by which the protein segment ruffles the heme, most likely modulating the redox potential as indicated for the cytochromes c3 [Ma, J.-G., et al. (1998) Biochemistry 37, 12431-12442]. Furthermore, the hydrophobic environment that is provided by the CTAB micelle is found to be crucial to the native folding of the pentapeptide and formation of two hydrogen bonds in the peptide backbone. These two H-bonds act to contract the peptide segment exerting the force on the macrocycle that causes the ruffling and makes the redox potential more negative than if the heme were to remain planar. The structure of the heme and pentapeptide may also be associated with redox-linked triggering of the formation and release of cytochrome-protein complexes.

Spectral diffusion waiting time experiments at 100 mK combined with aging time experiments are used to shed light on the features of the energy landscape of a cytochrome c-type protein and the respective conformational dynamics. The energy landscape shows features of a hierarchical organization. The time law which governs the dynamics in conformational phase space is a power law. The respective processes seem to be related to generalized diffusive-like motions.

Charged groups reside mainly on protein surfaces, but for proteins that incorporate redox centers, a charge typically exists at the prosthetic group within the interior. How a protein accommodates a buried charge and the effect of redox changes on protein stability are thermodynamically related problems. To examine these problems in cytochrome c, the metal-free protein was used as a model. When pH is lowered, the neutral, monocation, and dication forms of the porphyrin are progressively formed as indicated by their characteristic absorption spectra. Infrared studies of the protein over this pH range show that the protein remains in a predominately alpha-helical structure, although the carboxyl groups of the dicarboxylic amino acids become protonated at lower pH. The monocation porphyrin form (which has not been previously reported in a protein and is a charge analogue of ferric heme) has a fluorescence maximum at 609 nm. The pKs for the respective one and two protonation of the porphyrin pyrrole Ns are 3.2 and 1.6 for the folded protein, and 4.4 and 3.1 for the unfolded protein. These values indicate that the protection of the polypeptide chain for protonation is approximately 3 kcal.

Three ways are generally used to visualize proteins: (1) a static model in which the atomic positions are defined, (2) a dynamic model taking into account fluctuations, and (3) a reactive model that reflects the internal and external electric fields of the molecule. The properties of chromophoric prosthetic groups can be probed by optical spectroscopy, and when high resolution techniques are used, the results reveal information about the local electric fields in proteins, as influenced and determined by atomic positions and dynamics.

Resonance Raman spectra with Q-band excitation are reported for microperoxidase-11, the cytochrome c analog. Spectra were acquired in the mid-frequency range for the oxidized, and reduced forms of the undecapeptide, as well as for the imidazole and carbonyl complexes. Oxidation and spin state marker bands of the undecapeptides are consistent with a six-coordinate, low spin iron in both oxidation states. Porphyrin core size correlations yield a porphyrin-centre to pyrrole-nitrogen distance of 2.00 A for MP11, suggestive of a six-coordinate species in a distorted heme environment. Molecular dynamics results show that the non-planarity of the heme of the parent cytochrome is conserved in the microperoxidase and its carbonmonoxy analog.

We performed hole burning Stark effect experiments on a cytochrome c type protein. From the behavior of the holes in an external electric field conclusions on local electric fields in the heme pocket can be drawn. We varied the pH value in order to study the influence of different groups on the pocket field: (a) titratable amino acid residues, (b) the porphyrin side chains (especially the propionates) and (c) the two axial ligands His18 and Met80. Surprisingly, a variation of the pH between 4.1 and 12.7 has no influence on the Stark effect. However, at a pH-level

The effect of the orientation of CO bound to the heme of two c-type cytochromes on the CO-stretch frequency νCO has been investigated using molecular mechanics and finite difference Poisson−Boltzmann calculations. Our approach treats the charge distribution of the protein as an external electric field capable of inducing Stark frequency shifts. Results show that modifying the Fe−C−O bending angle (β) does not change the CO stretch frequency within a range of 100−175°, equivalent to a bending motion away from the propionic acid chains. The calculated Stark shifts range from 5.4 to 8.6 cm-1 and are in good agreement with the experimentally observed shift (6 cm-1). However, motion of the CO toward the propionics exerts significant influence on the calculated shifts (−4.5 to −1.8 cm-1), which are then in total disagreement with experiment, not only in magnitude but also in predicting the wrong direction for the shift. The Stark shifts calculated for the tilt angle (τ) show that it has no significant effect on...

