Synthesis and characterization of an ionizable polyhexapeptide collagen model

Poly(Lys(HBr)-Gly-Pro-Pro-Gly-Pro) has been synthesized and studied by circular dichroism (CD) spectroscopy. It is apparently the first polyhexapeptide collagen model reported with an ionizable side chain. The monomer (ε-(p-nitrobenzyloxycarbonyl)-Lys-Gly-Pro-Pro-Gly-Pro-p-nitrophenyl-ester) was prepared by a stepwise strategy employing active esters. Polymerization in N,N-dimethyl formamide, followed by removal of the Lys side chain protection with HBr/acetic acid, gave a polydisperse product. Fractionation was accomplished by gel filtration chromatography. The polydisperse material had a molecular weight (M_r = 5–17,000). High molecular weight fractions from triple helices under concentrated conditions at 2°C. The triple helical structure gives a CD pattern very similar to that of collagen and its triple helical analogs. However, unlike collagen, the polyhexapeptide undergoes spontaneous dissociation at temperatures substantially below the melting temperature from a triple helical form to single chains. This process is promoted at low concentrations, high temperature, neutral pH, and low molecular weight, and is apparently due, in large part, to unfavorable ionic side-chain interactions. In addition to this relatively slow “ionic” dissociation the triple helical polypeptide may be thermally dissociated in a manner similar to collagen. The thermal denaturation is a relatively fast process compared with ionic dissociation. A high molecular weight fraction (3 × M_r = 48,000) was found to melt at 42°C at neutral pH but increased to 54°C at pH 12 where the lysyl side chains are predominantly deprotonated. Furthermore, reconstitution of triple helices appeared to be more readily achieved at high pH. Thus it is concluded that ionic repulsion between side chains causes destabilization of the triple helix and hinders reconstitution.     

The Contribution of Interchain Salt Bridges to Triple-Helical Stability in Collagen

Studies on collagen and collagen-like peptides suggest that triple-helical stability can vary along the amino acid chain. In this regard, it has been shown that lysine residues in the Y position and acidic residues in the X′ position of (GPO)₃GXYGX′Y′(GPO)₃ peptides lead to triple-helical structures with melting temperatures similar to (GPO)₈ (where O is hydroxyproline), which is generally regarded as the most stable collagen-like sequence of this length. This enhanced stability has been attributed to the formation of salt bridges between adjacent collagen chains. In this study, we explore the relationship between interchain salt bridge formation and triple-helical stability using detailed molecular simulations. Although our results confirm that salt bridges promote triple-helical stability, we find that not all salt bridges are created equal. In particular, lysine-glutamate salt bridges are most stabilizing when formed between residues in the middle strand (B) and the trailing strand (C), whereas lysine-aspartate salt bridges are most stabilizing when formed between residues in the leading (A) and middle (B) strand—the latter observation being consistent with recent NMR data on a heterotrimeric model peptide. Overall, we believe these data clarify the role of salt bridges in modulating triple-helical stability and can be used to guide the design of collagen-like peptides that have specific interchain interactions.     

The triple helix ⇌ coil conversion of collagen-like polytripeptides in aqueous and nonaqueous solvents. Comparison of the thermodynamic parameters and the binding of water to (L-Pro-L-Pro-Gly)n and (L-Pro-L-Hyp-Gly)n

