Easily polarizable N+H…N hydrogen bonds between histidine side chains and proton translocation in proteins

Histidinium perchlorate having protecting groups at the α-amino and α-carboxylate group is studied by IR spectroscopy as function of the addition of protected histidine molecules. An intense continuous absorption arises, indicating that the N⁺H…N ? N…H⁺N formed are easily polarizable hydrogen bonds. From the integral absorbance of a band the concentration of the histidine-histidinium complex, i.e. the concentration of the easily polarizable hydrogen bonds is determined. It is shown that the absorbance of the continuum increases in proportion to the concentration of the easily polarizable N⁺H…N ? N…H⁺N bonds. Finally, it is discussed that via such an easily polarizable histidine-histidinium hydrogen bond a proton translocation in the active center of ribonuclease A may occur.     

Infrared investigation of poly-L-histidine structure dependent on protonation

Poly-L -histidine (PLH) films at different degrees of protonation were produced mid subjected to infrared spectroscopic investigation (range 4000-650 cm^?1). In addition, the N-deuterated film spectra were plotted. The amide II and III bands show that the peptide group is present in the trans form. The amide I and II bands show that at 0% and 50% protonation the PLH occurs as an α-helix and at 100% protonation as a random coil with some ranges in β structure. At 0% and 50% protonation, no hydration water is bound to the backbone. At 0% protonation all NH groups are linked to each other or to water molecules via hydrogen bonds. At 50% protonation NH⁺?N bonds form between the imidazole rings. These protons are present in continuous energy level distribution. Such bonds with tunneling protons are extremely polarizable and between these bonds may act proton dispersion forces. The Cl^? ions are bonded to the NH groups of the imidazole groups. The hydration water is bonded to the Cl^?? ions and to the NH groups. At 100% protonation, hydration water is bonded also to the CO groups of the backbone. The NH groups of the backbone, like those of the rings, endeavor especially in the dry state to bond to the Cl^? ions. This leads to a strong steric constraint of the random coil.     

Polysaccharide-polynucleotide complexes. Part 32. Structural analysis of the curdlan/poly(cytidylic acid) complex with semiempirical molecular orbital calculations

Natural Curdlan adopts a right-handed 6(1) triple helix, in which the constituting glucan chains are underpinned with each other by the intermolecular hydrogen bonds. Curdlan can form a stoichiometric complex with polynucleotides [e.g., poly(cytidylic acid), poly(C)]. In this paper, we carried out the MOPAC (semiempirical molecular-orbital package) calculation to examine the molecular structure of the Curdlan/poly(C) complex. The calculation exhibited that two types of hydrogen bonds are formed between the Curdlan and the poly(C); the third nitrogen (N3) in cytosine forms a hydrogen bond with the second OH of one Curdlan chain, and the proton of N4 is interacting with the O2 of another Curdlan chain. In our model, the helix diameter of poly(C) is expanded from 11.0 to 15.3 A upon complexation. Despite such large conformational changes, the 6(1) helix structure of poly(C) was maintained even after the complexation. This fact is complementary to the experimental fact that the complexation does not change the band shape of the circular dichroism of poly(C). The chain length dependence of the reaction enthalpy indicated that the complexation becomes thermodynamically more favorable with the chain length increasing. This feature is also consistent with the experimental data.     

Proton transfer in and polarizability of hydrogen bonds coupled with conformational changes in proteins. II. IR investigation of polyhistidine with various carboxylic acids

