Structurally symmetrical,easily polarizable hydrogen bonds between side chains in proteins and proton-conducting mechanisms. III

(L -Cys)_n, (L -Lys)_n, and (L -Glu)_n were studied by ir spectroscopy in terms of their degree of deprotonation or protonation. It is shown that structurally symmetrical, easily polarizable SH ?S^? ? ^?S ?HS, N⁺H ?N ? N ?H⁺N, and OH ?O^? ? ^?O ?HO hydrogen bonds are formed between the side chains. The different wave number distributions of the ir continua caused by these hydrogen bonds show that the barrier in the double-minimum proton potential decreases in the series of these hydrogen bonds. The stability of these hydrogen bonds against hydration increases in this series. The OH ?O^? ? ^?O ?HO bonds are not broken by small amounts of water. With (L -Cys)_n the formation of easily polarizable hydrogen bonds and a β-structure–coil transition are strongly interdependent. As a result of this coupling effect, the β-structure–coil transition becomes cooperative. With (L -Glu)_n, the formation of the polarizable hydrogen bonds and the observed conformational change are independent processes. The (L -Glu)_n conformation changes from α-helix to coil only if more than 80% of the residues are deprotonated. Finally, on the basis of the various types of easily polarizable hydrogen bonds, charge shifts in active centers of enzymes and the proton-conducting mechanism through hydrophobic regions of biological membranes are discussed.     

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.     

Proton polarizability and proton transfer in histidine-phosphate hydrogen bonds as a function of cations present: ir investigations

(L -His)_n- dihydrogen phosphate systems are studied by ir spectroscopy in the presence of various cations and as a function of the degree of hydration. Ir continua indicate that (I) OH … N ? O^?…H⁺N (IIR) hydrogen bonds are formed and that these bonds show high proton polarizability, which increases from the Li⁺ to the K⁺ system. In the K⁺?system, His-P_i-P_i chains are formed, showing particularly high proton polarizability due to collective proton motion within both hydrogen bonds. The OH N ? O^?…H^?N equilibria are determined from ir bands. With the Li⁺ system, 55% of the protons are present at the histidine residues; this percentage is smaller with the Na⁺ system (41%), and amounts to only 32% with the K⁺ system. With the increasing degree of hydration the removal of the degeneracy of ν_as?PO^2?₃ vanishes, indicating loosening of the cations from the phosphates. Nevertheless, the hydrogen bond acceptor O atom becomes more negative; a shift of the equilibrium to the right is observed in the OH… N ? O^?…H⁺N bond. This is explained by the strong interaction of the dipole of the hydrogen bonds with the water molecules. All these results show that protons can be shifted easily in these hydrogen bonds due to their high proton polarizability. The transfer equilibria can be controlled easily by local electrical fields. In addition, these results may be of significance when phosphates interact with proteins.     

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.     

Proton translocation in hydrogen bonds with large proton polarizability formed between a Schiff base and phenols

OH…N ? O^?…H⁺N hydrogen bonds formed between N-all-transretinylidene butylamine (Schiff base) and phenols (1:1) are studied by IR spectroscopy. It is shown that both proton limiting structures of these hydrogen bonds have the same weight with Δ pK_a (50%) = (pK_a protonated Schiff base minus pK_a phenol) = 5.5. With the largely symmetrical systems, continua demonstrate that these hydrogen bonds show great proton polarizability. In the Schiff base + tyrosine system in a non-polar solvent the residence time of the proton at the tyrosine residue is much larger than that at the Schiff base. In CH₂CCl₂ these hydrogen bonds show, however, still proton polarizability, i.e., the position of the proton transfer equilibrium OH…N ? O^?…H⁺N is shifted to and fro as function of the nature of the environment of this hydrogen bond. Consequences regarding bacteriorhodopsin are discussed.     

