Alpha-helix Dipole Research Articles

Crystal structure of a bacterial homologue of the kidney urea transporter

Urea is highly concentrated in the mammalian kidney to produce the osmotic gradient necessary for water re-absorption. Free diffusion of urea across cell membranes is slow owing to its high polarity, and specialized urea transporters have evolved to achieve rapid and selective urea permeation. Here we present the 2.3 A structure of a functional urea transporter from the bacterium Desulfovibrio vulgaris. The transporter is a homotrimer, and each subunit contains a continuous membrane-spanning pore formed by the two homologous halves of the protein. The pore contains a constricted selectivity filter that can accommodate several dehydrated urea molecules in single file. Backbone and side-chain oxygen atoms provide continuous coordination of urea as it progresses through the filter, and well-placed alpha-helix dipoles provide further compensation for dehydration energy. These results establish that the urea transporter operates by a channel-like mechanism and reveal the physical and chemical basis of urea selectivity.

Structures of yeast glutathione‐S‐transferase Gtt2 reveal a new catalytic type of GST family

Glutathione-S-transferases (GSTs) are ubiquitous detoxification enzymes that catalyse the conjugation of electrophilic substrates to glutathione. Here, we present the crystal structures of Gtt2, a GST of Saccharomyces cerevisiae, in apo and two ligand-bound forms, at 2.23 A, 2.20 A and 2.10 A, respectively. Although Gtt2 has the overall structure of a GST, the absence of the classic catalytic essential residues--tyrosine, serine and cysteine--distinguishes it from all other cytosolic GSTs of known structure. Site-directed mutagenesis in combination with activity assays showed that instead of the classic catalytic residues, a water molecule stabilized by Ser129 and His123 acts as the deprotonator of the glutathione sulphur atom. Furthermore, only glycine and alanine are allowed at the amino-terminus of helix-alpha1 because of stereo-hindrance. Taken together, these results show that yeast Gtt2 is a novel atypical type of cytosolic GST.

How Proteins Come Together in the Plasma Membrane and Function in Macromolecular Assemblies: Focus on Receptor Mosaics

Some theoretical aspects on structure and function of proteins have been discussed previously. Proteins form multimeric complexes, as they have the capability of binding other proteins (Lego property) resulting in multimeric complexes capable of emergent functions. Multimeric proteins might have either a genomic or a postgenomic origin. Proteins spanning the plasma membrane have been analyzed by considering the effects of the microenvironment in which the protein is embedded. In particular, the different effects of the hydrophilic (extracellular and intracellular) versus the lipophilic (intramembrane) environment have been considered. These aspects have been discussed in the framework of membrane microdomains, in particular, the so-called rafts. In alpha-helix proteins the individual peptide dipoles align to produce a macrodipole crossing the entire membrane. This macrodipole has its positive (extracellular) pole at the N-terminal end of the helix and its negative (intracellular) pole at the C-terminal end. This arrangement has been analyzed in the framework of the counter-ion atmosphere, that is, the formation of a cloud of small ions bearing an opposite charge. Excitable cells reverse their resting potential during the all-or-none action potentials. Hence, the extracellular side of the plasma membrane becomes negative with respect to the intracellular side. This change of polarization affects also the direction and magnitude of the alpha-helix dipole in view of the fact that there is a displacement of the counter ions. The oscillation in the intensity of the dipole caused by the action potentials opens the possibility of an interaction among dipoles by electromagnetic waves.

Atomic resolution density maps reveal secondary structure dependent differences in electronic distribution.

The X-ray crystal structure of the flavoenzyme cholesterol oxidase, SCOA (Streptomyces sp.SA-COO) has been determined to 0.95 A resolution. The large size (55kDa) and the high-resolution diffraction of this protein provides a unique opportunity to observe detailed electronic effects within a protein environment and to obtain a larger sampling for which to analyze these electronic and structural differences. It is well-known through spectroscopic methods that peptide carbonyl groups are polarized in alpha-helices. This electronic characteristic is evident in the sub-Angstrom electron density of SCOA. Our analysis indicates an increased tendency for the electron density of the main chain carbonyl groups within alpha-helices to be polarized toward the oxygen atoms. In contrast, the carbonyl groups in beta-sheet structures tend to exhibit a greater charge density between the carbon and oxygen atoms. Interestingly, the electronic differences observed at the carbonyl groups do not appear to be correlated to the bond distance of the peptide bond or the peptide planarity. This study gives important insight into the electronic effects of alpha-helix dipoles in enzymes and provides experimentally based observations that have not been previously characterized in protein structure.