Polyhistidine-carboxylic acid systems are studied by ir spectroscopy. It is shown that OH ?N ? O^?…H⁺N bonds formed between carboxylic groups and histidine residues are easily polarizable proton-transfer hydrogen bonds when the pK_a of the protonated histidine residues is about 2.8 units larger than that of the carboxylic groups. From these results it bis concluded that OH ?N ? O^? ?H⁺N bonds between glutamic or aspartic acid histidine residues in proteins may be easily polarizable proton-transfer bonds. Furthermore, it is demonstrated that water molecules shift the proton-transfer equilibria in these hydrogen bonds in favor of the polar structure, i.e., due to water or polar environments OH ?N ? O^? ?H⁺N bonds with smaller ΔpK_a values become easily polarizable proton-transfer hydrogen bonds. A consideration of the amide bands of polyhistidine shows that it can be present in five different conformations. It is shown that these conformational changes are strongly related to the degree of proton transfer. Hence, the degree of proton transfer, the degree of hydration, and conformation are not independent of each other, but are strongly coupled. Further proof for the interdependence of proton transfer and conformational changes are hysteresis effects, which are observed with studies of polyhistidine dependent on carboxylic acid, adsorption and desorption. OH ?N ? O^? ?H⁺N bonds between aspartic and glutamic acid and histidine residues are present in hemoglobin, in ribonucleases, and in proteases, whereby this type of bond is preferentially found in the active centers of these enzymes. It is pointed out that hydrogen bonds with such interaction properties should be of great significance for structure and especially functions of proteins in which they are present.     

Time-resolved Fourier transform infrared spectroscopy of the polarizable proton continua and the proton pump mechanism of bacteriorhodopsin

Nanosecond-to-microsecond time-resolved Fourier transform infrared (FTIR) spectroscopy in the 3000-1000-cm(-1) region has been used to examine the polarizable proton continua observed in bacteriorhodopsin (bR) during its photocycle. The difference in the transient FTIR spectra in the time domain between 20 ns and 1 ms shows a broad absorption continuum band in the 2100-1800-cm(-1) region, a bleach continuum band in the 2500-2150-cm(-1) region, and a bleach continuum band above 2700 cm(-1). According to Zundel (G., J. Mol. Struct. 322:33-42), these continua appear in systems capable of forming polarizable hydrogen bonds. The formation of a bleach continuum suggests the presence of a polarizable proton in the ground state that changes during the photocycle. The appearance of a transient absorption continuum suggests a change in the polarizable proton or the appearance of new ones. It is found that each continuum has a rise time of less than 80 ns and a decay time component of approximately 300 micros. In addition, it is found that the absorption continuum in the 2100-1800-cm(-1) region has a slow rise component of 190 ns and a fast decay component of approximately 60 micros. Using these results and those of the recent x-ray structural studies of bR(570) and M(412) (H. Luecke, B. Schobert, H.T. Richter, J.-P. Cartailler, and J. K., Science 286:255-260), together with the already known spectroscopic properties of the different intermediates in the photocycle, the possible origins of the polarizable protons giving rise to these continua during the bR photocycle are proposed. Models of the proton pump are discussed in terms of the changes in these polarizable protons and the hydrogen-bonded chains and in terms of previously known results such as the simultaneous deprotonation of the protonated Schiff base (PSB) and Tyr185 and the disappearance of water molecules in the proton release channel during the proton pump process.     

Hydrogen bonds between protein side chains and phosphates and their role in biological calcification

Poly(L-histidine)-phosphate (H2PO4-, HPO4(2-)) and poly(L-glutamate)-phosphate systems (residue/phosphate, 1:1) in the presence of Ca2+ are studied by infrared spectroscopy. In the poly(L-histidine)-phosphate systems N...HOP in equilibrium NH+...O-P hydrogen bonds are formed where most phosphate protons are found at the histidine ring. With an increase in the degree of hydration the proportion of the proton limiting structure NH+...O-P increases. In the poly(L-glutamate)-dihydrogen phosphate system most phosphate protons are found at the carboxylate groups. Different behavior is observed for poly(L-glutamate)-hydrogen phosphate mixtures, where the residence time of the phosphate proton at the hydrogen acceptor carboxylate group is very short. This residence time increases, however, with increasing humidity. All these results support the triphasic theory of biological calcification involving a tripartite protein-calcium-phosphate complex where these hydrogen bonds can be present. The behavior of these hydrogen bonds can also explain the formation of a nidus of calcium phosphate salts in calcium oxalate-containing urinary calculi.     

An intramolecular hydrogen bond with large proton polarizability within the head group of phosphatidylserine. An infrared investigation.