Association studies of N-acetyl-amino acid N,N-dimethylamides in carbon tetrachloride

The self-association of N-acetylglycine N,N-dimethylamide, N-acetyl-L -valine N,N-dimethylamide, and N-acetyl-L -phenylalanine N,N-dimethylamide in carbon tetrachloride was investigated by using ir and ¹H-nmr methods. It was concluded from ir measurements that the associated species is the dimer formed as a result of the simultaneous formation of two intermolecular hydrogen bonds. This is supported by the results of ¹H-nmr measurements. Thermodynamic quantities for the association were determined from the temperature and concentration dependence of the NH proton chemical shifts of the sample solutions. Compared with the Gly derivative, L -Val and L -Phe derivatives have larger values of ?ΔH for association, which shows good correlation with Δv_NH values, the difference between the maxima of the monomer and dimer bands, obtained from ir spectra. This is due to the less stable monomer conformation and to the stronger intermolecular hydrogen bonding of the dimers in L -Val and L -Phe derivatives. The line shapes of both methyl proton resonances of L -Val residue and methylene proton resonances of L -Phe residue were found to vary with concentration and temperature of the sample solutions. These data indicate that the rotation about the C^α—C^β bond is restricted by the steric hindrance present in the associated dimers. All these experimental results can be related to the fact that L -Val and L -Phe derivatives have a warped framework because of the bulky side chains, whereas the Gly derivative has a planar framework.     

Proton transfer in and polarizability of hydrogen bonds in proteins. Tyrosine-lysine and glutamic acid-lysine hydrogen bonds — IR investigations

The OH N O^– H⁺N hydrogen bonds formed between tyrosine and lysine, and between glutamic acid and lysine residues are studied by infrared spectroscopy considering the following systems: (l-lys)_n + phenol, copoly (l-lys, l-tyr)_n, (l-lys)_n + (l-tyr)_n and (l-lys)_n + (l-glu)_n. The phenol-lysine hydrogen bonds are largely symmetrical in the average if the pK_a of the protonated lysine is 2.2 units larger than that of the phenols. In the case of the hydrogen bonds between tyrosine and lysine residues in copoly (l-lys, l-tyr)_n and (l-lys)_n + (l-tyr)_n, the weight of the proton limiting structure OH N is 80–90%, and that of the polar O^– H⁺N structure 10–20%. Double minimum proton potentials occur but the proton is preferentially present at the tyrosine residues. In the (l-lys)_n + (l-glu)_n system, the protons are present at the lysine residues. Thus, these hydrogen bonds have very large dipole moments (about 10 D). With the lysine-phenole hydrogen bonds, hydration shifts the proton transfer equilibrium a little in favour of the polar proton limiting structure O^– H⁺N. These hydrogen bonds are broken to a large extent, however, when only about 3 water molecules are present per lysine residue. When less water is present, as in the copoly (l-lys, l-tyr)_n and (l-lys)_n + (l-tyr)_n systems, these hydrogen bonds are, however, formed quantitatively. Thus — as discussed in this paper — the tyrosine-lysine hydrogen bonds can participate in proton conducting hydrogen bonded systems — as, for instance, present in bacteriorhodopsin — performing the proton transport through hydrophobic regions of biological membranes.     

Easily polarizable proton transfer hydrogen bonds between the side chains of histidine and the carboxylic acid groups of glutamic and aspartic acid residues in proteins

The nature of the hydrogen bonds formed between glutamic acid and histidine residues between aspartic acid and histidine residues is studied by i.r. spectroscopy. These studies were performed with $\text{(}\text{l}\text{-Glu}\text{)}{}_{\mathrm{n}}\text{+(}\text{l}\text{-His}\text{)}{}_{\mathrm{n}}$ and with associates of monomeric Glu + His and Asp + His systems in solutions whereby these amino acids had protected α-amino and α-carboxylic groups. It is shown that the OH …N?^?O?H⁺N bonds are easily polarizable proton transfer hydrogen bonds. The residence time of the proton at the His is a little larger in the case of the Asp + His than in the case of the Glu + His systems. Polar environments shift this proton transfer equilibrium in favour of the proton limiting structure ^?O?H⁺N, and less polar ones in favour of the structure OH?N. These results demonstrate that the large proton polarizability of the hydrogen bonded system in the active centre of chymotrypsin is responsible for the charge shift caused by the substrate, and thus for the increase in reactivity of the serine residue and the catalytic activity of the enzyme.     

