D2O Buffer Research Articles

Notable deuterium effect on the electron transfer rate of myoglobin

The electron transfer reaction of wild-type myoglobin at an electrode was significantly facilitated in a D2O buffer as compared with that in an H2O buffer, with k(0)'(H2O)/k(0)'(D2O)= 0.13, while a minimal deuterium kinetic isotope effect on the myoglobin with modification at distal histidine (His-64) was observed.

The polymerization of actin: Thermodynamics near the polymerization line

Studies of the dependence of actin polymerization on thermodynamic parameters are important for understanding processes in living systems, where actin polymerization and depolymerization are crucial to cell structure and movement. We report measurements of the extent of polymerization, Φ, of rabbit muscle actin as a function of temperature [T=(0–35) °C], initial G-actin concentration [[G0]=(1–3) mg/ml], and initiating salt concentration [[KCl]=(5–15) mmol/l with bound Ca2+], in H2O and D2O buffers and in the presence of adenosine triphosphate (ATP). A preliminary account of the data and analysis for H2O buffers has appeared previously [P. S. Niranjan, J. G. Forbes, S. C. Greer, J. Dudowicz, K. F. Freed, and J. F. Douglas, J. Chem. Phys. 114, 10573 (2001)]. We describe the details of the studies for H2O buffers, together with new data and analysis for D2O buffers. The measurements show a maximum in Φ(T) for H2O buffers and D2O buffers. For H2O buffers, Tp decreases as either [G0] or [KCl] increases. For D2O buffers, Tp decreases as [KCl] increases, but Tp is not monotonic in [G0]. The measurements are interpreted in terms of a Flory–Huggins-type lattice model that includes the essential steps: monomer activation, dimerization of activated species, and propagation of trimers to higher order polymers. The competition between monomer activation and chain propagation leads to the observed nonmonotonic variation of Φ(T). The actin polymerization in D2O buffer differs considerably from that in the H2O buffer and underscores the significant deuterium effect on hydrophobic interactions and hydrogen bonding in the polymerization process.

Substrate binding to NO-ferro-naphthalene 1,2-dioxygenase studied by high-resolution Q-band pulsed 2H-ENDOR spectroscopy.

The active site of naphthalene 1,2-dioxygenase (NDO) contains a Rieske Fe-S cluster and a mononuclear non-heme iron, which are contributed by different alpha-subunits in the (alphabeta)(3) structure. The enzyme catalyzes cis-dihydroxylation of aromatic substrates, in addition to numerous other adventitious oxidation reactions. High-resolution Mims (2)H-ENDOR (electron nuclear double resonance) spectra have been recorded for the NO-ferrous center of NDO bound with the substrates d(8)-naphthalene, d(2)-naphthalene, d(8)-toluene, d(3)-toluene, and d(6)-benzene; samples were prepared in a D(2)O buffer to test for solvent-derived ligands; spectra were collected for enzymes with the Rieske diiron center in both its oxidized and reduced states. A sharp quartet ENDOR pattern from a nearby deuteron of the substrate in a major binding geometry (denoted as A) was detected for all perdeuterated substrates. Examination of the sample prepared with 1,4-di-deutero-naphthalene shows that the signal arises from D1. Analysis of two-dimensional (2-D) orientation-selective ENDOR patterns collected for this sample defined the location of the D1 deuteron, with respect to the g-frame of the iron center and the orientation of the C-D1 bond. Consideration of the orientations of naphthalene that are permitted within the constraints of these results, as supported by a novel approach to simulations of orientation-selective, 2-D ENDOR patterns for the perdeuterated naphthalene sample, which summed contributions from D1/D2/D8, disclose the geometry of the naphthalene and the Fe-NO fragment. The two deuterons of the reactive carbons, D1 and D2, are closest to the Fe atom (r(Fe)(-)(D1) approximately 4.3 A, r(Fe)(-)(D2) approximately 5.0 A), whereas D8 is farther away (r(Fe)(-)(D8) approximately 5.3 A). Perhaps more instructive, D1-N and D2-N distances to the O(2) surrogate, NO, are approximately 2.4 and approximately 3.3 A, respectively, whereas the D8-N distance is approximately 3.7 A. The data show that benzene and the aromatic ring of toluene also sit within the substrate-binding pocket adjacent to the mononuclear Fe atom. These rings occupy a position similar to that of the "proximal" ring of naphthalene, with the closest ring deuteron being located at a distance of approximately 4.3-4.4 A from the Fe atom and with the Fe-D vector being slightly off the Fe-N(O) direction. In particular, comparison of the data for d(8)-toluene and methyl-d(3)-toluene shows that the methyl group of toluene points away from the Fe atom, despite observations that the oxidation of toluene occurs at the methyl group during catalysis. The Rieske cluster is reduced during both steady-state and single-turnover catalysis; therefore, the effect of its oxidation state on the geometry of substrate binding was examined. The spectra from the NDO-naphthalene complex also revealed a second binding conformation (denoted as B), in which the substrate is located approximately 0.5 A farther from the Fe atom. The relative populations of A- and B-sites are allosterically changed when the Rieske cluster is reduced. ENDOR of exchangeable protons shows that the water/hydroxide of Fe-NDO is retained upon binding NO.