X-ray structure of a ClC chloride channel at 3.0 A reveals the molecular basis of anion selectivity.

The ClC chloride channels catalyse the selective flow of Cl- ions across cell membranes, thereby regulating electrical excitation in skeletal muscle and the flow of salt and water across epithelial barriers. Genetic defects in ClC Cl- channels underlie several familial muscle and kidney diseases. Here we present the X-ray structures of two prokaryotic ClC Cl- channels from Salmonella enterica serovar typhimurium and Escherichia coli at 3.0 and 3.5 A, respectively. Both structures reveal two identical pores, each pore being formed by a separate subunit contained within a homodimeric membrane protein. Individual subunits are composed of two roughly repeated halves that span the membrane with opposite orientations. This antiparallel architecture defines a selectivity filter in which a Cl- ion is stabilized by electrostatic interactions with alpha-helix dipoles and by chemical coordination with nitrogen atoms and hydroxyl groups. These findings provide a structural basis for further understanding the function of ClC Cl- channels, and establish the physical and chemical basis of their anion selectivity.

Electric fields in active sites: substrate switching from null to strong fields in thiol- and selenol-subtilisins.

Although known to be important factors in promoting catalysis, electric field effects in enzyme active sites are difficult to characterize from an experimental standpoint. Among optical probes of electric fields, Raman spectroscopy has the advantage of being able to distinguish electronic ground-state and excited-state effects. Earlier Raman studies on acyl derivatives of cysteine proteases [Doran, J. D., and Carey, P. R. (1996) Biochemistry 35, 12495-502], where the acyl group has extensive pi-electron conjugation, showed that electric field effects in the active site manifest themselves by polarizing the pi-electrons of the acyl group. Polarization gives rise to large shifts in certain Raman bands, e.g. , the C=C stretching band of the alpha,beta-unsaturated acyl group, and a large red shift in the absorption maximum. It was postulated that a major source of polarization is the alpha-helix dipole that originates from the alpha-helix terminating at the active-site cysteine of the cysteine protease family. In contrast, using the acyl group 5-methylthiophene acryloyl (5-MTA) as an active-site Raman probe, acyl enzymes of thiol- or selenol-subtilisin exhibit no polarization even though the acylating amino acid is at the terminus of an alpha-helix. Quantum mechanical calculations on 5-MTA ethyl thiol and selenol ethyl esters allowed us to identify the conformational states of these molecules along with their corresponding vibrational signatures. The Raman spectra of 5-MTA thiol and selenol subtilisins both showed that the acyl group binds in a single conformation in the active site that is s-trans about the =C-C=O single bond. Moreover, the positions of the C=C stretching bands show that the acyl group is not experiencing polarization. However, the release of steric constraints in the active site by mutagenesis, by creating the N155G form of selenol-subtilisin and the P225A form of thiol-subtilisin, results in the appearance of a second conformer in the active sites that is s-cis about the =C-C=O bond. The Raman signature of this second conformer indicates that it is strongly polarized with a permanent dipole being set up through the acyl group's pi-electron chain. Molecular modeling for 5-MTA in the active sites of selenol-subtilisin and N155G selenol-subtilisin confirms the findings from Raman spectroscopic studies and identifies the active-site features that give rise to polarization. The determinants of polarization appear to be strong electron pull at the acyl carbonyl group by a combination of hydrogen bonds and the field at the N-terminus of the alpha-helix and electron push from a negatively charged group placed at the opposite end of the chromophore.

Raman study of the polarizing forces promoting catalysis in 4-chlorobenzoate-CoA dehalogenase.