The collagen-like peptides (L -Pro-L -Pro-Gly)_n and (L -Pro-L -Hyp-Gly)_n with n = 5 and 10, were examined in terms of their triple helix ? coil transitions in aqueous and nonaqueous solvents. The peptides were soluble in 1,2-propanediol containing 3% acetic acid and they were found to form triple-helical structures in this solvent system. The water content of the solvent system and the amount of water bound to the peptides were assayed by equilibrating the solvent with molecular sieves and carrying out Karl Fischer titrations on the solvent phase. After the solvent was dehydrated, much less than one molecule of water per tripeptide unit was bound to the peptides. Since the peptides remained in a triple-helical conformation, the results indicated that water was not an essential component of the triple-helical structure. Comparison of peptides with the same chain length demonstrated that the presence of hydroxyproline increased the thermal stability of the triple helix even under anhydrous conditions. The results, therefore, did not support recent hypotheses that hydroxyproline stabilizes the triple helix of collagen and collagen-like peptides by a specific interaction with water molecules. Analysis of the thermal transition curves in several solvent systems showed that although the peptides containing hydroxyproline had t_m values which were 18.6° to 32.7°C higher, the effect of hydroxyproline on ΔG was only 0.1 to 0.3 kcal per tripeptide unit at 25°C. The results suggested, therefore, that the influence of hydroxyproline on helical stability may be explained by intrinsic effects such as dipole–dipole interactions or by changes in the solvation of the peptides by alcohol, acetic acid, and water. A direct calorimetric measurement of the transition enthalpy for (L -Pro-L -Pro-Gly)_n in 3% or 10% acetic acid gave a value of ?1.84 kcal per tripeptide unit for the coil-to-helix transition. From the value for enthalpy and from data on the effects of different chain lengths on the thermal transition, it was calculated that the apparent free energy for nucleation was +5 kcal/mol at 25°C (apparent nucleation parameter = 2 × 10^?4 M^?2). The value was dependent on solvent and on chemical modification of end groups.     

An energetic evaluation of a "Smith" collagen microfibril model.

An energy minimized three-dimensional structure of a collagen microfibril template was constructed based on the five-stranded model of Smith (1968), using molecular modeling methods and Kollman force fields (Weiner and Kollman, 1981). For this model, individual molecules were constructed with three identical polypeptide chains ((Gly-Pro-Pro) _n , (Gly-Prop-Hyp) _n , or (Gly-Ala-Ala) _n , wheren=4, 12, and 16) coiled into a right-handed triple-helical structure. The axial distance between adjacent amino acid residues is about 0.29 nm per polypeptide chain, and the pitch of each chain is approximately 3.3 residues. The microfibril model consists of five parallel triple helices packed so that a left-handed superhelical twist exists. The structural characteristics of the computed microfibril are consistent with those obtained for collagen by X-ray diffraction and electron microscopy. The energy minimized Smith microfibril model for (Gly-Pro-Pro)₁₂ has an axial length of about 10.2 nm (for a 36 amino acid residue chain), which gives an estimated D-spacing (234 amino acids per chain) of approximately 66.2 nm. Studies of the microfibril models (Gly-Pro-Pro)₁₂, (Gly-Pro-Hyp)₁₂, and (Gly-Ala-Ala)₁₂ show that nonbonded van der Waals interactions are important for microfibril formation, while electrostatic interactions contribute to the stability of the microfibril structure and determine the specificity by which collagen molecules pack within the microfibril.     

Variable chain conformations of renatured β‐glucan in dimethylsulfoxide/water mixture

We have firstly demonstrated the renaturation process of dissociated single chains of lentinan (s‐LNT) and the variable conformations of the renatured LNT (r‐LNT). The results from ultrasensitive differential scanning calorimetry and circular dichroism revealed that the variable structures including perfect triple helix, defective triple helix containing duplex segment, and single chains occurred in the renaturation of s‐LNT, depending on the renaturation time, solvent composition, molecular weight, and the mode of renaturation. When water was added into s‐LNT/dimethylsulfoxide (DMSO) to reach 95% (v/v), the classic low‐temperature intra‐triple‐helical conformational transition at ～10^°C (T₁) appeared within 4 h, indicative of a rapid reconstruction of triple helical structure. Besides, one newly endothermic peak at ～43^°C (T₂) simultaneously occurred, which was first ascribed to the melting of duplex segment in the imperfect triplex. The duplex stretches disappeared when DMSO reached 50%, in which single chains coexisted with triplex. Moreover, the duplex segment disappeared by slowly dropping water into s‐LNT/DMSO. This work suggested that the structure of r‐LNT could be controllable, and provided important information for their successful development and application in polymer and life science. © 2012 Wiley Periodicals, Inc. Biopolymers 97:988–997, 2012.     