The absorption spectra of 20 amino acids (Gly, Ala, Val, Leu, Ile, Ser, Thr, Asp, Asn, Glu, Gln, Lys, His, Arg, Phe, Trp, Cys, Met, Pro, and hexafluorovaline) and some of their metabolites (α-ketoglutarate, oxalacetate, pyruvate, succinate, citrate, and acetate) were determined in the infrared (IR) region from 1300 to 1700 cm−1 under conditions that are appropriate for biological studies (i.e., in phosphate-buffered D2O solution). The strongest transition in this region is , with an extinction coefficient ∼1 mM−1 cm−1, and an emphasis was made to demonstrate use of this transition for enzymatic assays and to study proteins. To these ends, these relevant features were demonstrated. The value for is a function of the residue pK: the higher the frequency, the lower the pK of the carboxylic acid. The high extinction of permits detection of carboxyl groups in parvalbumin, a protein that is rich in Asp and Glu. The IR profiles for the amino acids and their metabolite products are sufficiently characteristic so that IR can be used to monitor enzymatic reactions involving amino acids. We show that transaminase reactions, which interconvert amino and keto acids, can be monitored by IR. © 1997 John Wiley & Sons, Inc. Biospectroscopy 3: 457–467, 1997

We performed hole-burning Stark effect experiments on cytochrome c in which the iron of the herne was either removed or replaced by Zn. According to the experiments, the free-base compound has an effective inversion center, even in the protein. The Zn compound, on the other hand, shows quite peculiar features: in the low-frequency range of the inhomogeneous band, it definitely has a dipole moment, as indicated by a splitting of the hole in the external field. However, in the maximum of the inhomogeneous band, a severe charge redistribution occurs, as the experiments show. In addition to the Stark experiments, we performed calculations of the electrostatic fields at the pyrrole rings and at the metal site of the heme group. We interpret our findings with a model based on structural hierarchies: the protein can exist in a few subconformations, which can be distinguished through the structure of the heme pocket. The different pocket structures support different structures of the chromophore, which, in turn, can be distinguished through their behavior in an external field. These distinct structures, in turn, correspond to a rather broad distribution of protein structures, which leave, however, the pocket structure largely unchanged. These structures show up in inhomogeneous broadening.

We report electrostatic potential and electric field calculations at the CO ligand of the heme in both horse heart and yeast cytochrome c, obtained from a finite difference solution to the Poisson−Boltzmann equation. This method takes into account the protein shape and charge distribution, as well as the solvent and generalized ionic strength effects. The calculations support recent experimental and theoretical evidence suggesting that polar interactions can significantly affect the vibrational frequency of the ligand. Our work shows that the ionizable amino acid residues and polar contributions of the protein matrix can induce a Stark effect on the CO stretch frequency of the carbonmonoxycytochromes. The observed CO stretches, at 1965.9 and 1960.1 cm-1 for horse and yeast cytochromes c, respectively, show that the experimental shift is of the order of 6 cm-1. This is in good agreement with a calculated value of 8 cm-1 (±1 cm-1) for a vibrational Stark shift due to the different charge distributions in bo...