Films of O-phospho-L-serine-P-ethylester (PSE) were studied by infrared spectroscopy. PSE films were studied pure and as 1:1 mixture with LiOH, NaOH, KOH, and Ca(OH)2 as a function of the degree of hydration. The same investigations were performed if (L-glu)n was added to the system (ratio 1:1, PSE/glu residue). In the PSE molecules an intramolecular (I) COOH...-OP in equilibrium with COO-...HOP (II) hydrogen bond is present. In this bond a double minimum proton potential occurs and it shows large proton polarizability. This hydrogen bond is relatively stable as shown by the neutralization experiments. At low degree of hydration the cations are present at the phosphate groups. The Li ions polarize the intramolecular hydrogen bonds much more than the other cations, i.e., the weight of the proton-limiting structure COOH...-OP is increased by Li ions. Regarding these results one has to assume that such a hydrogen bond is also present in the phosphatidylserine head groups. It is discussed that such hydrogen bonds could be part of a lateral charge-conducting system in the polar surfaces of biological membranes. Such systems could connect proton-creating and proton-consuming centers at the membrane surface and conduct positive charge at an extremely high rate.     

Proton transfer and polarizability of hydrogen bonds in proteins coupled with conformational changes. I. Infrared investigation of poly(glutamic acid) with various N Bases

The nature of hydrogen bonds formed between carboxylic acid residues and histidine residues in proteins is studied by ir spectroscopy. Poly(glutamic acid) [(Glu)_n] is investigated with various monomer N bases. The position of the proton transfer equilibrium OH…?N ? O^?…?H⁺N is determined considering the bands of the carboxylic group. It is shown that largely symmetrical double minimum energy surfaces are present in the OH…?N ? O^?…?H⁺N bonds when the pK_a of the protonated N base is two values larger than that of the carboxylic groups of (Glu)_n. Hence OH…?N ? O^?…?H⁺N bonds between glutamic and aspartic acid residues and histidine residues in proteins may be easily polarizable proton transfer hydrogen bonds. The polarizability of these bonds is one to two orders of magnitude larger than usual electron polarizabilities; therefore, these bonds strongly interact with their environment. It is demonstrated that water molecules shift these proton transfer equilibria in favor of the polar proton boundary structure. The access of water molecules to such bonds in proteins and therefore the position of this proton transfer equilibrium is dependent on conformation. The amide bands show that (Glu)_n is α-helical with all systems. The only exception is the (Glu)_n-n-propylamine system. When this system is hydrated (Glu)_n is α-helical, too. When it is dried, however, (Glu)_n forms antiparallel β-structure. This conformational transition, dependent on degree of hydration, is reversible. An excess of n-propylamine has the same effect on conformation as hydration.     

Thermodynamics of proton transfer in carboxylic acid-retinal Schiff base hydrogen bonds with large proton polarizability

During the photocycle of bacteriorhodopsin (BR) the chromophore, a retinal Schiff base, is deprotonated. Simultaneously an asp residue is protonated. These results suggest that this deprotonation occurs via a Schiff base - asp hydrogen bond. Therefore, we studied carboxylic acid - retinal Schiff base model systems in CCl4 using IR spectroscopy. The IR spectra show that double minimum proton potentials are present in the OH ... N in equilibrium with O- ... HN+ H-bonds formed and that the proton can easily be shifted in these bonds by local electrical fields. The thermodynamic data of H-bond formation and proton transfer within these H-bonds are determined. On the basis of these data a hypothesis is developed with regard to the molecular mechanism of the deprotonation of the Schiff base of BR.     

Poly(8-aminoguanylic acid): formation of ordered self-structures and interaction with poly(cytidylic acid).

Poly(8-aminoguanylic acid) has in neutral solution a novel ordered structure of high stability. The 8-amino group permits formation of three hydrogen bonds between two residues along the "top", or long axis, of the purines. The usual hydrogen bonding protons and Watson-Crick pairing sites are not involved in the association. The bonding scheme has a twofold rotation axis and is hemiprotonated at N(7). Poly(8NH2G) is converted by alkaline titration (pK = 9.7) to a quite different ordered structure, which is the favored form over the range approximately pH 10-11. The bonding scheme appears to be composed of a planar, tetrameric array of guanine residues, in which the 8-amino group does not participate in interbase hydrogen bonding. Poly (8NH2G) does not interact with poly(C) in neutral solution because of the high stability of the hemiprotonated G-G self-structure. Titration to the alkaline plateau, however, permits ready formation of a two-stranded Watson-Crick helix. In contrast to the monomer 8NH2GMP, poly(8NH2G) does not form a triple helix with poly(C) under any conditions. The properties of the ordered structures are interpreted in terms of a strong tendency of the 8-amino group to form a third interbase hydrogen bond, when this possibility is not prevented by high pH.     