The enzyme 4-chlorobenzoate-CoA dehalogenase catalyzes the hydrolysis of 4-chlorobenzoate-CoA (4-CBA-CoA) to 4-hydroxybenzoyl-CoA (4-HBA-CoA). In order to facilitate electrophilic catalysis, the dehalogenase utilizes a strong polarizing interaction between the active site residues and the benzoyl portion of the substrate [Taylor, K. L., et al. (1995) Biochemistry 34, 13881]. As a result of this interaction, the normal modes of the benzoyl moiety of the bound 4-HBA-CoA undergo a drastic rearrangement as shown by Raman spectroscopy. Here, we present Raman difference spectroscopic data on the product-enzyme complex where the product's benzoyl carbonyl is labeled with 18O (C=18O) or 13C (13C=O) or where the 4-OH group is labeled with 18O. The data demonstrate that the carbonyl group participates in the most intense normal modes occurring in the Raman spectrum in the 1520-1560 cm-1 region. The substrate analog 4-methylbenzoate-CoA (4-MeBA-CoA) has also been characterized by Raman difference spectroscopy in its free form and bound to the dehalogenase. Upon binding, the 4-MeBA-CoA shows evidence of polarization within the delocalized pi-electrons, but to a lesser extent compared to that seen for the product. The use of 4-MeBA-CoA labeled with 18O at the carbonyl enables us to estimate the degree of electron polarization within the C=O group of the bound 4-MeBA-CoA. The C=O stretching frequency occurs near 1663 cm-1 in non-hydrogen bonding solvents such as CCl4, near 1650 cm-1 in aqueous solution, and near 1610 cm-1 in the active site of dehalogenase. From model studies, we can estimate that in the active site the carbonyl group behaves as though it is being polarized by hydrogen bonds approximately 57 kJ mol-1 in strength. Major contributions to this polarization come from hydrogen bonds from the peptide NHs of Gly114 and Phe64. However, an additional contribution, which may account for up to half of the observed shift in nuC=O, originates in the electrostatic field due to the alpha-helix dipole from residues 121-114. The helix which terminates at Gly114, near the C=O group of the bound benzoyl, provides a dipolar electrostatic component which contributes to the polarization of the C=O bond and to the polarization of the entire benzoyl moiety. The effect of both the helix dipole and the hydrogen bonds on the C=O is a "pull" of electrons onto the carbonyl oxygen, which, in turn, polarizes the electron distribution within the benzoyl pi-electron system. The ability of these two factors to polarize the electrons within the benzoyl moiety is increased by the environment about the benzoyl ring; it is surrounded by hydrophobic residues which provide a low-dielectric constant microenvironment. Electron polarization promotes catalysis by reducing electron density at the C4 position of the benzoyl ring, thereby assisting attack by the side chain of Asp145. An FTIR study on the model compound 4-methylbenzoyl S-ethyl thioester, binding to a number of hydrogen bonding donors in CCl4, is described and is used to relate the observed shift of the C=O stretching mode of 4-MeBA-CoA in the active site to the hydrogen bonding strength value. Since the shift of the C=O frequency upon binding is due to hydrogen bonding and helix dipole effects, we refer to this bonding strength as the effective hydrogen bonding strength.

Three-dimensional structure of porcine kidney D-amino acid oxidase at 3.0 A resolution.

The X-ray crystallographic structure of porcine kidney D-amino acid oxidase, which had been expressed in Escherichia coli transformed with a vector containing DAO cDNA, was determined by the isomorphous replacement method for the complex form with benzoate. The known amino acid sequence, FAD and benzoate were fitted to an electron density map of 3.0 A resolution with an R-factor of 21.0%. The overall dimeric structure exhibits an elongated ellipsoidal framework. The prosthetic group, FAD, was found to be in an extended conformation, the isoalloxazine ring being buried in the protein core. The ADP moiety of FAD was located in the typical beta alpha beta dinucleotide binding motif, with the alpha-helix dipole stabilizing the pyrophosphate negative charge. The substrate analog, benzoate, is located on the re-face of the isoalloxazine ring, while the si-face is blocked by hydrophobic residues. The carboxylate group of benzoate is ion-paired with the Arg283 side chain and is within interacting distance with the hydroxy moiety of Tyr228. The phenol ring of Tyr224 is located just above the benzene ring of benzoate, implying the importance of this residue for catalysis. There is no positive charge or alpha-helix dipole near N(1) of flavin. Hydrogen bonds were observed at C(2) = O, N(3)-H, C(4) = O, and N(5) of the flavin ring.