Proton polarizability of poly(L-tyrosine)–hydrogen phosphate hydrogen bonds as a function of alkali cations

We studied films of poly(L -tyrosine) with hydrogen phosphate (residue/phosphate, 1:1) by ir spectroscopy. The influences of the alkali cations (Li⁺, Na⁺, K⁺) and of the degree of hydration were clarified. If Li⁺ ions are present, the OH ?^?OP hydrogen bonds formed in the dried films between the tyrosine OH groups and hydrogen phosphate are asymmetrical. The formation of hydrogen phosphate–hydrogen phosphate hydrogen bonds is prevented by the presence of the Li⁺ ions. With an increase in the degree of hydration, the tyrosine–phosphate bonds are not broken but become slightly stronger. Completely different behaviour is found if K⁺ ions are present. In dry films, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed between tyrosine and hydrogen phosphate show large proton polarizability. The tyrosine proton has a noticeable residence time at the acceptor O atom of the phosphate. The difference in the behaviour of the system with K⁺ ions when compared to the system with Li⁺ ions can be explained, since the hydrogen acceptor O atom of phosphate ions is more negatively charged due to the weaker influence of the K⁺ ions. Furthermore, POH ?^?OP hydrogen bonds between hydrogen phosphate molecules are formed. With an increase in the degree of hydration, the tyrosine–hydrogen phosphate hydrogen bonds are broken, all tyrosine protons are found at the tyrosine residues, and the -PO₃^? groupings are in a symmetrical environment, indicating that the K⁺ ions are removed from these groupings. If the degree of hydration increases further, hydrogen-bonded systems such as hydrogen phosphate–water–hydrogen phosphate are formed that show large proton polarizability due to collective proton motion. When Na⁺ ions are present, the OH ?^?OP ? O^? ?HOP hydrogen bonds formed in dry films still show proton polarizability, but the residence time of the tyrosine proton at the phosphate is very short.     

Abundance and arrangement of single,double and bifurcated hydrogen bonds in protein α-helices: Statistical analysis of PDB-select

Statistics are collected and analyzed for the possibility of hydrogen bonding in the secondary structures of globular proteins, based on geometric criteria. Double and bifurcated bonds are considered as pairs of admissible H-bonds with two proton donors or two proton acceptors, respectively. Most of such bonds belong to peptide groups in α-helices, with O _i …N _{i + 3} nearly as frequent as O _i …N _{i + 4}; in contrast, most of the 3/10-helical segments are too short to have any. Alternating double and bifurcated bonds in α-helices form an apparently cooperative network structure. A typical α-helical segment perhaps carries two stretches of the H-bond network broken in the middle. The constituent H-bonds are nonlinear: the hydrogen atom is off the straight line connecting the proton donor and proton acceptor atoms. This deflection is larger for H _{i + 3} vs. bond line O _i −N _{i + 3} than for H _{i + 4} vs. O _i −N _{i + 4}, and though the two kinds of bond have about the same length (exceeding those typical of low-molecular compounds), O _i …N _{i + 4} must be stronger than O _i …N _{i + 3}. Double/bifurcated bonds are also not coplanar, i.e., hydrogen atoms are beyond the N…O…N (or O…N…O) plane. The text was submitted by the authors in English.     

Helix promotion in polypeptides by polyols

The helix content of [L -Lys(Me₃)]_n · ClO₄, and [L -Lys(Me₃)⁵⁰, L -Ala⁵⁰]_n · ClO₄ in water is markedly increased by the presence of sucrose and glycerol. For [L -Lys(Me₃)]_n · ClO₄ the ellipticity at 222 nm changes from +2 × 10³ deg cm² dmole^?1 in water to ?44 × 10³ in 50% glycerol. Sucrose does not promote helix formation in melittin at pH 7.2, but glycerol does. At pH 5.5 sucrose and, more so, glycerol, induce helix in melittin. Glycerol induces some helix in methylated melittin, but less than in melittin. The results are discussed in relation to excluded volume effects, ΔG of transfer of peptide and hydrophobic groups from water to mixed solvents, electrostatic effects, and preferential hydration. © 1993 John Wiley & Sons, Inc.     

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.     

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.     