Congo Red Populates Partially Unfolded States of an Amyloidogenic Protein to Enhance Aggregation and Amyloid Fibril Formation

Congo red (CR) has been reported to inhibit or enhance amyloid fibril formation by several proteins. To gain insight into the mechanism(s) for these apparently paradoxical effects, we studied as a model amyloidogenic protein, a dimeric immunoglobulin light chain variable domain. With a range of molar ratios of CR, i.e. r = [CR]/[protein dimer], we investigated the aggregation kinetics, conformation, hydrogen-deuterium exchange, and thermal stability of the protein. In addition, we used isothermal titration calorimetry to characterize the thermodynamics of CR binding to the protein. During incubation at 37 degrees C or during thermal scanning, with CR at r = 0.3, 1.3, and 4.8, protein aggregation was greatly accelerated compared with that measured in the absence of the dye. In contrast, with CR at r = 8.8, protein unfolding was favored over aggregation. The aggregates formed with CR at r = 0 or 0.3 were typical amyloid fibrils, but mixtures of amyloid fibrils and amorphous aggregates were formed at r = 1.3 and 4.8. CR decreased the apparent thermal unfolding temperature of the protein. Furthermore, CR perturbed the tertiary structure of the protein without significantly altering its secondary structure. Consistent with this result, CR also increased the rate of hydrogen-deuterium exchange by the protein. Isothermal titration calorimetry showed that CR binding to the protein was enthalpically driven, indicating that binding was mainly the result of electrostatic interactions. Overall, these results demonstrate that at low concentrations, CR binding to the protein favors a structurally perturbed, aggregation-competent species, resulting in acceleration of fibril formation. At high CR concentration, protein unfolding is favored over aggregation, and fibril formation is inhibited. Because low concentrations of CR can promote amyloid fibril formation, the therapeutic utility of this compound or its analogs to inhibit amyloidoses is questionable.

Time and spectral resolved phosphorescence of singlet oxygen and pigments in photosystem II particles

Singlet oxygen generated via chlorophyll triplets in photosynthetic systems can destroy basic components of photosynthetic apparatus. In order to study this process a sensitive spectroscopic experimental set-up was built to detect both weak infrared (IR) chlorophyll phosphorescence (between 900 and 1000nm) and singlet oxygen phosphorescence (at 1270nm). The spectral and time resolution of the used monochromator and photon counting multiscaler are sufficient to provide two-dimensional matrix of temporally and spectrally resolved IR luminescence data. We have studied IR emission of photosystem II particles in D2O and H2O buffer including the effect of the sodium dodecyl sulphate (SDS) detergent. Both sub-microsecond lifetime of chlorophyll triplet states and microsecond lifetime of singlet oxygen were determined. The singlet oxygen lifetime in D2O (of 18μs) was approximately five times longer than that in H2O. Quantum efficiency of singlet oxygen generation in photosystem II particles was significantly lower than that in chlorophyll a in acetone, however, it could be substantially increased by addition of SDS.