Alpha-helix dipoles and catalysis: absorption and Raman spectroscopic studies of acyl cysteine proteases.

Raman and absorption spectroscopic data are combined with the deacylation rate constants for a series of acyl cysteine proteases to provide insight into the role of alpha-helix dipoles in rate acceleration. The Raman spectra, obtained by Raman difference spectroscopy, of (5-methylthienyl)acryloyl adducts with papain, cathepsins B and L, and two oxyanion hole mutants of cathepsin B (Q23S and Q23A) show that extensive polarization throughout the pai-electron chain occurs for the bound acyl group in the active sites. A similar result is obtained using the specific chromophoric substrate ethyl 2-[(N-acetyl-L-phenylalanyl)amino]-3-(5-methylthienyl)acrylate. By using 13C = O substitution it is possible to detect the acyl C = O stretching frequency, vC = O, for each acyl enzyme. A correlation between vC = O and log k3, where k3 is the deacylation rate constant, is found where vC = O increases with increasing reactivity. This is exactly the opposite sense to the relationship found for a series of acyl serine proteases [Carey & Tonge (1995) Acc. Chem. Res. 28, 8]. The opposite trend in the direction of the correlation for the acyl cysteine proteases is ascribed to the strong electron polarizing forces in the active site, due principally to the active-site alpha-helix dipole, giving rise to canonical (valence bond) forms of the acyl group which change the hybridization about the C = O carbon atom. A correlation is also observed between the absorption maximum, lambda max, and log k3 for each acyl cysteine protease. As the deacylation rate increases, 214-fold across the series, lambda max red-shifts from 367 to 384 nm. It is proposed that differential interactions between the active site's alpha-helix dipole and the acyl chromophore give rise to the observed changes in lambda max, with the red shift being caused principally by interactions with the excited electronic state, which has a high degree of charge separation, and the dipole. Similar interactions between the dipole and the negatively charged tetrahedral intermediate, which resembles the transition state, are proposed as the source of differential rates in deacylation. It is interesting to note that similar energies are operating in both cases. A shift in lambda max from 367 to 384 nm corresponds to a change in electronic absorption transition energies of 3.2 kcal/mol and a change of deacylation rate constants of 214-fold also corresponds to a change of activation energies of 3.2 kcal/mol.

Determinants of protein thermostability observed in the 1.9-.ANG. crystal structure of malate dehydrogenase from the thermophilic bacterium Thermus flavus

A binary complex of malate dehydrogenase from the thermophilic bacterium Thermus flavus (tMDH) with NADH has been crystallized from poly(ethylene glycol) 3500, pH 8.5, yielding diffraction-quality crystals in space group P2(1)2(1)2(1). The structure was solved at 1.9-A resolution using molecular replacement and refined to an R factor of 15.8% with good geometry. The primary sequence of tMDH is 55% identical to that of cytoplasmic malate dehydrogenase (cMDH) [Birktoft, J. J., Rhodes, G., & Banaszak, L. J. (1989) Biochemistry 28, 6065-6081], and overall their three-dimensional structures are very similar. Like cMDH, tMDH crystallized as a dimer with one coenzyme bound per subunit. The coenzyme binds in the extended conformation, and most of the interactions with enzyme are similar to those in cMDH. In tMDH, small local conformational changes are caused by the replacement of a glutamic acid for the aspartic acid involved in hydrogen bonding to the adenine ribose of NADH. Comparison of tMDH with cMDH reveals that both tMDH subunits more closely resemble the B subunit of cMDH which therefore is the more likely representative of the solution conformation. While cMDH is inactivated at temperatures above about 50 degrees C, tMDH is fully active at 90 degrees C. On the basis of the X-ray crystal structure, a number of factors have been identified which are likely to contribute to the relative thermostability of tMDH compared to cMDH. The most striking of the differences involves the introduction of four ion pairs per monomer. All of these ion pairs are solvent-accessible. Three of these ion pairs are located in the dimer interface, Glu27-Lys31, Glu57-Lys168, and Glu57-Arg229, and one ion pair, Glu275-Arg149, is at the domain interface within each subunit. Additionally, we observe incorporation of additional alanines into alpha-helices of tMDH and, in one instance, incorporation of an aspartate that functions as a counterchange to an alpha-helix dipole. The possible contributions of these and other factors to protein thermostability in tMDH are discussed.