A theoretical study of the structures of (Gly-Pro-Leu)n and (Gly-Leu-Pro)n

Theoretical conformation studies have been carried out for the polytripeptides (Gly-Pro-Leu)n and (Gly-Leu-Pro)n and the Fourier transforms of the structures have been calculated. X-ray powder patterns of these polymers had indicated that both these polymers take up coiled-coil triple-helical structures, but in the case of (Gly-Pro-Leu)n it was not clear whether the triple helix is formed by three parallel polypeptide chains or by a single chain folding back on itself (Scatturin et al 1975). Our studies show that both the polytripeptides can take up stereochemically satisfactory triple-helical structures with three parallel chains. There is also very good agreement between the calculated intensity distribution and that of the observed X-ray pattern, in each case.     

Mechanism of collagen folding propagation studied by Molecular Dynamics simulations

Collagen forms a characteristic triple helical structure and plays a central role for stabilizing the extra-cellular matrix. After a C-terminal nucleus formation folding proceeds to form long triple-helical fibers. The molecular details of triple helix folding process is of central importance for an understanding of several human diseases associated with misfolded or unstable collagen fibrils. However, the folding propagation is too rapid to be studied by experimental high resolution techniques. We employed multiple Molecular Dynamics simulations starting from unfolded peptides with an already formed nucleus to successfully follow the folding propagation in atomic detail. The triple helix folding was found to propagate involving first two chains forming a short transient template. Secondly, three residues of the third chain fold on this template with an overall mean propagation of ~75 ns per unit. The formation of loops with multiples of the repeating unit was found as a characteristic misfolding event especially when starting from an unstable nucleus. Central Gly→Ala or Gly→Thr substitutions resulted in reduced stability and folding rates due to structural deformations interfering with folding propagation.     

The formation of the triple helix in a mixed solution of (Pro-Pro-Gly)n and (Pro-Pro-Gly)n'. A model of molecular size recognition

A theoretical analysis is given of the triple-helix–random-coil transition in a mixed solution of poly(Pro-Pro-Gly)_n with two different but defined degrees of polymerization n and n′. Because of the highly cooperative nature of this helix–coil transition, each polypeptide chain tends to form a triple helix with other polypeptide chains with the same degree of polymerization (size recognition). Occurrence of triple helices consisting of polypeptide chains with different degrees of polymerization (error in recognition) is studied in detail as a function of the cooperativity, and n and n′. Implication of this analysis for molecular recognition in general is discussed.     

Cooperative nonenzymic base recognition II. thermodynamics of the helix-coil transition of oligoadenylic + oligouridylic acids

The properties of oligonucleotide helices of adeuylic- and uridylic acid oligomers have been investigated by measurements of hypo-and hyperchromieity. High ionic strengths favor the formation of triple helices. Thus, the double helix-coil transition can be studied (without interference by triple helices) only at low ionic-strength. A “phase diagram” is given representing the T_m-values of the various transitions at different ionic strengths for the system A(pA)₁₇ + U(pU)₁₇. Oligonucleolides of chain lengths <8 always form both double and triple helices at the nucleotide concentrations required for base pairing. For this reason the double helix-coil transition without coupling of the triple helix equilibrium can only be measured for chain lengths higher than 7. Melting curves corresponding to this transition have been determined for chain lengths 8, 9, 10, 11, 14 and 18 at different concentrations. An increase in nucleotide concentration leads to an increase in melting temperature. The shorter the chain length the lower the T_m-value and the broader the helix-coil transition. The experimental transition curves have been analysed according to a staggering zipper model with consideration of the stacking of the adeuylic acid single strands and the electrostatic repulsion of tlip phosphate charges on opposite strands. The temperature dependence of the nucleation parameter has been accounted for by a slacking factor x. The stacking factor expresses the magnitude of the stacking enthalpy. By curve fitting xwas computed to be 0.7, corresponding to a stacking enthalpy of about S kcal/mole. The model described allows the reproduction of the experimental transition curves with relatively high accuracy. In an appendix the thermodynamic parameters of the stacking equilibrium of poly A and of the helix-coil equilibria of poly A + poly U at neutral pH are calculated (ΔH_A = ?7.9 kcal/mole for the poly A stacking and ΔH₁₂ = ?10.9 kcal/mole for the formation of the double helix from the randomly coiled single strands). A formula for the configurational entropy of polymers derived by Flory on the basis of a liquid lattice model is adapted to calculate the stacking entropies of adenylic oligomers.     