Non-oxidative decarboxylation of glycine derivatives by a peroxidase.

Under anaerobic, peroxide-free conditions (pH 5.5, 25 degrees C), horseradish peroxidase (HRP) catalyzes the rapid, non-oxidatve decarboxylation of N-alkyl-N-phenylglycine derivatives to the corresponding N-alkyl-N-methylanilines in 100% yield. When the reaction is conducted in D2O buffer, the product contains a single deuterium in the methyl group. The reactions are very fast compared to the oxidative decarboxylation of the same substrates under standard peroxidatic conditions (i.e., hydrogen peroxide added, air present) and in fact are inhibited by peroxide and oxygen. To account for these unprecedented observations, we propose a cyclic mechanism in which ferric HRP abstracts an electron from the substrate, giving an aminium ion intermediate that decarboxylates; protonation of the resulting alpha-aminoradical on carbon gives an aminium ion that is reduced by ferrous HRP to complete the cycle.

The Structural Basis of Compstatin Activity Examined by Structure-Function-based Design of Peptide Analogs and NMR

We have previously identified compstatin, a 13-residue cyclic peptide, that inhibits complement activation by binding to C3 and preventing C3 cleavage to C3a and C3b. The structure of compstatin consists of a disulfide bridge and a type I beta-turn located at opposite sides to each other. The disulfide bridge is part of a hydrophobic cluster, and the beta-turn is part of a polar surface. We present the design of compstatin analogs in which we have introduced a series of perturbations in key structural elements of their parent peptide, compstatin. We have examined the consistency of the structures of the designed analogs compared with compstatin using NMR, and we have used the resulting structural information to make structure-complement inhibitory activity correlations. We propose the following. 1) Even in the absence of the disulfide bridge, a linear analog has a propensity for structure formation consistent with a turn of a 3(10)-helix or a beta-turn. 2) The type I beta-turn is a necessary but not a sufficient condition for activity. 3) Our substitutions outside the type I beta-turn of compstatin have altered the turn population but not the turn structure. 4) Flexibility of the beta-turn is essential for activity. 5) The type I beta-turn introduces reversibility and sufficiently separates the two sides of the peptide, whereas the disulfide bridge prevents the termini from drifting apart, thus aiding in the formation of the hydrophobic cluster. 6) The hydrophobic cluster at the linked termini is involved in binding to C3 and activity but alone is not sufficient for activity. 7) beta-Turn residues Gln(5) (Asn(5))-Asp(6)-Trp(7)(Phe(7))-Gly(8) are specific for the turn formation, but only Gln(5)(Asn(5))-Asp(6)-Trp(7)-Gly(8) residues are specific for activity. 8) Trp(7) is likely to be involved in direct interaction with C3, possibly through the formation of a hydrogen bond. Finally we propose a binding model for the C3-compstatin complex.

Spectroscopic observation of intermediates formed during the oxidative half-reaction of copper/topa quinone-containing phenylethylamine oxidase.

The catalytic reaction of copper/topa quinone (TPQ) containing amine oxidase consists of the initial, well-characterized, reductive half-reaction and the following, less studied, oxidative half-reaction. We have analyzed the oxidative half-reaction catalyzed by phenylethylamine oxidase from Arthrobacter globiformis (AGAO) by rapid-scan stopped-flow measurements. Upon addition of dioxygen to the substrate-reduced AGAO at pH 8.2, the absorption bands derived from the semiquinone (TPQ(sq)) and aminoresorcinol forms of the TPQ cofactor disappeared within the dead time (<1 ms) of the measurements, indicating that the reaction of the substrate-reduced enzyme with dioxygen is very rapid. Concomitantly, an early intermediate exhibiting an absorption band at about 410 nm was formed, which then decayed with a rate constant of 390 +/- 50 s(-1). This intermediate was detected more prominently in the reaction in D2O buffer (pD 8.1) and was assigned to a Cu(II)-peroxy species. The assignment was based on the observation that addition of H2O2 to the substrate-reduced AGAO under anaerobic conditions led to the formation of a new band at about 415 nm, accompanied by partial quenching of absorption bands derived from TPQ(sq). Other intermediates exhibiting absorption bands at about 310 and 340 nm were also observed in the oxidative half-reaction. Kinetics of the disappearance of these latter bands did not correspond with that of the Cu(II)-peroxy band at 410 nm but did well with that of the increase of the 480 nm absorption band due to the reoxidized TPQ. Rapid increase of the absorption in the 320-370 nm region was also observed for the reaction of the substrate-reduced, Ni-substituted enzyme with dioxygen. On the basis of these results, a possible mechanism is proposed for the oxidative half-reaction of the bacterial copper amine oxidase.