Conformational features of a hexapeptide model Ac-TGAAKA-NH2 corresponding to a hydrated alpha helical segment from glyceraldehyde 3-phosphate dehydrogenase: implications for the role of turns in helix folding

Recent analysis of alpha helices in protein crystal structures, available in literature, revealed hydrated alpha helical segments in which, water molecule breaks open helix 5-->1 hydrogen bond by inserting itself, hydrogen bonds to both C=O and NH groups of helix hydrogen bond without disrupting the helix hydrogen bond, and hydrogen bonds to either C=O or NH of helix hydrogen bond. These hydrated segments display a variety of turn conformations and are thought to be 'folding intermediates' trapped during folding-unfolding of alpha helices. A role for reverse turns is implicated in the folding of alpha helices. We considered a hexapeptide model Ac-1TGAAKA6-NH2 from glyceraldehyde 3-phosphate dehydrogenase, corresponding to a hydrated helical segment to assess its role in helix folding. The sequence is a site for two 'folding intermediates'. The conformational features of the model peptide have been investigated by 1H 2D NMR techniques and quantum mechanical perturbative configuration interaction over localized orbitals (PCILO) method. Theoretical modeling largely correlates with experimental observations. Based upon the amide proton temperature coefficients, the observed d alpha n(i, i + 1), d alpha n(i, i + 2), dnn(i, i + 1), d beta n(i, i + 1) NOEs and the results from theoretical modeling, we conclude that the residues of the peptide sample alpha helical and neck regions of the Ramachandran phi, psi map with reduced conformational entropy and there is a potential for turn conformations at N and C terminal ends of the peptide. The role of reduced conformational entropy and turn potential in helix formation have been discussed. We conclude that the peptide sequence can serve as a 'folding intermediate' in the helix folding of glyceraldehyde 3-phosphate dehydrogenase.     

Phosphate- N base hydrogen bonds involving proton transfer with reference to the non-enzymic hydrolysis of ATP

IR spectra of aqueous solutions of 1:1 mixtures of H₂PO₄^? and various N bases have been studied as models for (POH?N) → (P^?O?H⁺N) hydrogen bonds. 50% proton transfer is observed when the pKa of the protonated N base is 1.1 smaller than that of the phosphate group. The hydrogen bonds are easily polarizable near this equilibrium. These results strongly support the conclusion that such bonds contribute 1) to the self-association of ATP and ADP and 2) to the association of the hydrolysis products ADP and inorganic phosphate.     

Vibrational fluctuations of hydrogen bonds in a DNA double helix with nonuniform base pairs.

The Green's function technique is applied to a study of breathing modes in a DNA double helix which contains a region of different base pairs from the rest of the double helix. The calculation is performed on a G-C helix in the B conformation with four consecutive base pairs replaced by A-T. The average stretch in hydrogen bonds is found amplified around the A-T base pair region compared with that of poly(dG)-poly(dC). This is likely related to the A-T regions lower stability against hydrogen bond melting. The A-T region may be considered to be the initiation site for melting in such a helix.     

Synergistic effects in the melting of DNA hydration shell: melting of the minor groove hydration spine in poly(dA).poly(dT) and its effect on base pair stability.

We propose that water of hydration in contact with the double helix can exist in several states. One state, found in the narrow groove of poly(dA).poly(dT), should be considered as frozen to the helix, i.e., an integral part of the double helix. We find that this enhanced helix greatly effects the stability of that helix against base separation melting. Most water surrounding the helix is, however, melted or disassociated with respect to being an integral part of helix and plays a much less significant role in stabilizing the helix dynamically, although these water molecules play an important role in stabilizing the helix conformation statically. We study the temperature dependence of the melting of the hydration spine and find that narrow groove nonbonded interactions are necessary to stabilize the spine above room temperature and to show the broad transition observed experimentally. This calculation requires that synergistic effects of nonbonded interactions between DNA and its hydration shell affect the state of water-base atom hydrogen bonds. The attraction of waters into narrow groove tends to retain waters in the groove and compress or strain these hydrogen bonds.     