Asparagine and glutamine differ in their propensities to form specific side chain-backbone hydrogen bonded motifs in proteins

Short range side chain‐backbone hydrogen bonded motifs involving Asn and Gln residues have been identified from a data set of 1370 protein crystal structures (resolution ≤ 1.5 Å). Hydrogen bonds involving residues i ? 5 to i + 5 have been considered. Out of 12,901 Asn residues, 3403 residues (26.4%) participate in such interactions, while out of 10,934 Gln residues, 1780 Gln residues (16.3%) are involved in these motifs. Hydrogen bonded ring sizes (C_n, where n is the number of atoms involved), directionality and internal torsion angles are used to classify motifs. The occurrence of the various motifs in the contexts of protein structure is illustrated. Distinct differences are established between the nature of motifs formed by Asn and Gln residues. For Asn, the most highly populated motifs are the C₁₀ (CO^δ_i …NH_{i + 2}), C₁₃ (CO^δ_i …NH_{i + 3}) and C₁₇ (N^δH_i …CO_{i ? 4}) structures. In contrast, Gln predominantly forms C₁₆ (CO^ε_i …NH_{i ? 3}), C₁₂ (N^εH_i …CO_{i ? 2}), C₁₅ (N^εH_i …CO_{i ? 3}) and C₁₈ (N^εH_i …CO_{i ? 4}) motifs, with only the C₁₈motif being analogous to the Asn C₁₇structure. Specific conformational types are established for the Asn containing motifs, which mimic backbone β‐turns and α‐turns. Histidine residues are shown to serve as a mimic for Asn residues in side chain‐backbone hydrogen bonded ring motifs. Illustrative examples from protein structures are considered. Proteins 2012; © 2011 Wiley Periodicals, Inc.     

Chain length dependent transition of 310- to α-helix of Boc-(Ala-Aib)n-OMe

An apolar synthetic octapeptide, Boc-(Ala-Aib)₄-OMe, was crystallized in the triclinic space group P1 with cell dimensions a = 11.558 Å, b = 11.643 Å, c = 9.650 Å, α = 120.220°, β = 107.000°, γ = 90.430°, V = 1055.889 ų, Z = 1, C₃₄H₆₀O₁₁N₈·H₂O. The calculated crystal density was 1.217 g/cm³ and the absorption coefficient ? was 6.1. All the intrahelical hydrogen bonds are of the 3₁₀ type, but the torsion angles, ? and ψ, of Ala(5) and Ala(7) deviate from the standard values. The distortion of the 3₁₀-helix at the C-terminal half is due to accommodation of the bulky Boc group of an adjacent peptide in the nacking. A water molecule is held between the N-terminal of one peptide and the C-terminal of the other. The oxygen atom of water forms hydrogen bonds with N (1) -H and N (2) -H, which are not involved in the intrahelical hydrogen bonds. The hydrogen atoms of water also formed hydrogen bonds with carbonyl oxygens of the adjacent peptide molecule. On the other hand, ¹H-nmr analysis revealed that the octapeptide took an α-helical structure in a CD₃CN solution. The longer peptides, Boc-(Ala-Aib)₆-OMe and Boc-(Ala-Aib)₈-OMe, were also shown to take an α-helical structure in a CD₃CN solution. An α-helical conformation of the hexadecapeptide in the solid state was suggested by x-ray analysis of the crystalline structure. Thus, the critical length for transition from the 3₁₀- to α-helix of Boc-(Ala-Aib)_n-OMe is 8. © 1993 John Wiley & Sons, Inc.     

Vibrational CD studies of the solution conformation of N-urethanyl-L-amino acid derivatives

The solution conformations of several N-urethanyl-L -amino acids in 0.2–0.002M chloroform and 0.2M dimethylsulfoxide have been investigated by using vibrational circular dichroism (VCD), ir absorption, and ¹³C-nmr spectroscopies. Both the N-carbobenzoxy (N-CBZ) and N-t-butoxycarbonyl derivatives of L -alanine, L -proline, L -valine, and L -phenylalanine, and N-CBZ-serine were studied. The ¹³C-nmr results indicate that the molecules occur predominantly as the cis isomer about the C? N peptide bond at room temperature. The interpretation of the strong VCD couplet in the carbonyl-stretching region using the degenerate coupled oscillator model is consistent with the conformational range of ? = ?60° to ?90° and ψ = 30° to 90° for molecules forming acid dimers. Conformations with an intramolecularly hydrogen-bonded C₇ ring are also present, which give rise to biased VCD features in the NH-, CH-, and C?O-stretching regions that can arise due to vibrationally generated ring currents.     