Chromophore structure in lumirhodopsin and metarhodopsin I by time-resolved resonance Raman microchip spectroscopy.

Time-resolved resonance Raman microchip flow experiments have been performed on the lumirhodopsin (Lumi) and metarhodopsin I (Meta I) photointermediates of rhodopsin at room temperature to elucidate the structure of the chromophore in each species as well as changes in protein-chromophore interactions. Transient Raman spectra of Lumi and Meta I with delay times of 16 micros and 1 ms, respectively, are obtained by using a microprobe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to detect the scattering. The fingerprint modes of both species are very similar and characteristic of an all-trans chromophore. Lumi exhibits a relatively normal hydrogen-out-of-plane (HOOP) doublet at 951/959 cm(-1), while Meta I has a single HOOP band at 957 cm(-1). These results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation of the chromophore to a more planar all-trans conformation and the elimination of the structural perturbation that uncouples the 11H and 12H wags in bathorhodopsin. Surprisingly, the protonated Schiff base C=N stretching mode in Lumi (1638 cm(-1)) is unusually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down by only 7 cm(-1) in D2O buffer. This indicates that the Schiff base hydrogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition. However, the C=N stretching mode in Meta I is found at 1654 cm(-1) and exhibits a normal deuteration-induced downshift of 24 cm(-1), identical to that of the all-trans protonated Schiff base. The structural relaxation of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive the Schiff base group out of its hydrogen-bonded environment near Glu113, and the hydrogen bonding recovers to a normal solvated PSB value but presumably a different hydrogen bond acceptor with the formation of Meta I.

Interface Polymerization in a Polymer Micelle: An NMR Study of the Radical Polymerization of Methyl Methacrylate at the Core−Shell Interface of Polystyrene-block-poly(methacrylic acid) Micelles

Systems containing poly(styrene)-block-poly(methacrylic acid) micelles (1.67 g/L), methyl methacrylate (1.88−3.76 g/L), and initiator (polymerization) or inhibitor (pure solubilization) in D2O buffer solution were studied by 1H NMR. The proton NMR signals of MMA dissolved in the micellar system have the same chemical shifts as those in the corresponding D2O buffer solution but exhibit a characteristically broadened and asymmetric shape. Separate signals with different chemical shifts and signal shapes were observed for MMA absorbed into the poly(styrene) core. From the shape analysis of the signals of the water-dissolved MMA in the micellar system, it can be deduced that the monomer is almost exclusively accumulated near the core−shell interface. Its radial distribution can be approximated by a Gaussian function with the maximum at the core radius R and half-width b of 1.65R and 1.93R for the MMA concentrations 2 and 4 g/L, respectively. An increase in temperature from 295 to 330 K leads to a faster self-...

1H NMR studies on the CuA center of nitrous oxide reductase from Pseudomonas stutzeri.