Histidine residues at the N- and C-termini of alpha-helices: perturbed pKas and protein stability.

A single histidine residue has been placed at either the N-terminus or the C-terminus of each of the two alpha-helices of barnase. The pKa of that histidine residue in each of the four mutants has been determined by 1H NMR. The pKas of the two residues at the C-terminus are, on average, 0.5 unit higher, and those of the residues at the N-terminus are 0.8 unit lower, than the pKa of histidines in unfolded barnase at low ionic strength. The conformational stability of the mutant proteins at different values of pH has been measured by urea denaturation. C-Terminal histidine mutants are approximately 0.6 kcal mol-1 more stable when the introduced histidine is protonated, both at low and high ionic strength. N-Terminal mutants with a protonated histidine residue are approximately 1.1 kcal mol-1 less stable at low ionic strength and 0.5 kcal mol-1 less stable at high ionic strength (1 M NaCl). The low-field 1H NMR spectra of the mutant proteins at low pH suggest that the C-terminal histidines form hydrogen bonds with the protein while the N-terminal histidines do not form the same. The perturbations of pKa and stability result from a combination of different electrostatic environments and hydrogen-bonding patterns at either ends of helices. The value of 0.6 kcal mol-1 represents a lower limit to the favorable electrostatic interaction between the alpha-helix dipole and a protonated histidine residue at the C-terminal end of the helix.(ABSTRACT TRUNCATED AT 250 WORDS)

Proline residues in transmembrane helices of channel and transport proteins: a molecular modelling study.

Proline residues are commonly found in putative transbilayer helices of many integral membrane proteins which act as transporters, channels and receptors. Intramembranous prolines are often conserved between homologous proteins. It has been suggested that such intrahelical prolines provide liganding sites for cations via exposure of the backbone carbonyl oxygen atoms of residues i-3 and i-4 (relative to the proline). Molecular modelling studies have been carried out to evaluate this proposal. Bundles of parallel proline-kinked helices are considered as simplified models of ion channels. The energetics of K+ ion-helix bundle interactions are explored. It is shown that carbonyl oxygens exposed by the proline-induced kink and at the C-terminus of the helices may provide cation-liganding sites. 'Hybrid' bundles of antiparallel helices, only some of which contain proline residues, are considered as models of transport proteins. Again, proline-exposed carbonyl oxygens are shown to be capable of liganding cations. The roles of alpha-helix dipoles and of the geometry of helix packing are considered in relation to cation-bundle interactions. Implications with respect to modelling of ion channel and transport proteins are discussed.

Analysis of the interaction between charged side chains and the .alpha.-helix dipole using designed thermostable mutants of phage T4 lysozyme

It was shown previously that the introduction of a negatively charged amino acid at the N-terminus of an alpha-helix could increase the thermostability of phage T4 lysozyme via an electrostatic interaction with the "helix dipole" [Nicholson, H., Becktel, W. J., & Matthews, B. W. (1988) Nature 336, 651-656]. The prior report focused on the two stabilizing substitutions Ser 38----Asp (S38D) and Asn 144----Asp (N144D). Two additional examples of stabilizing mutants, T109D and N116D, are presented here. Both show the pH-dependent increase in thermal stability expected for the interaction of an aspartic acid with an alpha-helix dipole. Control mutants were also constructed to further characterize the nature of the interaction with the alpha-helix dipole. High-resolution crystal structure analysis was used to determine the nature of the interaction of the substituted amino acids with the end of the alpha-helix in both the primary and the control mutants. Control mutant S38N has stability essentially the same as that of wild-type lysozyme but hydrogen bonding similar to that of the stabilizing mutant S38D. This confirms that it is the electrostatic interaction between Asp 38 and the helix dipole, rather than a change in hydrogen-bonding geometry, that gives enhanced stability. Structural and thermodynamic analysis of mutant T109N provide a similar control for the stabilizing replacement T109D. In the case of mutant N116D, there was concern that the enhanced stability might be due to a favorable salt-bridge interaction between the introduced aspartate and Arg 119, rather than an interaction with the alpha-helix dipole. The additivity of the stabilities of N116D and R119M seen in the double mutant N116D/R119M indicates that favorable interactions are largely independent of residue 119. As a further control, Asp 92, a presumed helix-stabilizing residue in wild-type lysozyme, was replaced with Asn. This decreased the stability of the protein in the manner expected for the loss of a favorable helix dipole interaction. In total, five mutations have been identified that increase the thermostability of T4 lysozyme and appear to do so by favorable interactions with alpha-helix dipoles. As measured by the pH dependence of stability, the strength of the electrostatic interaction between the charged groups studied here and the helix dipole ranges from 0.6 to 1.3 kcal/mol in 150 mM KCl. In the case of mutants S38D and N144H, NMR titration was used to measure the pKa's of Asp 38 and His 144 in the folded structures.(ABSTRACT TRUNCATED AT 400 WORDS)