Conformational change of the triple-helical structure. II. Conformation of (Pro-Pro-Gly)n and (Pro-Pro-Gly)n (Ala-Pro-Gly)m(Pro-Pro-Pro-Gly)n in an aqueous solution

Measurements of the molecular weight of (Pro-Pro-Gly)_n and (Pro-Pro-Gly)_n(Ala-Pro-Gly)_m(Pro-Pro-Gly)_n, which were synthesized by the solid-phase method, revealed that they formed a trimer in an aqueous solution, and dissociated into single-stranded chains on warming. Accompanying the transition, a large decrease of optical rotation was observed, like the collagen–gelatin transition. The shape of the trimeric molecule was rodlike, and the dimensions were 12 Å in diameter and 2.8 Å per residue in length, regardless of the length of Ala-Pro-Gly sequences in a peptide chain. The data indicate that both Pro-Pro-Gly sequences and Ala-Pro-Gly sequences from the triple-helical structure similar to that of collagen in aqueous solution. All optical rotational dispersion (ORD) curves of solutions of the peptides were represented by a single-term Drude equation, and the Drude constant λ_c was 200 nm for all peptides regardless of the length of Ala-Pro-Gly sequences. The resemblance between the helical structure formed by Pro-Pro-Gly sequences and that by Ala-Pro-Gly sequences was also suggested by the formation of the hybrid triple helix from two kinds of peptide chains with different lengths of Ala-Pro-Gly sequences.     

Template-assembled triple-helical peptide molecules: mimicry of collagen by molecular architecture and integrin-specific cell adhesion

Most proteins fold into specific structures to exert their biological functions, and therefore the creation of protein-like molecular architecture is a fundamental prerequisite toward realizing a novel biologically active protein-like biomaterial. To do this with an artificial collagen, we have engineered a peptide template characterized by its collagen-like primary structure composed of Gly-Phe-Gly-Glu-Glu-Gly sequence to assemble (Pro-Hyp-Gly)n (n = 3 and 5) into triple-helical conformations that resemble the native structure of collagen. The peptide template has three carboxyl groups connected to the N-termini of three collagen peptides. The coupling was accomplished by a simple and direct branching protocol without complex strategies. A series of biophysical studies, including melting curve analyses and CD and NMR spectroscopy, demonstrated the presence of stable triple-helical conformation in the template-assembled (Pro-Hyp-Gly)3 and (Pro-Hyp-Gly)5 solution. Conversely, nontemplated peptides showed no evidence of assembly of triple-helical structure. A cell binding sequence (Gly-Phe-Hyp-Gly-Glu-Arg) derived from the collagen alpha1(I) chain was incorporated to mimic the integrin-specific cell adhesion of collagen. Cell adhesion and inhibition assays and immunofluorescence staining revealed a correlation of triple-helical conformation with cellular recognition of collagen mimetics in an integrin-specific way. This study offers a robust strategy for engineering native-like peptide-based biomaterials, fully composed of only amino acids, by maintaining protein conformation integrity and biological activity.     

