Measurement of grain growth in the recrystallization of rapidly frozen solutions of antifreeze glycoproteins

A quantitative estimate of the activation energy for grain growth has been obtained by analyzing ice recrystallization experiments from water and from solutions with small amounts (< 1.0 μg/mL) of antifreeze glycoprotein (AFGP). Rates of grain growth are measured as changes of grain diameter in time, with the supercooled holding temperature aVid glycoprotein concentration as parameters. Arrhenius plots of these rates vs (1/T) yielded slopes proportional to the activation energies for the particular species. The values of activation energy are almost independent of solution concentration or the species of AFGP. Averaged activation energy value for the AFGP-4 species is Q_g = (6.61 ± 1.02) × 10⁵ J/mole. The “less active” AFGP-8 yielded an average Q_g = (5.71 ± 2.39) × 10⁵ J/mole, quite similar to the AFGP-4 species. The activation energy for recrystallization in a pure ice-water system was estimated from two temperature points, T = ?5.4 and ?7.5°C. The best value is 2.39 × 10⁵ J/mole, nearly twice that obtained by M. N. Martino and N. E. Zaritsky [(1989) Cryobiology, Vol. 26, p. 138] in a recrystallization experiment using salt solution, but much smaller than the values derived from the AFGP solutions. Results further show that activation entropy is at least a factor of 2 larger for the AFGP species than that of pure ice-water system under the same growth conditions. These results suggest significant roles, both energetically and entropically, for AFGP molecules in their ability to inhibit grain growth of ice. © 1994 John Wiley & Sons, Inc.     

The dynamics,structure, and conformational free energy of proline-containing antifreeze glycoprotein

Recent NMR studies of the solution structure of the 14-amino acid antifreeze glycoprotein AFGP-8 have concluded that the molecule lacks long-range order. The implication that an apparently unstructured molecule can still have a very precise function as a freezing inhibitor seems startling at first consideration. To gain insight into the nature of conformations and motions in AFGP-8, we have undertaken molecular dynamics simulations augmented with free energy calculations using a continuum solvation model. Starting from 10 different NMR structures, 20 ns of dynamics of AFGP were explored. The dynamics show that AFGP structure is composed of four segments, joined by very flexible pivots positioned at alanine 5, 8, and 11. The dynamics also show that the presence of prolines in this small AFGP structure facilitates the adoption of the poly-proline II structure as its overall conformation, although AFGP does adopt other conformations during the course of dynamics as well. The free energies calculated using a continuum solvation model show that the lowest free energy conformations, while being energetically equal, are drastically different in conformations. In other words, this AFGP molecule has many structurally distinct and energetically equal minima in its energy landscape. In addition, conformational, energetic, and hydrogen bond analyses suggest that the intramolecular hydrogen bonds between the N-acetyl group and the protein backbone are an important integral part of the overall stability of the AFGP molecule. The relevance of these findings to the mechanism of freezing inhibition is discussed.     

Conformational changes due to vicinal glycosylation: The branched α-l-Rhap(1–2)[β-d-Galp(1–3)]-β-d-Glc1-OMe trisaccharide compared with its parent disaccharides*

Conformations of the α-l -Rhap(1-2)-β-d -Glc1-OMe and β-d -Galp(1-3)-β-d -Glc1-OMe disaccharides and the branched title trisaccharide were examined in DMSO-d₆ solution by ¹H-nmr. The distance mapping procedure was based on rotating frame nuclear Overhauser effect (NOE) constraints involving C- and O-linked protons, and hydrogen-bond constraints manifested by the splitting of the OH nmr signals for partially deuteriated samples. An “isotopomer-selected NOE” method for the unequivocal identification of mutually hydrogen-bonded hydroxyl groups was suggested. The length of hydrogen bonds thus detected is considered the only one motionally nonaveraged nmr-derived constraint. Molecular mechanics and molecular dynamics methods were used to model the conformational properties of the studied oligosaccharides. Complex conformational search, relying on a regular Φ,Ψ-grid based scanning of the conformational space of the selected glycosidic linkage, combined with simultaneous modeling of different allowed orientations of the pendant groups and the third, neighboring sugar residue, has been carried out. Energy minimizations were performed for each member of the Φ,Ψ grid generated set of conformations. Conformational clustering has been done to group the minimized conformations into families with similar values of glycosidic torsion angles. Several stable syn and anti conformations were found for the 1→2 and 1→3 bonds in the studied disaccharides. Vicinal glycosylation affected strongly the occupancy of conformational states in both branches of the title trisaccharide. The preferred conformational family of the trisaccharide (with average Φ,Ψ values of 38°, 17° for the 1→2 and 48°, 1° for the 1→3 bond, respectively) was shown by nmr to be stabilized by intramolecular hydrogen bonding between the nonbonded Rha and Gal residues. © 1998 John Wiley & Sons, Inc. Biopoly 46: 417–432, 1998     