The photoactivated metastable triplate states of the porphyrin (free-base, i.e., metal-free) zinc and tin derivatives of horse cytochrome c were investigated using electron paramagnetic resonance. Zero-field splitting parameters, line shape, and Jahn-Teller distortion in the temperature range 3.8-150 K are discussed in terms of porphyrin-protein interactions. The zero-field splitting parameters D for the free-base, Zn and Sn derivatives are 465 x 10(-4), 342 x 10(-4) and 353 x 10(-4) cm-1, respectively, and are temperature invariant over the temperature ranges studied. AN E value at 4 K of 73 x 10(-4) cm-1 was obtained for Zn cytochrome c, larger than any previously found for Zn porphyrins derivatives of hemeproteins, showing that the heme site of cytochrome c imposes an asymmetric field. Though the E value for Zn cytochrome c is large, the geometry of the site appears quite constrained, as indicated by a spectral line shape showing a single species. Intersystem crossing occurred predominantly to the T2 > zero-field spin sublevel. EPR line shape changes with respect to temperature of Zn cyt c are interpreted in terms of vibronic coupling, and a maximum Jahn-Teller crystal-field splitting of approximately 180 cm-1 is obtained. Sn cytochrome c in comparison with the Zn protein exhibits a photoactivated triplet line shape that is less well resolved in the X-Y region. The magnitude of E value is approximately 60 x 10(-4) cm-1 at 4 K; its value rapidly tends toward zero with increasing temperature, from which a value for the Jahn-Teller crystal-field splitting of > or = 40 cm-1 is estimated. In contrast to those for the metal cytochromes, the magnitude of E value for the free-base derivative was essentially zero at all temperatures studied. This finding is discussed as a consequence of an excited-state tautomerization process that occurs even at 4 K.

The interaction of spermine, spermidine and putrescine with the Ca(2+)-binding protein, parvalbumin, was studied at pH 6 and 7, with the help of the intrinsic fluorescence properties of tryptophan and circular dichroic spectroscopy of the protein in the ultraviolet region. Polyamines bind to parvalbumin that is either Ca(2+)-free or partially saturated with Ca2+, as indicated by a change in the emission maximum and intensity of tryptophan fluorescence. The binding affinities for the interactions are about 4 mM, 8 mM and > 20 mM for spermine, spermidine and putrescine, respectively. No alterations in fluorescence properties were detected when the polyamines were added to fully Ca(2+)-bound parvalbumin. An increase in the ellipticity of the circular dichroic spectrum in the region where tryptophan absorbs was observed when polyamines were added to Ca(2+)-free parvalbumin. This finding indicates that polyamine binding affects the segment of the protein where tryptophan is located. Based on these results it is postulated that polyamines bind to the Ca(2+)-free or partially saturated parvalbumin and stabilize its structure.

Optical and proton nuclear magnetic resonance (NMR) studies were carried out to assess the structure of the polypeptide chain and metal ligation in zinc-substituted horse heart cytochrome c (Zn Cyt c). The 1D- and 2D-NMR (COSY, TOCSY, and NOESY) spectra allowed the assignment of proton resonances in 67 amino acid residues. These residues arose from all structural elements of the protein, alpha-helices, beta-turns, and segments of the protein with no defined secondary structure. Small deviations of the chemical shifts of Zn Cyt c proton resonances from native Fe(II) Cyt c of less than 0.1 ppm are due to not fully matching solvent conditions. Differences in the chemical shifts between the two proteins in the range 0.10-0.20 ppm are not clustered and are observed not only in the vicinity of the Zn porphyrin but also on distant surface locations of the cytochrome. The resonance positions of the bridge protons, from the thioether bonds of the porphyrin with Cys 14 and Cys 17, were conserved in Zn Cyt c. Similarly, the Met 80 and His 18 protons had chemical shifts supporting the proposal that His 18 and Met 80, as for Fe(II) Cyt c, may provide the axial ligation in the Zn protein and that zinc may be in an unusual hexacoordinated geometry. Chemical shifts from proton resonances of alternative axial ligands of misfolded cytochrome like His 33, Lys 79, and Phe 82 were found to be the same as in the Fe(II) protein, excluding the possibility of their axial ligation to Zn. The His 18-Zn-Met 80 ligation was also consistent with data from absorption and luminescence studies. We conclude that Zn Cyt c is an adequate structural model for Fe(II) Cyt c as both share the same overall structure, including axial ligands, environment in the porphyrin vicinity, and the same binding interface with redox partners.