The significance of the 2' OH group and the influence of cations on the secondary structure of the RNA backbone.

In the IR spectra, the coupling of vibrations leads to band splitting and/or bands shifting in opposite directions which provides information on the mutual orientation of groupings. From such band shifts in the range 1800 to 1500 cm-1 one can draw conclusions on the double helix formation of polynucleotides. These band shifts are caused either by vibrational coupling of stretching vibrations within pairs of base residues or by coupling of stretching vibrations with the bending (scissor) vibration of the -NH2 groups; the latter is indicated by band shifts after deuterium substitution within the amino groups. Couplings of phosphate and 1 ibose vibrations in the range 1300 to 1000 cm-1 provide information on the secondary structure of the backbone. In order to obtain information of the structure of the RNA backbone, the IR spectra of poly(ribonucleotides) were studied in neutral media in which they were single-stranded. The shift due to coupling of the band of the 2'OD bending vibration and that of the antisymmetric stretching vibration of the ether group of the ribose residue proves that ribose residues of the backbone are cross-linked via hydrogen bonds. These are formed between the 2'OD or 2'OH groups, respectively, and the O atoms of the ether group of the neighboring ribose residues. This is the reason for the difference between DNA and RNA as regards the 2'OH group. The structure formation caused by these hydrogen bonds results in a stiffening of the RNA backbone. The tendency to form these hydrogen bonds increases in the order poly (U), poly(C), poly (A). This order of secondary structure stabilization is due to an interplay between the influences of (1) the 2'OH hydrogen bonds and (2) the base residues' stacking. Furthermore, the coupling of the antisymmetric stretching vibration of the greater than PO2- groups with a vibration involving the 2'OH group can result in a doublet structure of the band at about 1240 cm-1 if cations with strong fields are present. This probably shows that these cations can turn the greater than PO2-groups-which are usually turned outward at the backbone, as shown by construction of molecular models- towards the basic residues. Thus they cause stiff monohelices which are right-handed screws.     

Premelting thermal fluctuational interbase hydrogen-bond disrupted states of a B-DNA guanine-cytosine base pair: significance for amino and imino proton exchange.

Modified self-consistent phonon theory when applied to the DNA double helix indicates the existence of fairly long-lived states in which single interbase H bonds are disrupted. One can then postulate a number of situations in which particular disrupted H bonds can enhance particular proton exchange. In this paper we postulate a number of such partially open states for a B-conformation GC base pair and calculate the probability of each of these states for a B-conformation poly(dG).poly(dC). We compare these probabilities to those probabilities needed to explain various observed proton exchange rates. We propose that, for a GC base pair in B conformation, there are two amino proton exchangeable states--a cytosine amino proton exchangeable state and a guanine amino proton exchangeable state; both require the disruption of only the corresponding interbase H bond. The imino proton exchange, however, requires the disruption of all three interbase H bonds and this defines a third open state. Our calculated probabilities for a GC base pair in these three states are in fair agreement with available experimental estimates from measurements of amino and imino proton exchange.     

Vibrational fluctuations of hydrogen bonds in a DNA double helix with alternating TA type inserts.

The Green's function technique is applied to a study of breathing modes in a DNA double helix which contains a region of different base pairs from the rest of the double helix. The calculation is performed on an alternating poly(dC-dG).poly(dC-dG) helix in the B conformation with four consecutive base pairs replaced by a model of a biological promoter region with four alternating T-A,A-T base pairs, henceforth referred to as (TATA)2. The average stretch of interbase hydrogen bonds is found to be amplified around the insert. This is likely related to the (TATA)2 insert having a lower stability against hydrogen bond melting than the two semi-infinite poly(dC-dG).poly(dC-dG) helices. The insert region may be considered to be a site of enhanced tendency to melt in such a helix. The results show that an alternating AT insert of four base pairs has a larger average hydrogen bond stretch inside and outside the insert region than the average hydrogen bond stretch inside and outside an insert of four consecutive A-T base pairs, henceforth referred to as (AAAA).(TTTT). Calculations are performed which show that the enhancement of the average hydrogen bond stretch around an alternating TA type insert is greatly dependent upon the local modes and not the inband modes. The amount of local mode enhanced average stretch is explored as a function of insert size.     