Conformation of the glycotripeptide repeating unit of antifreeze glycoprotein of polar fish as determined from the fully assigned proton n.m.r. spectrum

With its simple glycotripeptide repeating structure the antifreeze glycoprotein of polar fish may be an especially simple conformational mode for mucin glycoproteins with similar but more complex structures. The fully assigned proton n.m.r. spectrum confirms the anomeric configurations of the hexapyranosidic sugars of the side chains and the coupling constants of the alpha GalNAc and the beta Gal residues show both to be in the expected 4C1 chair conformation. The assignment of a single resonance for each proton of the (Ala-Thr-Ala)n repeat unit coupled with the observation of long range nuclear Overhauser effects (n.O.e.) implies a three-fold repeating conformation. The resonances of the two alanines are distinct and can be assigned to their correct positions in the peptide sequence by n.O.e. observed at the amide proton resonances on saturation of the alpha proton signals. The amide proton coupling constants of all three peptide residues are similar and imply a limited range of peptide backbone torsion angles, phi CN. The large n.O.e. which has been observed between the amide proton and the alpha proton of the residue preceding it in the sequence implies large positive values for the peptide dihedral angle, psi CC. Limits are placed on possible values of side chain dihedral angles by the observation of the coupling constant between the alpha and beta protons of the threonyl residue. The observation of n.O.e. between the anomeric proton of GalNAc and the threonyl side chain protons gives information on the conformation of the alpha glycosidic linkage between the disaccharide and the peptide. n.O.e. observed between the protons of the beta glycosidic linkage indicates the conformation of the disaccharide and the large amide proton coupling constant of the GalNAc residue shows a trans proton relationship. The spectroscopically derived data have been combined with conformational energy calculations to give a conformational model for antifreeze glycoprotein in which the hydrophobic surfaces of the disaccharide side chains are wrapped closely against a three-fold left handed helical peptide backbone. The hydrophilic sides of the disaccharides are aligned so that they may bind to the ice crystal face, which is perpendicular to the fast growth axis inhibiting normal crystal growth.     

Conformations of blood group H-active oligosaccharides of ovarian cyst mucins

Spectroscopic data and conformational energy calculations are reported for eight oligosaccharides from ovarian cyst mucins and from human milk, the nonreducing terminals of which have fucose (α1 → 2)galactose linked either (β1 → 3) (type I) or (β1 → 4)(type II) to N-acetylglucosamine or in (β1 → 3) linkage to galactosaminitol. The fully assigned proton nmr spectra are reported along with nuclear Overhauser enhancement (NOE) data. Amide proton coupling constants and vacuum-uv CD spectra provide information on the amide plane orientation and amide environment. Our results imply that the fucosidic dihedral angles are similar for all three cases and that the substantial differences in the chemical shifts of the fucosyl protons of type I, type II, and 3-ol chains result from different perturbations by the amide group of the residue to which the β-galactose is linked. Stereopair diagrams of conformational models for both type I and II H chains are presented that are consistent with NOE, coupling constants, conformational energy calculations, and the CD data. While the temperature dependence of the observed NOE of penta- and hexasaccharides indicates that their rotational correlation times are strongly temperature dependent, we conclude that the conformations are essentially independent of temperature.     

Conformations of type 1 and type 2 oligosaccharides from ovarian cyst glycoprotein by nuclear Overhauser effect spectroscopy and T1 simulations.