Comparison of alpha-helix stability in peptides having a negatively or positively charged residue block attached either to the N- or C-terminus of an alpha-helix: the electrostatic contribution and anisotropic stability of the alpha-helix.

An estimation of the thermodynamic effects of a charged random coil, which is attached either to the N- or C-terminus of polyalanine, upon alpha-helix stability is attempted. A temperature-induced helix-coil transition of Ala20Lys20Phe and Lys20Ala20Phe was studied under various conditions of salt concentration and pH. By combining the results with previous ones for Ala20Glu20Phe and Glu20Ala20Phe, which have opposite electric charges to the present system [S. Ihara et al. (1982) Biopolymers 21, 131-145], the free energy of the coil to helix transition of the polyalanine block could be separated into two terms--one term for the electrostatic interaction of electric charges in the random-coil block with the alpha-helix dipole, and a second term for the intrinsic stability of the helix. The first term indicates the significance of the helix dipole-charge interactions, which affects the helix stability depending on the attaching side of the charged block and on the sign of the charges. This clearly shows the anisotropic stability of the alpha-helix. Furthermore, analysis of the dependence of these thermodynamic quantities on salt concentrations showed, assuming that the effect of the attached electric charges was symmetric (in other words, the absolute values of the electrostatic interaction terms were independent of the sign of electric charges), that the intrinsic stability of the alpha-helix was dependent on which side of the helix was attached to the random coil: a random coil attached to the N-terminus of the alpha-helix had little effect while that attached to a C-terminal significantly destabilized the helix.

Enhanced protein thermostability from designed mutations that interact with alpha-helix dipoles.

Two different genetically engineered amino-acid substitutions designed to interact with alpha-helix dipoles in T4 lysozyme are shown to increase the thermal stability of the protein. Crystallographic analyses of the mutant lysozyme structures suggest that the stabilization is due to electrostatic interaction and does not require precise hydrogen bonding between the substituted amino acid and the end of the alpha-helix.

Electrostatic potentials of the alpha helix dipole and of elastase

Molecular graphics has been used to display the electrostatic potentials of the α-helix dipole and that of elastase calculated using atomic charges obtained by a new, simple method 1–3. Calculations on the α-helix dipole support the simple dipole model in which the helix is represented by single, half integral charges at the helix termini. The potentials of elastase show some interesting features which may be related to the binding processes.

Alpha-Helix dipole model and electrostatic stabilization of 4-alpha-helical proteins.

A simple dipole model is developed for estimation of the electrostatic interaction energy between alpha-helices in proteins. This model is used to estimate the electrostatic stabilization in a recurrent protein tertiary structural motif, an array of four closely packed alpha-helices. It is found that, for the proteins examined (cytochrome c', hemerythrin, myohemerythrin, cytochrome b562, and a T4 phage lysozyme domain), their common antiparallel arrangement of adjacent helices confers a stabilization of 5--7 kcal/mol (1 cal = 4.18 J). In contrast, a similarly packed array of parallel helices is relatively destabilized by 20 kcal/mol. These results show that helix-dipole interactions are important in the stabilization of this structural motif. These effects are discussed both in the context of folding pathways for 4-alpha-helical proteins and the stabilization of the higher aggregates.