Template‐tethered collagen mimetic peptides for studying heterotrimeric triple‐helical interactions

Collagen mimetic peptides (CMPs) have been used to elucidate the structure and stability of the triple helical conformation of collagen molecules. Although CMP homotrimers have been widely studied, very little work has been reported regarding CMP heterotrimers because of synthetic difficulties. Here, we present the synthesis and characterization of homotrimers and ABB type heterotrimers comprising natural and synthetic CMP sequences that are covalently tethered to a template, a tris(2‐aminoethyl) amine (TREN) succinic acid derivative. Various tethered heterotrimers comprising synthetic CMPs [(ProHypGly)₆, (ProProGly)₆] and CMPs representing specific domains of type I collagen were synthesized and characterized in terms of triple helical structure, thermal melting behavior, and refolding kinetics. The results indicated that CMPs derived from natural type I collagen sequence can form stable heterotrimeric helical complexes with artificial CMPs and that the thermal stability and the folding rate increase with the increasing number of helical stabilizing amino acids (e.g. Hyp) in the peptide chains. Covalent tethering enhanced the thermal stability and refolding kinetics of all CMPs; however, their relative values were not affected suggesting that the tethered system can be used for comparative study of heterotrimeric CMP's folding behavior in regards to chain composition and for characterization of thermally unstable CMPs. © 2010 Wiley Periodicals, Inc. Biopolymers 95: 94–104, 2011.     

Synthesis and physical properties of (hydroxyproline-proline-glycine)10: Hydroxyproline in the X-position decreases the melting temperature of the collagen triple helix

The collagen-like polytripeptide (hydroxyproline-proline-glycine)₁₀ was synthesized with a solid-phase procedure. Analytical ultracentrifugation indicated that the peptide in aqueous solution at 6 °C had a molecular weight of 2550, the expected size of a single chain. The peptide had a relatively small negative optical rotation at 578 nm, and it did not show a thermal transition as is seen with collagen or collagen-like polytripeptides which form triple helices. At low temperatures in aqueous solution, the circular dichroism spectrum was similar to that of triple-helical collagen and collagen-like peptides in that there was a positive peak at 224 nm and a negative peak at 200 nm. The amplitudes of the peaks, however, were considerably less than the peaks obtained with triple-helix proteins and peptides. Since (proline-proline-glycine)₁₀ was triple helical under the same conditions, the results demonstrated that hydroxyproline in the X-position of the repeating -glycine-X-Y- sequences decreases rather than increases, the thermal stability of the triple helix. This positional specificity cannot be explained by any of the current models for the structure of the triple helix or any of the current proposals for how hydroxyproline stabilizes the structure.     

Streptococcal Scl1 and Scl2 proteins form collagen-like triple helices

The collagens are a family of animal proteins containing segments of repeated Gly-Xaa-Yaa (GXY) motifs that form a characteristic triple-helical structure. Genes encoding proteins with repeated GXY motifs have also been reported in bacteria and phages; however, it is unclear whether these prokaryotic proteins can form a collagen-like triple-helical structure. Here we used two recently identified streptococcal proteins, Scl1 and Scl2, containing extended GXY sequence repeats as model proteins. First we observed that prior to heat denaturation recombinant Scl proteins migrated as homotrimers in gel electrophoresis with and without SDS. We next showed that the collagen-like domain of Scl is resistant to proteolysis by trypsin. We further showed that circular dichroism spectra of the Scl proteins contained features characteristic of collagen triple helices, including a positive maximum of ellipticity at 220 nm. Furthermore the triple helices of Scl1 and Scl2 showed a temperature-dependent unfolding with melting temperatures of 36.4 and 37.6 degrees C, respectively, which resembles those seen for collagens. We finally demonstrated by electron microscopy that the Scl proteins are organized into "lollipop-like" structures, similar to those seen in human proteins with collagenous domains. This implies that the repeated GXY tripeptide motif is a structural indicator of collagen-like triple helices in proteins from such phylogenetically distant sources as bacteria and humans.     