To probe differences in conformation of the type 1 and type 2 linkages in blood group oligosaccharides, two-dimensional nuclear Overhauser effect spectroscopy (2D-NOESY) and 1H T1 data were obtained for two blood group A oligosaccharide alditols containing the type 1 and type 2 linkage. The NOE data were interpreted using a complete relaxation matrix approach. Simulations of NOE and T1 values were made using disaccharide and tetrasaccharide model conformations generated by a systemic variation of the glycosidic dihedral angles phi and psi. NOEs from the amide protons of GlcNAc and GalNAc in the type 1 pentasaccharide alditol were obtained, and simulated in a manner similar to those from carbon-bound protons. In addition to providing data for determining the conformation of the type 1 linkage from amide proton NOEs of GlcNAc and GalNAc to neighboring residues, amide proton NOEs also yield information on the orientation of the acetamido side chains. The amide NOE data indicated subtle differences in the orientation of the amide side chain of GlcNAc among the A type 1 pentasaccharide alditol and two previously studied blood group oligosaccharides, lacto-N-difucohexaose 1 and lacto-N-fucopentaose 1. From the NOE and 1H T1 data, and from simple rigid geometry energy calculations, it is concluded that the type 1 and type 2 linkages in the oligosaccharides studied have different conformations and that these conformations are relatively rigid in solution.     

A kinetic description of antifreeze glycoprotein activity

The antifreeze glycoproteins (AFGP) of polar fish have the ability to depress the freezing temperature of water approximately 500 times the amount expected based on the number of AFGP molecules in solution; yet AFGP solutions have a purely colligative melting point depression. The difference of solution melting and freezing temperatures is the antifreeze activity of AFGP. One characteristic of AFGP activity that requires further examination is the effect of concentration on antifreeze activity, especially whether the activity saturates at high concentrations or the measured activity increases ad infinitum. This study first surveys the activity of the various antifreeze components from both Pagothenia borchgrevinki and the Arg-containing antifreeze glycoprotein from Eleginus gracilis (EgAF). It was found that all AFGP components examined have a plateau in activity at high concentration, but the actual value of the plateau activity differs between the different length AFGP components and between AFGP and EgAF. While the low molecular weight components of both AFGP and EgAF lose activity at deep supercooling, at high concentration activity is restored. The activity data is then shown to fit a reversible kinetic model of AFGP activity, and the coefficients obtained are used to compare the activity differences between AFGP components and between AFGP and EgAF. The model is also shown to describe the activity of the antifreeze protein of the fish Pseudopleuronectes americanus and the thermal hysteresis protein of the insect, Tenebrio molitor.     

Use of proton Nuclear Overhauser Effects for the determination of the conformations of amino acid residues in oligopeptides

The use of the Nuclear Overhauser Effect to determine backbone and side-chain conformations of oligopeptides is discussed. The distance between the H^α proton of a given residue and the amide proton of the following residue depends only on the dihedral angle ψ. A calibration curve is given for the determination of ψ from the Nuclear Overhauser Effect involving these protons. In amino acids with branched side chains, e.g., threonine, isoleucine, and valine, the Nuclear Overhauser Effect involving the H^β proton and the amide proton in either the same or the following residue gives limited information about both χ¹ and either or ψ. The Nuclear Overhauser Effect involving the H^α and H^γ protons in leucine gives information about χ¹ and χ².     

Conformation of the oligosaccharide receptor for E-selectin

A tetrasaccharide related to the blood group oligosaccharides, known as sialyl Lewis^X, has been proposed as the receptor for the lectin responsible for leukocyte adhesion named alternatively as E-selectin or ELAM-1. The ¹³C- and ¹H-nmr spectra have been completely assigned for a tetrasaccharide model of this receptor, Neu5Ac α-(2 → 3)-Gal β-(1 → 4)-[ Fuc α-(1 → 3)-] GlcNAc β-NHAc. Quantitative nuclear Overhauser data (NOESY) have been recorded and analyzed by a complete spin matrix simulation method. Conformational space was exhaustively searched and all conformational models whose simulated NOESY spectra matched the experiment were found. Molecular mechanics and molecular dynamics calculations were carried out to test whether the experimental conformations are low energy and thus likely to represent true single conformations for the tetrasaccharide. It was concluded that while the Lewis^X trisaccharide portion of the compound adopts a single conformation, there is likely to be some flexibility about the Neu5Ac α-(2 → 3)-linkage. A model featuring fast exchange between two different conformations of this linkage is found to be consistent with both the nmr experiments and the molecular dynamics simulations. © 1994 John Wiley & Sons, Inc.     