Observation of internucleotide NH...N hydrogen bonds in the absence of directly detectable protons

Several structural motifs found in nucleic acids involve N-H...N hydrogen bonds in which the donor hydrogens are broadened to extinction due to chemical or conformational exchange. In such situations, it is impossible to use the well-established HNN-COSY or soft HNN-COSY experiments, which report the presence of the hydrogen bond directly on the donor proton(s). We present a pulse sequence, H(CN)N(H), for alleviating this problem in hydrogen bonds of the type NdH...Na-CH, in which the donor Nd nitrogen is correlated with the corresponding non-exchangeable C-H proton associated with the acceptor Na nitrogen. In this way, missing NdH...Na correlations in an HNN-COSY spectrum may be recovered from CH-Nd correlations in the H(CN)N(H) spectrum. By correlating a different set of nuclei relative to the HNN-COSY class of experiments, the H(CN)N(H) experiment also serves to remove ambiguities associated with degeneracies in HNN-COSY spectra. The technique is demonstrated on d(GGAGGAG)4,a quadruplex containing a novel A. (G.G.G.G). A hexad and on d(GGGCAGGT)4, containing a G.G.G.C tetrad, in which missing NH2...N7 correlations are retrieved via H8-(N2,N6) correlations in the H(CN)N(H) spectrum.     

Proton magnetic resonance studies of double helical oligonucleotides. The effect of base sequence on the stability of deoxydinucleotide dimers.

The concentration dependence of the proton magnetic resonance chemical shifts of a series of deoxydinucleotides and deoxydinucleoside monophosphates in neutral H2O solution has been recorded in the 1-100 mM concentration range by the use of pulsed Fourier transform techniques. The self-complementary molecules pdG-dC, dG-dC, pdC-dG, and dC-dG and the complementary mixtures pdG-dG + pdC-dC as well as pdG-dT + pdA-dC interact at low temperatures by the formation of intermolecular hydrogen bonded dimers. Noncomplementary molecules such as pdG-dT, pdT-dG, pdG-dG, pdA-dc, and pdC-dC do not self-associate by the formation of intermolecular hydrogen bonds under the present experimental conditions. The chemical shifts of the amino protons and the base protons are consistent with the interaction of two complementary dinucleotides to form a miniature double helix. An analysis of the chemical shift of the guanine amino proton resonance as a function of dinucleotide concentration has provided approximate dimerization constants. These results show that the stability of the miniature double helices is in the order (pdG-dG)-(pdC-dC) greater than or approximately (pdG-dC)-(pdG-dC) greater than (pdC-dG)-(pdC-dG) greater than (pdG-dT)-(pdA-dC) which reflects the effect of nucleotide sequence (and composition) on helix stability.     

Forces stabilizing proteins

The goal of this article is to summarize what has been learned about the major forces stabilizing proteins since the late 1980s when site-directed mutagenesis became possible. The following conclusions are derived from experimental studies of hydrophobic and hydrogen bonding variants. (1) Based on studies of 138 hydrophobic interaction variants in 11 proteins, burying a –CH₂− group on folding contributes 1.1 ± 0.5 kcal/mol to protein stability. (2) The burial of non-polar side chains contributes to protein stability in two ways: first, a term that depends on the removal of the side chains from water and, more importantly, the enhanced London dispersion forces that result from the tight packing in the protein interior. (3) Based on studies of 151 hydrogen bonding variants in 15 proteins, forming a hydrogen bond on folding contributes 1.1 ± 0.8 kcal/mol to protein stability. (4) The contribution of hydrogen bonds to protein stability is strongly context dependent. (5) Hydrogen bonds by side chains and peptide groups make similar contributions to protein stability. (6) Polar group burial can make a favorable contribution to protein stability even if the polar group is not hydrogen bonded. (7) Hydrophobic interactions and hydrogen bonds both make large contributions to protein stability.