Triple helical stabilities of guest-host collagen mimetic structures

The peptoid Nleu (N-isobutylglycine) has been successfully incorporated into a series of collagen mimetics composed of Gly-Pro-Nleu and Gly-Nleu-Pro sequences and has been able to maintain triple helices in appropriate structures. The achiral trimeric sequence Gly-Nleu-Nleu as a guest sequence in structures such as Ac-(Gly-Pro-Hyp)3-(Gly-Nleu-Nleu)3-(Gly-Pro-Hyp)3-NH2 retains triple helicity. As an extension of this study, we report, in this paper, on a series of guest-host collagen mimetic structures in which Gly-Nleu-Pro sequences are employed as the host. The guest sequences for these guest-host structures include Gly-Nleu-Nleu and Gly-Nx-Pro sequences where Nx is composed of a variety of alkyl and aralkyl peptoid residues. From these guest-host collagen mimetic structures, we are able to elucidate the contributions of hydrophobic and steric effects on triple helix formation. The Gly-Nleu-Pro sequences have been shown to be effective in inducing triple helicity. Conformational characterization of the guest-host collagen mimetic structures was established by techniques such as temperature-dependent optical rotation measurements and circular dichroism (CD) spectroscopy.     

Curious structure in “canonical” alanine-based peptides

We have performed all atom simulations of blocked peptides of the form (AAXAA)₃, where X = Gln, Asn, Glu, Asp, Arg, and Lys with explicit water molecules to examine the interactions between side chains spaced i,i–5 in the sequence. Although side chains in this i,i–5 arrangement are commonly believed to be noninteracting, we have observed the formation of unusual i,i–5 main chain hydrogen bonding in such sequences with positively charged residues (Lys) as well as polar uncharged groups (Gln). Our results are consistent with the unusual percentage of hydrogen bonding curves produced by amide exchange measurements on the well-studied sequence acetyl-(AAQAA)₃-amide in water (Shalongo, W., Dugad, L., Stellwagen, E. J. Am. Chem. Soc. 116:8288–8293, 1994). Analysis of our simulations indicated that the glutamine side chain showed the greatest propensity to support π helix formation and that the i,i–5 intramolecular hydrogen bonds were stabilized by water-bridging side chain interactions. This intermittent formation of the unusual π helix structure was observed for up to 23% of the total simulation time in some residues in (AAQAA)₃. Control studies on peptides with glutamine side chains spaced i,i–3, i,i–4, and i,i–6 did not reveal similar unique structures, providing stronger evidence for the unique role side chain interactions with i,i–5 spacing. © 1997 Wiley-Liss Inc.     

Intramolecular triple helix as a model for regular polyribonucleotide (CAA)n

The regular (CAA)_n polyribonucleotide, as well as the omega leader sequence containing (CAA)-rich core, have recently been shown to form cooperatively melted and compact structures. In this report, we propose a structural model for the (CAA)_n sequence in which the polyribonucleotide chain is folded upon itself, so that it forms an intramolecular triple helix. The triple helix is stabilized by hydrogen bonding between bases thus forming coplanar triads, and by stacking interactions between the base triads. A distinctive feature of the proposed triple helix is that it does not contain the canonical double-helix elements. The difference from the known triple helices is that Watson-Crick hydrogen bond pairings do not take place in the interactions between the bases within the base triads.     

Glycosylated Threonine but not 4-Hydroxyproline Dominates the Triple Helix Stabilizing Positions in the Sequence of a Hydrothermal Vent Worm Cuticle Collagen

The cuticle collagen of the vestimentiferanRiftia pachyptila, an organism which is endemic to deep-sea hydrothermal vents, has several unusual properties including an extraordinary length (1.5 μm), a high thermal stability (37°C) in spite of a low 4-hydroxyproline content and an atypically high threonine content (20 mol%). We have now purified the constituent chain of cuticle collagen and show that it contains about 40% carbohydrate, which is mainly galactose, indicating that the chain has a molecular mass of approximately 750 kDa. Several large (30 to 150 kDa) fragments, which all contained carbohydrate, could be produced by cleavage with endoproteinase Lys-C, bacterial collagenase and cyanogen bromide (CNBr). Edman degradation of these and several smaller fragments was used to determine about 3000 sequence positions comprising 60% of the total triple-helical sequence. This demonstrated mainly typical Gly-X-Y triplet repeats with a few imperfections and a longer N-terminal non-triplet sequence. Most of the 4-hydroxyproline was found in triplet position X, where it decreases the stability of the triple helix. About 40% of the Y positions could not be identified, which correlated with a low abundance of threonine in the sequence and the demonstration of threonine in these positions after deglycosylation of several peptides by treatment with hydrofluoric acid. Matrix-assisted laser desorption ionisation mass spectrometry of selected peptides indicated that the blocked threonine residues are occupied by chains of one, two or three hexoses (presumably galactose). These glycosylated threonine residues in Y positions are therefore likely to replace 4-hydroxyproline as the major contributor to triple helix stabilization. Studies with a synthetic (Gly-Pro-Thr)₁₀oligopeptide demonstrated a low thermal stability of its triple helix which emphasizes a crucial role of glycosylation for stabilization.     