The ruminant parasite Haemonchus contortus expresses an α1,3-fucosyltransferase capable of synthesizing the Lewis x and sialyl Lewis x antigens

Glycoproteins from the ruminant helminthic parasite Haemonchus contortus react with Lotus tetragonolobus agglutinin and Wisteria floribunda agglutinin, which are plant lectins that recognize α1,3-fucosylated GlcNAc and terminal β-GalNAc residues, respectively. However, parasite glycoconjugates are not reactive with Ricinus communis agglutinin, which binds to terminal β-Gal, and the glycoconjugates lack the Lewis x (Lex) antigen or other related fucose-containing antigens, such as sialylated Lex, Lea, Leb Ley, or H-type 1. Direct assays of parasite extracts demonstrate the presence of an α1,3-fucosyltransferase (α1,3FT) and β1,4-N-acetylgalactosaminyltransferase (β1,4GalNAcT), but not β1,4-galactosyltransferase. The H. contortus α1,3FT can fucosylate GlcNAc residues in both lacto-N-neotetraose (LNnT) Galα1→4GlcNAcβ1→3Galβ1→4Glc to form lacto-N-fucopentaose III Galβ1→ 4[Fucα1→3]GlcNAcβ1→3Galβ1→4Glc, which contains the Lex antigen, and the acceptor lacdiNAc (LDN) GalNAcβ1→4GlcNAc to form GalNAcβ1→4[Fucα1 →3]GlcNAc. The α1,3FT activity towards LNnT is dependent on time, protein, and GDP-Fuc concentration with a Km 50 μ M and a Vmax of 10.8 nmol-mg?1 h?1. The enzyme is unusually resistant to inhibition by the sulfhydryl-modifying reagent N-ethylmaleimide. The α1,3FT acts best with type-2 glycan acceptors (Galβ1→4GlcNAcβ1-R) and can use both sialylated and non-sialylated acceptors. Thus, although in vitro the H. contortus α1,3FT can synthesize the Lex antigen, in vivo the enzyme may instead participate in synthesis of fucosylated LDN or related structures, as found in other helminths.     

The isolation and the structure of new glycopeptide from blood group substances

Three new glycopeptides with O-glycosidic and one glycopeptide with N-glycosylaminic carbohydrate-peptide linkages have been isolated after degradation of blood group substances (BGS). Their structure have been determined as O-(α-GalNAc)-Ser(I), O-(GalNAc)-(Pro)-Ser(II), O-(GalNAc 1 → 3 GalNAc)-(Thr-Ala)-Ser(III), N-(β-GlcNAc)-Asn(IV). The isolation of glycopeptide I confirmed α-configuration of O-glycosidic carbohydrate-peptide bonds. The structure of glycopeptide III with two galactosamine residues is in accordance with the data on the presence of hexosamine core of BGS carbohydrate chains.     

Comparison of the solution conformation and dynamics of antifreeze glycoproteins from Antarctic fish

The (1)H- and (13)C-NMR spectra of antifreeze glycoprotein fractions 1-5 from Antarctic cod have been assigned, and the dynamics have been measured using (13)C relaxation at two temperatures. The chemical shifts and absence of non-sequential (1)H-(1)H NOEs are inconsistent with a folded, compact structure. (13)C relaxation measurements show that the protein has no significant long-range order, and that the local correlation times are adequately described by a random coil model. Hydroxyl protons of the sugar residues were observed at low temperature, and the presence of exchange-mediated ROEs to the sugar indicate extensive hydration. The conformational properties of AFGP1-5 are compared with those of the previously examined 14-mer analog AFGP8, which contains proline residues in place of some alanine residues (Lane, A. N., L. M. Hays, R. E. Feeney, L. M. Crowe, and J. H. Crowe. 1998. Protein Sci. 7:1555-1563). The infrared (IR) spectra of AFGP8 and AFGP1-5 in the amide I region are quite different. The presence of a wide distribution of backbone torsion angles in AFGP1-5 leads to a rich spectrum of frequencies in the IR spectrum, as interconversion among conformational states is slow on the IR frequency time scale. However, these transitions are fast on the NMR chemical shift time scales. The restricted motions for AFGP8 may imply a narrower distribution of possible o, psi angles, as is observed in the IR spectrum. This has significance for attempts to quantify secondary structures of proteins by IR in the presence of extensive loops.     