1H NMR spectra of the CuA center of N2OR from Pseudomonas stutzeri, and a mutant enzyme that contains only CuA, were recorded in both H2O- and D2O-buffered solution at pH 7.5. Several sharp, well-resolved hyperfine-shifted 1H NMR signals were observed in the 60 to -10 ppm chemical shift range. Comparison of the native and mutant N2OR spectra recorded in H2O-buffered solutions indicated that several additional signals are present in the native protein spectrum. These signals are attributed to a dinuclear copperII center. At least two of the observed hyperfine-shifted signals associated with the dinuclear center, those at 23.0 and 13.2 ppm, are lost upon replacement of H2O buffer with D2O buffer. These data indicate that at least two histidine residues are ligands of a dinuclear CuII center. Comparison of the mutant N2OR 1H NMR spectra recorded in H2O and D2O indicates that three signals, c (27.5 ppm), e (23.6 ppm), and i (12.4 ppm), are solvent exchangeable. The two most strongly downfield-shifted signals (c and e) are assigned to the two N epsilon 2H (N-H) protons of the coordinated histidine residues, while the remaining exchangeable signal is assigned to a backbone N-H proton in close proximity to the CuA cluster. Signal e was found to decrease in intensity as the temperature was increased, indicating that proton e resides on a more solvent-exposed histidine residue. One-dimensional nOe studies at pH 7.5 allowed the histidine ring protons to be definitively assigned, while the remaining signals were assigned by comparison to previously reported spectra from CuA centers. The temperature dependence of the observed hyperfine-shifted 1H NMR signals of mutant N2OR were recorded over the temperature range of 276-315 K. Both Curie and anti-Curie temperature dependencies are observed for sets of hyperfine-shifted protons. Signals a and h (cysteine protons) follow anti-Curie behavior (contact shift increases with increasing temperatures), while signals b-g, i, and j (histidine protons) follow Curie behavior (contact shift decreases with increasing temperatures). Fits of the temperature dependence of the observed hyperfine-shifted signals provided the energy separation (Delta EL) between the ground (2B3u) and excited (2B2u) states. The temperature data obtained for all of the observed hyperfine-shifted histidine ligand protons provided a Delta EL value of 62 +/- 35 cm-1. The temperature dependence of the observed cysteine C beta H and C alpha H protons (a and h) were fit in a separate experiment providing a Delta EL value of 585 +/- 125 cm-1. The differences between the Delta EL values determined by 1H NMR spectroscopy and those determined by EPR or MCD likely arise from coupling between relatively low-frequency vibrational states and the ground and excited electronic states.

Electrochemical, FTIR, and UV/VIS spectroscopic properties of the ba(3) oxidase from Thermus thermophilus.

The ba3 cytochrome c oxidase from Thermus thermophilus has been studied with a combined electrochemical, UV/VIS, and FTIR spectroscopic approach. Oxidative electrochemical redox titrations yielded midpoint potentials of Em1= -0.02 +/- 0.01 V and Em2 = 0.16 +/- 0.04 V for heme b and Em1 = 0.13 +/- 0.04 V and Em2 = 0.22 +/- 0.03 V for heme a(3) (vs Ag/AgCl/3 M KCl). Fully reversible electrochemically induced UV/VIS and FTIR difference spectra were obtained for the full potential step from -0. 5 to 0.5 V as well as for the critical potential steps from -0.5 to 0.1 V (heme b is fully oxidized and heme a3 remains essentially reduced) and from 0.1 to 0.5 V (heme b remains oxidized and heme a3 becomes oxidized). The difference spectra thus allow to us distinguish modes coupled to heme b and heme a3. Analogous difference spectra were obtained for the enzyme in D2O buffer for additional assignments. The FTIR difference spectra reveal the reorganization of the polypeptide backbone, perturbations of single amino acids and of hemes b and a3 upon electron transfer to/from the four redox-active centers heme b and a3, as well as CuB and CuA. Proton transfer coupled to redox transitions can be expected to manifest in the spectra. Tentative assignments of heme vibrational modes, of individual amino acids, and of secondary structure elements are presented. Aspects of the uncommon electrochemical and spectroscopic properties of the ba3 oxidase from T. thermophilus are discussed.

Stabilization of tubulin by deuterium oxide.