Fluorescence-line-narrowing (FLN) spectra are presented for Sn cytochrome c (Snc) obtained under Q0-0 and Q0-1 excitation and for Zn cytochrome c (Znc) under Q0-1 excitation. Vibrational frequencies of the ground and first excited states are reported for Snc. Additional excited-state Znc frequencies are also presented, thus contributing to a previous FLN Znc investigation. The spectra of Snc shows more phonon broadening than for Znc, but vibrational frequencies of the S0 and S1 states could be obtained and the distribution function of the 0, 0 transition was determined. Snc and Znc showed good agreement in their excited-state vibrational frequencies. Some S1 vibrational frequencies of Znc are seen to downshift with respect to ground-state vibrations, suggesting that the porphyrin S0 to S1 expansion observed in other porphyrin systems also occurs in cytochrome c derivatives. © 1995 John Wiley & Sons, Inc.

The fluorescence properties of porphyrin were compared in protoporphyrin-protoheme hybrid hemoglobins (Hb) in which the protohemes (Fe) in either the alpha or beta subunits were substituted with protoporphyrin IX, alpha (P)2 beta (Fe)2-Hb and alpha (Fe)2 beta(P)2-Hb, respectively. The fluorescence lifetimes of the porphyrin in these hybrid derivatives are shorter than for the tetra-substituted protoporphyrin Hb, indicating that there is energy transfer from the porphyrin to the heme. The energy transfer resulted in only approximately 20% diminution of donor fluorescence, thereby allowing for the examination by fluorescence of the interaction of porphyrin with a given subunit peptide chain. Fluorescence line-narrowing spectroscopy, a high resolution fluorescence technique that involves laser excitation, produced vibrationally resolved emission spectra in which the zero phonon lines were separated from a broadened background consisting of phonon wings. Resolved spectra were obtained in the temperature range of 5-50 K; above 70 K the spectra were unresolved. By changing the excitation frequency the mean energy of the 0,0 transition, characterizing the separation in energy between the ground and excited states, can be determined. For both derivatives a bimodal distribution was seen, indicating that more than one conformation of molecules was present. The distribution of 0,0 transition energies of the porphyrin in the beta-chain in alpha(Fe)2 beta(P)2-Hb was shifted to lower energy relative to the alpha chain in alpha(P)2 beta(P)2-Hb, whereas the excited state molecules in the two subunits had very little difference in vibrational energy. These data point to the same configuration of the porphyrins in the two sites, but differences in the electric field for the alpha and beta subunits.

The reactivity of nitric oxide under a given condition is a complex function of its diffusivity and the concentration of reacting partners. Quenching by NO of luminescence from Ru and Pd chelates of mesoporphyrin IX, two molecules which exhibit phosphorescence at room temperature, was utilized to evaluate the gas concentration and apparent diffusion coefficients. The properties of Ru-mesoporphyrin, a dye not previously employed as a probe for O2 or NO, were determined and the assay was verified and used to quantify NO produced by decomposition of nitrosocysteine. The pseudo-second order quenching constants were obtained from Stern-Volmer plots measured under various conditions and used to calculate diffusion coefficients for nitric oxide in solutions, proteins and membranes. The diffusion coefficients were greater at 37 than at 25 degrees C and, at a given temperature, smaller in proteins and membranes than in water. The conclusion is that NO and O2 closely resemble each other in diffusivity but that NO is slightly less lipophilic, resulting in somewhat faster apparent diffusion in protein and slower diffusivity in lipid, relative to O2. Taking a mean diffusion coefficient for NO of 10(-7) cm2s-1, then within 10 s the mean path is 10(-3) cm, or less than the diameter of a single cell. However, at low NO and O2 concentrations, the halflife of NO will be considerably longer than 10 s, and consequently the path of NO diffusion much greater.