Conformational properties of poly[d(G-T)].poly[d(C-A)] and poly[d(A-T)] in low- and high-salt solutions: NMR and laser Raman analysis

³¹P- and ¹H-nmr and laser Raman spectra have been obtained for poly[d(G-T)]·[d(C-A)] and poly[d(A-T)] as a function of both temperature and salt. The ³¹P spectrum of poly[d(G-T)]·[d(C-A)] appears as a quadruplet whose resonances undergo separation upon addition of CsCl to 5.5M. ¹H-nmr measurements are assigned and reported as a function of temperature and CsCl concentration. One dimensional nuclear Overhauser effect (NOE) difference spectra are also reported for poly[d(G-T)]·[d(C-A)] at low salt. NOE enhancements between the H8 protons of the purines and the C5 protons of the pyrimidines, (H and CH₃) and between the base and H-2′,2″ protons indicate a right-handed B-DNA conformation for this polymer. The NOE patterns for the TH3 and GH1 protons in H₂O indicate a Watson–Crick hydrogen-bonding scheme. At high CsCl concentrations there are upfield shifts for selected sugar protons and the AH2 proton. In addition, laser Raman spectra for poly[d(A-T)] and poly[d(G-T)]·[d(C-A)] indicate B-type conformations in low and high CsCl, with predominantly C2′-endo sugar conformations for both polymers. Also, changes in base-ring vibrations indicate that Cs⁺ binds to O2 of thymine and possibly N3 of adenine in poly[d(G-T)]·[d(C-A)] but not in poly[d(A-T)]. Further, ¹H measurements are reported for poly[d(A-T)] as a function of temperature in high CsCl concentrations. On going to high CsCl there are selective upfield shifts, with the most dramatic being observed for TH1′. At high temperature some of the protons undergo severe changes in linewidths. Those protons that undergo the largest upfield shifts also undergo the most dramatic changes in linewidths. In particular TH1′, TCH₃, AH1′, AH2, and TH6 all undergo large changes in linewidths, whereas AH8 and all the H-2′,2″ protons remain essentially constant. The maximum linewidth occurs at the same temperature for all protons (65°C). This transition does not occur for d(G-T)·d(C-A) at 65°C or at any other temperature studied. These changes are cooperative in nature and can be rationalized as a temperature-induced equilibrium between bound and unbound Cs⁺, with duplex and single-stranded DNA. NOE measurements for poly[d(A-T)] indicate that at high Cs⁺ the polymer is in a right-handed B-conformation. Assignments and NOE effects for the low-salt ¹H spectra of poly[d(A-T)] agree with those of Assa-Munt and Kearns [(1984) Biochemistry 23 , 791–796] and provide a basis for analysis of the high Cs⁺ spectra. These results indicate that both polymers adopt a B-type conformation in both low and high salt. However, a significant variation is the ability of the phosphate backbone to adopt a repeat dependent upon the base sequence. This feature is common to poly[d(G-T)]·[d(C-A)], poly[d(A-T)], and some other pyr–pur polymers [J. S. Cohen, J. B. Wouten & C. L Chatterjee (1981) Biochemistry 20 , 3049–3055] but not poly[d(G-C)].     

3d haro-Noesy-ch3nh and caro-Noesy-ch3nh Experiments for Double Labeled Proteins

Precision in the determination of the 3D structures of proteins by NMR depends on obtaining an adequate number of NOE restraints. Ambiguity in the assignment of NOE cross peaks between aromatic and other protons is an impediment to high quality structure determination. Two pulse sequences, 3D H_aro-NOESY-CH₃NH and 3D C_aro-NOESY-CH₃NH, based on a modification of a technique for simultaneous detection of ¹³C-¹H (of CH₃) and ¹⁵N-¹H correlations in one measurement, are proposed in the present work. These 3D experiments, which are optimized for resolution in the ¹³C and ¹⁵N dimensions, provide NOE information between aromatic protons and methyl or amide protons. CH₂ moieties are filtered out and the CH groups in aromatic rings are selected, allowing their NOE cross peaks to be unambiguously assigned. Unambiguous NOEs connecting aromatic and methyl or amide protons will provide important restraints for protein structure calculations.     