Tubulin is an unstable protein when stored in solution and loses its ability to form microtubules rapidly. We have found that D2O stabilizes the protein against inactivation at both 4 and 37 degrees C. In H2O-based buffer, tubulin was completely inactivated after 40 h at 4 degrees C, but in buffer prepared in D2O, no activity was lost after 54 h. Tubulin was completely inactivated at 37 degrees C in 8 h in H2O buffer, but only 20% of the activity was lost in D2O buffer. Tubulin also lost its colchicine binding activity at a slower rate in D2O. The deuterated solvent retarded an aggregation process that occurs during incubation at both temperatures. Inactivation in H2O buffer was partially reversed by transferring the protein to D2O buffer; however, aggregation was not reversed. The level of binding of BisANS, a probe of exposed hydrophobic sites in proteins, increases during the inactivation of tubulin. In D2O, the rate of this increase is slowed somewhat. We propose that D2O has its stabilizing effect on a conformational step or steps that involve the disruption of hydrophobic forces. The conformational change is followed by an aggregation process that cannot be reversed by D2O. As reported previously [Ito, T., and Sato, H. (1984) Biochim. Biophys. Acta 800, 21-27], we found that D2O stimulates the formation of microtubules from tubulin. We also observed that the products of assembly in D2O/8% DMSO consisted of a high percentage of ribbon structures and incompletely folded microtubules. When these polymers were disassembled and reassembled in H2O/8% DMSO, the products were microtubules. We suggest that the combination of D2O and DMSO, both stimulators of tubulin assembly, leads to the rapid production of nuclei that lead to the formation of ribbon structures rather than microtubules.

Photoconversion of a Water-Soluble Chlorophyll Protein from Chenopodium Album: Resonance Raman and Fourier Transform Infrared Study of Protein and Pigment Structures

A water-soluble Chl a/b-protein complex, CP668, from Chenopodium album converts to another form of protein complex, CP743, upon light illumination. Structural changes of pigments and proteins upon photoconversion were studied using resonance Raman (RR) and Fourier transform infrared (FTIR) spectroscopies. RR spectra of CP668 and CP743 and a light-induced FTIR difference spectrum showed that the macrocyle C=C bands of Chl a in CP668 considerably changed upon conversion to the pigment (not chemically identified yet) in CP743. The C=C band pattern of the RR spectrum of CP743 was similar to that of bacteriochlorophyll a, suggesting that the conjugated system of the CP743 pigment resembles a bacteriochlorin ring. Judging from the C=O frequencies, the 131-keto C=O groups of Chl a and b in CP668 are free from hydrogen bonding, whereas the 132-ester C=O groups of both Chl a and b and the 7-formyl C=O of Chl b in CP668 are hydrogen bonded. Upon conversion to CP743, interactions of the 131-keto and 132-ester C=O groups were basically unaffected, demonstrating no drastic changes around these C=O groups. FTIR spectra in the amide I' region of CP668 and CP743 in D2O buffer showed a peak at 1,633 cm−1, which represents a major component of β-sheet conformation. Second-derivative spectra of the amide I' bands as well as a light-induced FTIR difference spectrum suggested that drastic change in the protein conformation does not occur upon photoconversion.

Pressure-induced structural rearrangements of bovine pancreatic trypsin inhibitor studied by FTIR spectroscopy.

Fourier transform infrared (FTIR) spectroscopy combined with resolution enhancement techniques, second-derivative and difference spectroscopies, have been used to characterize pressure-induced changes in the structural rearrangements of bovine pancreatic trypsin inhibitor (BPTI) in D2O solution at 25.0 degrees C. According to the observed changes in the amide I' band up to 550 MPa, the secondary structure elements of BPTI, such as the alpha-helix, 3(10)-helix, beta-sheet, and beta-turn, are scarcely rearranged except for the loop structure of residues of 9-17 and 36-43. The polypeptide backbone is not extensively unfolded up to 550 MPa. The minor pressure-induced structural rearrangements are completely reversible. A further increase in pressure above 1000 MPa associated with the precipitation of BPTI in D2O buffer solution induces the partial structural rearrangements of the alpha-helix, beta-turn and/or 3(10)-helix, and beta-sheet. The polypeptide backbone of BPTI is not fully unfolded even above 1000 MPa. Most of the protected backbone amide protons involved in the beta-sheet remain intact in the pressure range where BPTI is not precipitated, while those involved in the alpha-helix and beta-turn and/or 3(10)-helix are exchanged with solvent deuterons. The protected backbone amide protons located near the surface regions are more easily exchanged with solvent deuterons by application of high pressure than those involved in the core.