IR study of the proton acceptor ability of N-t-butoxycarbonylproline N′-methylamide

Hydrogen bonding between N-t-butoxycarbonylproline N′-methylamide and phenol derivatives (pK_a = 10.20–7.75) are investigated by ir and Fourier transform ir spectrometry. The thermodynamic parameters determined in carbon tetrachloride solution show that the complexes are of medium strength, the stability constants at 298 K range from 80 to 1530 L mol^?1, and the enthalpies of complex formation range from – 30 to –34 kJ mol^?1. The study of the ir spectra in the ν_OH, ν_NH, and ν_c?o regions shows that complex formation occurs at the oxygen atom of the amide carbonyl. Hydrogen-bond formation at this site strengthens the intramolecular hydrogen bond of the seven-membered ring. © 1993 John Wiley & Sons, Inc.     

Quantitative two-dimensional nmr study of dermenkephalin,a highly potent and selective δ-opioid peptide

Dermenkephalin, H-Tyr-(D ) Met-Phe-His-Leu-Met-Asp-NH₂, a highly potent and selective δ-opioid peptide isolated from frog skin, was studied in DMSO-d₆ solution by two-dimensional nmr spectroscopy, including the determination of NH temperature coefficients, the evaluation of ³J coupling constants from phase-sensitive correlated spectroscopy (COSY) and the volumes of nuclear Overhauser effect (NOE) correlations. The two-dimensional NOE spectroscopy (NOESY) spectrum of dermenkephalin revealed sequential, medium-, and long-range effects. To put this information on a quantitative basis, special attention was devoted to J cross-peak suppression, quantification of the NOE volumes and analysis of the overlaps, normalization of the NOEs against diagonal peaks and H_ββ′ geminal interactions. Although most of the dihedral angles deduced from the ³J_Nα coupling constants together with several N_iα_i and α_iN_{i + 1} NOEs pointed to a partially extended peptide backbone, several N_i N_{i + 1} NOEs and β_i N_{i + 1} interactions argued in favor of a folded structure. Moreover, several long-range correlations of strong intensities were found that supported a close spatial proximity between the side chains of D -Met² and Met⁶, Tyr¹ and His⁴, Tyr¹ and Asp⁷, and His⁴ and the C-terminal amide group. In Phe, the g^? rotamer in the side chain is deduced from the ³J_αβ coupling constants and αβ and Nβ NOE correlations. Whereas the amide proton dependency was not indicative of stable hydrogen bonds, the nonuniform values of the temperature coefficient may reflect an equilibrium mixture of folded and extended conformers. The overall data should provide realistic starting models for energy minimization and modelization studies. © 1993 John Wiley & Sons, Inc.     

15N-NMR spectroscopy. IV. Comparison of poly(L-lysine) and isopoly(L-lysine)

The natural abundance ¹⁵N-nmr spectroscopy has been used to characterize the isomeric polymers (L -Lys)_n and iso (L -Lys)_n in aqueous solution. Although the peptide nitrogens of the two polymers have nearly equivalent shifts at pH < 10, the amino nitrogens differ by 5–6 ppm at pH < 7 and provide an easy means of identification. Furthermore, the polymers are distinguishable by the pK_a of the amino group and the basicity of the peptide nitrogen. At pH 10.3 and 25°C, (Lys)_n exhibits line broadening and an upfield chemical shift of the peptide nitrogen, indicative of the coil → helix transition. The formation of 100% helix may produce a shift as large as 5 ppm, which probably makes ¹⁵N-nmr spectroscopy more suitable for studies of this transition.     

Infrared spectra and structure of synthetic polytripeptides

A number of polytripeptides related to collagen, namely, (Gly-Pro-Pro)_n, (Gly-Pro-Hyp)_n, (Gly-Hyp-Hyp)_n, (Gly-Pro-Ala)_n, (Gly-Pro-Leu)_n, (Gly-Pro-Gly)_n,(Gly-Ala-Pro)_n, (Gly-Ala-Hyp)_n, (Ala-Pro-Pro)_n, and (Ala-Hyp-Hyp)_n were investigated by the method of ir spectroscopy and hydrogen-deuterium kinetics. Strength and order of interpeptide hydrogen bonds of the polytripeptides in a triple-helical conformation were found to depend on the amino acid composition and residue sequence in the triplets. Correlation of X-ray diffraction and spectroscopic data for (Gly-Pro-Hyp)_n showed that the increase of the helix parameter in the process of dehydration is accompanied with the weakening of interpeptide hydrogen bonds. Influences of bound water on the length and order of interchain hydrogen bonding was also examined. It was shown that the incorporation of water molecules into the triple helix depends on the amino acid composition and residue sequence. Synthetic models and native collagens were compared.