A serendipitous discovery of antifreeze protein-specific activity in C-linked antifreeze glycoprotein analogs

Structurally diverse carbon-linked (C-linked) analogs of antifreeze glycoprotein (AFGP) have been prepared via linear or convergent solid phase synthesis. These analogs range in molecular weight from approx 1.5–4.1 KDa and do not possess the β-d-galactose-1,3-α-d-N-acetylgalactosamine carbohydrate moiety or the l-threonine-l-alanine-l-alanine polypeptide backbone native to the AFGP wild-type. Despite these dramatic structural modifications, the 2.7-KDa and 4.1-KDa analogs possess antifreeze protein-specific activity as determined by recrystallization-inhibition (RI) and thermal hysteresis (TH) assays. These analogs are weaker than the wild-type in their activity, but nanoliter osmometry indicates that these compounds are binding to ice and affecting a localized freezing point depression. This is the first example of a C-linked AFGP analog that possesses TH and RI activity and suggests that the rational design and synthesis of chemically and biologically stable AFGP analogs is a feasible and worthwhile endeavor. Given the low degree of TH activity, these compounds may prove useful for the protection of cells during freezing and thawing cycles.     

Evidence for a gamma-turn motif in antifreeze glycopeptides.

Knowledge of the secondary structure of antifreeze peptides (AFPs) and glycopeptides (AFGPs) is crucial to understanding the mechanism by which these molecules inhibit ice crystal growth. A polyproline type II helix is perhaps the most widely accepted conformation for active AFGPs; however, random coil and alpha-helix conformations have also been proposed. In this report we present vibrational spectroscopic evidence that the conformation of AFGPs in solution is not random, not alpha-helical, and not polyproline type II. Comparison of AFGP amide vibrational frequencies with those observed and calculated for beta and gamma-turns in other peptides strongly suggests that AFGPs contain substantial turn structure. Computer-generated molecular models were utilized to compare gamma-turn, beta-turn, and polyproline II structures. The gamma-turn motif is consistent with observed amide frequencies and results in a molecule with planar symmetry with respect to the disaccharides. This intriguing conformation may provide new insight into the unusual properties of AFGPs.     

Conformational analysis of polyoxyethylene-bound homo-oligo-L-glutamates in aqueous environment

A detailed conformational analysis of homo-oligo-L -glutamates was carried out in aqueous solution using ¹H-nmr spectroscopy. Three series of side-chain protected (α-OMe) glutamate oligopeptides, attached to polyoxyethylene (POE) to enhance their solubility, were synthesized. The effect of the N-terminal blocking groups—Boc, Ac, and pGlu—on the conformations of these peptides in water is discussed. Unequivocal assignments were obtained for all amide NH resonances through use of selectively α-deuterated oligo-glutamates. Analysis of vicinal coupling constants, temperature dependence of NH chemical shifts, transfer of saturation experiments, and titration studies with a denaturing solvent (DMSO) were used to investigate the peptide structure. These data suggest that the Glu¹ and Glu² NH protons of each heptamer are solvent exposed, while the NH protons of interior glutamate residues chain are solvent sequestered. The nmr data are consistent with the onset of helical structure at the heptamer of each series in aqueous solution. The POE-peptides with pGlu at the N-terminus showed considerably reduced stability of structure than those with the Boc or acetyl blocking groups. Peptide conformations and their stability in water are compared to those in other solvents.     