Topology of sarcoplasmic reticulum Ca2+-ATPase: an infrared study of thermal denaturation and limited proteolysis.

Sarcoplasmic reticulum Ca2+-ATPase structure and organization in the membrane has been studied by infrared spectroscopy by decomposition of the amide I band. Besides the component bands assignable to secondary structure elements such as alpha-helix, beta-sheet, etc...., two unusual bands, one at 1,645 cm(-1) in H2O buffer and the other at 1,625 cm(-1) in D2O buffer are present. By perturbing the protein using temperature and limited proteolysis, the band at 1,645 cm(-1) is tentatively assigned to alpha-helical segments located in the cytoplasmic domain and coupled to beta-sheet structure, whereas the band at 1,625 cm(-1) arises probably from monomer-monomer contacts in the native oligomeric protein. The secondary structure obtained is 33% alpha-helical segments in the transmembrane plus stalk domain; 20% alpha-helix and 22% beta-sheet in the cytoplasmic domain plus 19% turns and 6% unordered structure. Thermal unfolding of Ca2+-ATPase is a complex process that cannot be described as a two-state denaturation. The results obtained are compatible with the idea that the protein is an oligomer at room temperature. The loss of the 1,625 cm(-1) band upon heating would be consistent with a disruption of the oligomers in a process that later gives rise to aggregates (appearance of the 1,618 cm(-1) band). This picture would also be compatible with early results suggesting that processes governing Ca2+ accumulation and ATPase activity are uncoupled at temperatures above 37 degrees C, so that while ATPase activity proceeds at high rates, Ca2+ accumulation is inhibited.

The polymerization of actin: Study by small angle neutron scattering

We report measurements of small angle neutron scattering from solutions of rabbit muscle G-actin at 3.00 mg/mL in D2O buffer solution, with [Ca2+]=0.52 mM and with [KCl]=15, 8.9, and 5.4 mM. We observe the onset of the polymerization of G-actin to F-actin as the temperature is increased. The polymerization takes place on a time scale of 30–45 min for each temperature jump of 2 °C–3 °C. As the temperature is increased further, the average size of the polymers increases, and the characteristic length scale (or correlation length), ξ, of the F-actin in the dilute solution grows: ξ is about 10 Å below Tp, and about 70 Å a few degrees above Tp. The transition is sharper for lower concentrations of KCl. For the sample with [KCl]=8.9 mM, we observe a peak in ξ at about 2 °C above Tp, which indicates a crossover into the semidilute regime. The transition is essentially reversible, but shows evidence of incomplete depolymerization on cycling. We are unable to apply the available theoretical model for reversible polymerization to rabbit muscle actin because of a lack of information on the enthalpy and entropy of polymerization. However, our observations for rabbit muscle actin are quite analogous to observations on the equilibrium polymerization of α-methylstyrene [A. P. Andrews, K. P. Andrews, S. C. Greer, F. Boué, and P. Pfeuty, Macromolecules 27, 3902 (1994)].

Pressure‐induced structural rearrangements of bovine pancreatic trypsin inhibitor studied by FTIR spectroscopy

Fourier transform infrared (FTIR) spectroscopy combined with resolution enhancement techniques, second-derivative and difference spectroscopies, have been used to characterize pressure-induced changes in the structural rearrangements of bovine pancreatic trypsin inhibitor (BPTI) in D2O solution at 25.0°C. According to the observed changes in the amide I′ band up to 550 MPa, the secondary structure elements of BPTI, such as the α-helix, 310-helix, β-sheet, and β-turn, are scarcely rearranged except for the loop structure of residues of 9–17 and 36–43. The polypeptide backbone is not extensively unfolded up to 550 MPa. The minor pressure-induced structural rearrangements are completely reversible. A further increase in pressure above 1000 MPa associated with the precipitation of BPTI in D2O buffer solution induces the partial structural rearrangements of the α-helix, β-turn and/or 310-helix, and β-sheet. The polypeptide backbone of BPTI is not fully unfolded even above 1000 MPa. Most of the protected backbone amide protons involved in the β-sheet remain intact in the pressure range where BPTI is not precipitated, while those involved in the α-helix and β-turn and/or 310-helix are exchanged with solvent deuterons. The protected backbone amide protons located near the surface regions are more easily exchanged with solvent deuterons by application of high pressure than those involved in the core. © 1998 John Wiley & Sons, Inc. Biospectroscopy 4: 209–216, 1998