An energetic evaluation of a “Smith” collagen microfibril model

An energy minimized three-dimensional structure of a collagen microfibril template was constructed based on the five-stranded model of Smith (1968), using molecular modeling methods and Kollman force fields (Weiner and Kollman, 1981). For this model, individual molecules were constructed with three identical polypeptide chains ((Gly-Pro-Pro) _n , (Gly-Prop-Hyp) _n , or (Gly-Ala-Ala) _n , wheren=4, 12, and 16) coiled into a right-handed triple-helical structure. The axial distance between adjacent amino acid residues is about 0.29 nm per polypeptide chain, and the pitch of each chain is approximately 3.3 residues. The microfibril model consists of five parallel triple helices packed so that a left-handed superhelical twist exists. The structural characteristics of the computed microfibril are consistent with those obtained for collagen by X-ray diffraction and electron microscopy. The energy minimized Smith microfibril model for (Gly-Pro-Pro)₁₂ has an axial length of about 10.2 nm (for a 36 amino acid residue chain), which gives an estimated D-spacing (234 amino acids per chain) of approximately 66.2 nm. Studies of the microfibril models (Gly-Pro-Pro)₁₂, (Gly-Pro-Hyp)₁₂, and (Gly-Ala-Ala)₁₂ show that nonbonded van der Waals interactions are important for microfibril formation, while electrostatic interactions contribute to the stability of the microfibril structure and determine the specificity by which collagen molecules pack within the microfibril.     

Conformational analysis and stability of collagen peptides by CD and by 1H- and 13C-NMR spectroscopies

Four small type I collagen CNBr peptides containing complete natural sequences were purified from bovine skin and investigated by CD and 1H- and 13C-nmr spectroscopies to obtain information concerning their conformation and thermal stability. CD showed that a triple helix was formed at 10 degrees C in acidic aqueous solution by peptide alpha l(I) CB2 only, and to lesser extent, by alpha 1(I) CB4, whereas peptides alpha 1(I) CB5 and alpha 2(I) CB2 remained unstructured. Analytical gel filtration confirmed that peptides alpha 1(I) CB2 and alpha 1(I) CB4 only were able to form trimeric species at temperature between 14 and 20 degrees C, and indicated that the monomer = trimer equilibrium was influenced by the chaotropic nature of the salt present in the eluent, by its concentration, and by temperature variations. CD measurements at increasing temperatures showed that alpha 1(I) CB2 was less stable than its synthetic counterpart due to incomplete prolyl hydroxylation of the preparation from the natural source. 1H- and 13C-nmr spectra acquired in the temperature range 0-47 and 0-27 degrees C, respectively, indicated that with decreasing temperature the most abundant from of alpha 1(I) CB2 was in slow exchange with an assembled form, characterized by broad lines, as expected for the triple-helical conformation. A large number of trimer cross peaks was observed both in the proton and carbon spectra, and these were most likely due to the nonequivalence of the environments of the three chains in the triple helix. This nonequivalence may have implications for the aggregation of collagen molecules and for collagen binding to other molecules. The thermal transition from trimer to monomer was also monitored by 1H-nmr following the change in area of the signal belonging to one of the two beta protons of the C-terminal homoserine. The unfolding process was found to be fully reversible with a melting temperature of 13.4 degrees C, in agreement with CD results. The qualitative superposition of the melting curves obtained by CD for the peptide bond characteristics and by nmr for a side chain suggests that triple-helical backbone and side chains constitute a single unit.