Structure of human salivary histatin 5 in aqueous and nonaqueous solutions

The solution structure of human salivary histatin 5 (D-S-H-A-K-R-H-H-G-Y-K-R-K-F-H-E-K-H-H-S-H-R-G-Y) was examined in water (pH 3.8) and dimethyl sulfoxide solutions using 500 MHz homo- and heteronuclear two-dimensional (2D) nmr. The resonance assignment of peptide backbone and side-chain protons was accomplished by 2D total correlated spectroscopy and nuclear Overhauser effect (NOE) spectroscopy. The high J values (≥7.4 Hz), absence of any characteristic NH-NH(i, i + 1) or C^αH-C^βH(i, i + 3) NOE connectivities, high dδ/dT values (≥0.004 ppm K⁻¹) and the fast ¹H/²H amide exchange suggest that histatin 5 molecules remain unstructured in aqueous solution at pH 3.8. In contrast, histatin 5 prefers largely α-helical conformation in dimethyl sulfoxide solution as evident from the J values (≤6.4 Hz), slow ¹H/²H exchange, low dδ/dT values (≤0.003 ppm K⁻¹) observed for amide resonances of residues 6–24, and the characteristic NH-NH(i, i + 1) and C^αH-C^βH(i, i +3) NOE connectivities. All backbone amide ¹⁵N-¹H connectivities fall within 6 ppm on the ¹⁵N scale in the 2D heteronuclear single quantum correlated spectrum, and the restrained structure calculations using DIANA suggest the prevalence of α-helical conformations stabilized by 19 (5 → 1) intramolecular backbone amide hydrogen bonds in polar aprotic medium such as dimethyl sulfoxide. The interside-chain hydrogen bonding and salt-bridge type interactions that normally stabilize the helical structure of linear peptides in aqueous solutions are not observed. Histatin 5, unlike other naturally occurring antimicrobial polypeptides such as magainins, defensins, and tachyplesins, does not adopt amphiphilic structure, precluding its insertion into microbial membranes and formation of ion channels across membranes. Electrostatic (ionic type) and hydrogen bonding interactions of the positively charged and polar residues with the head groups of microbial membranes or with a membrane-bound receptor could be the initial step involved in the mechanism of antimicrobial activity of histatins. © 1998 John Wiley & Sons, Inc. Biopoly 45: 51–67, 1998     

Adsorption to ice of fish antifreeze glycopeptides 7 and 8.

Experimental results show that fish antifreeze glycopeptides (AFGPs) 8 and 7 (with 4 and 5 repeats respectively of the Ala-Ala-Thr backbone sequence) bond onto ice prism planes aligned along a-axes, and inhibit crystal growth on prism planes and on surfaces close to that orientation. The 9.31-A repeat spacing of the AFGP in the polyproline II helix configuration, deduced from NMR studies, matches twice the repeat spacing of ice in the deduced alignment direction, 9.038 A, within 3%. A specific binding model is proposed for the AFGP and for the alpha-helical antifreeze peptide of winter flounder. For AFGP 7-8, two hydroxyl groups of each disaccharide (one disaccharide is attached to each threonine) reside within the ice surface, so that they are shared between the ice crystal and the disaccharide. This provides 24 hydrogen bonds between AFGP 8 and the ice and 30 for AFGP 7, explaining why the chemical adsorption is virtually irreversible and the crystal growth can be stopped virtually completely. The same scheme of sharing polar groups with the ice works well with the alpha-helical antifreeze of winter flounder, for which an amide as well as several hydroxyls are shared. The sharing of polar groups with the ice crystal, rather than hydrogen-bonding to the ice surface, may be a general requirement for adsoprtion-inhibition of freezing.     

Antifreeze glycoproteins: influence of polymer length and ice crystal habit on activity

The effect of the ice crystalline habit and the length of the polymer on the ability of the antifreeze glycoproteins (AFGP) from polar fish to depress the freezing temperature of water was investigated. The low-molecular-weight components of the glycoproteins, AFGP- 6–8, are inactive when a solution of such a sample is nucleated at ?6°C. A solution of large AFGP (1–4) is fully functional under the same conditions. The low-molecular-weight components differ from the height-molecular-weight components in that they contain some proline replacing the alanine in the Ala-Ala-Thr · disaccharide polymer unit. In the present experiments, antifreeze activity was examined in the presence of two different forms of ice crystal growth habits, and homodimders of AFGP 6 and 8 were prepared to investigate the function of polymer length and the on antifreeze activity at different degrees of supercooling. The results indicate that the ice crystal growth habit and the introduction of proline into the polymer unit may be responsible for the loss of activity at deep supercooling (?6°C) of AFGP 6–8. The loss in the ability of AFGP to depress the freezing temperature of water at deep supercooling is not solely due to polymer length, as carbodiimide-linked dimers of AFGP 6 do not function under these freezing conditions. A Model of antifreezing action based on Langmuirian adsorption of AFGP on the ice surface and direct competition between water and AFGP molecules for the incorporation sites in the ice crystal lattice is presented.