Pressure-induced structural rearrangements of bovine pancreatic trypsin inhibitor studied by FTIR spectroscopy

Fourier transform infrared (FTIR) spectroscopy combined with resolution enhancement techniques, second-derivative and difference spectroscopies, have been used to characterize pressure-induced changes in the structural rearrangements of bovine pancreatic trypsin inhibitor (BPTI) in D2O solution at 25.0°C. According to the observed changes in the amide I′ band up to 550 MPa, the secondary structure elements of BPTI, such as the α-helix, 310-helix, β-sheet, and β-turn, are scarcely rearranged except for the loop structure of residues of 9–17 and 36–43. The polypeptide backbone is not extensively unfolded up to 550 MPa. The minor pressure-induced structural rearrangements are completely reversible. A further increase in pressure above 1000 MPa associated with the precipitation of BPTI in D2O buffer solution induces the partial structural rearrangements of the α-helix, β-turn and/or 310-helix, and β-sheet. The polypeptide backbone of BPTI is not fully unfolded even above 1000 MPa. Most of the protected backbone amide protons involved in the β-sheet remain intact in the pressure range where BPTI is not precipitated, while those involved in the α-helix and β-turn and/or 310-helix are exchanged with solvent deuterons. The protected backbone amide protons located near the surface regions are more easily exchanged with solvent deuterons by application of high pressure than those involved in the core. © 1998 John Wiley & Sons, Inc. Biospectroscopy 4: 209–216, 1998

Hydrogen bond stabilities in membrane-reconstituted alamethicin from amide-resolved hydrogen-exchange measurements

Amide-resolved hydrogen-deuterium exchange-rate constants were measured for backbone amides of alamethicin reconstituted in dioleoylphosphatidylcholine vesicles by an exchange-trapping method combined with high-resolution nuclear magnetic resonance spectroscopy. In vesicles containing alamethicin at molar ratios between 1:20 and 1:100 relative to lipid, the exchange-rate constants increased with increasing volume of the D20 buffer in which the vesicles were suspended, indicating that exchange under these conditions is dominated by partitioning of the peptide into the aqueous phase. This was supported by observation of a linear relationship between the exchange-rate constants for amides in membrane-reconstituted alamethicin and those for amides in alamethicin dissolved directly into D2O buffer. Significant protection of amides from exchange with D2O buffer in membrane-reconstituted alamethicin is interpreted in terms of stabilization by helical hydrogen bonding. Under conditions in which amide exchange occurred by partitioning of the peptide into solution, only lower limits for hydrogen-bond stabilities in the membrane were determined; all the potentially hydrogen-bonded amides of alamethicin are at least 1000-fold exchange protected in the membrane-bound state. When partitioning of alamethicin into the aqueous phase was suppressed by hydration of reconstituted vesicles in a limiting volume of water [D2O:dioleoylphosphatidylcholine:alamethicin; 220:1:0.05; (M:M:M)], the exchange-protection factors exhibited helical periodicity with highly exchange-protected, and less well-protected, amides on the nonpolar and polar helix faces, respectively. The exchange data indicate that, under the conditions studied, alamethicin adopts a stable helical structure in DOPC bilayers in which all the potentially hydrogen-bonded amides are stabilized by helical hydrogen bonds. The protection factors define the orientation of the peptide helix with respect to an aqueous phase, which is either the bulk solution or water within parallel or antiparallel transmembrane arrays of reconstituted alamethicin.