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.     

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.     

Two states of the triple helix in the thermal transition of the collagen model peptide (Pro-Pro-Gly)10

The collagen model peptide (Pro-Pro-Gly)10 is known to fold into a triple helix in solution. So far, the triple helix has been considered to exist as a single state. However, our previous study of (Pro-Pro-Gly)10 in solution has indicated the presence of two different states of the triple helix, a lower (HL) and a higher temperature state (HH). In the present study, these triple-helical states were investigated in more detail by NMR. Complete stereospecific assignments of the methylene protons of the proline residues were accomplished by the use of NOESY and TOCSY spectra. The temperature dependence of the 1H chemical shifts showed that the HL-to-HH thermal transition can be attributed to a conformational change of the first proline (Pro1) residues of the (Pro-Pro-Gly) triplets. Since TOCSY spectra with a 10 ms mixing-time confirmed a down puckering of these Pro residues in the HL state, but interconverting down and up puckerings in the HH state, the HL-to-HH thermal transition corresponds to conformational changes of the pyrrolidine rings of the Pro1 residues from an uniform down puckering to a more flexible state. The results confirm that thermal unfolding of the triple helix proceeds through the intermediate HH state.     

Vibrational neutron spectroscopy of collagen and model polypeptides.

A pulsed source neutron spectrometer has been used to measure vibrational spectra (20-4000 cm-1) of dry and hydrated type I collagen fibers, and of two model polypeptides, polyproline II and (prolyl-prolyl-glycine)10, at temperatures of 30 and 120 K. the collagen spectra provide the first high resolution neutron views of the proton-dominated modes of a protein over a wide energy range from the low frequency phonon region to the rich spectrum of localized high frequency modes. Several bands show a level of fine structure approaching that of optical data. The principal features of the spectra are assigned. A difference spectrum is obtained for protein associated water, which displays an acoustic peak similar to pure ice and a librational band shifted to lower frequency by the influence of the protein. Hydrogen-weighted densities of states are extracted for collagen and the model polypeptides, and compared with published calculations. Proton mean-square displacements are calculated from Debye-Waller factors measured in parallel quasi-elastic neutron-scattering experiments. Combined with the collagen density of states function, these yield an effective mass of 14.5 a.m.u. for the low frequency harmonic oscillators, indicating that the extended atom approximation, which simplifies analyses of low frequency protein dynamics, is appropriate.     

Comprehensive conformational analysis of (Gly-Pro-Pro)n and (Gly-Pro-Hyp)n related to collagen

A complete analysis of all possible conformations with correct hydrogen bonds of the collagen II type was performed on the basis of developed simultaneous equations. Using a unimodal search (by varying Ψ³), the energetically favorable structure was obtained. No other energetically satisfactory structural solutions are possible. The next aim was to obtain a precise model of the molecule. The program used includes a subroutine for continual deformation of the pyrrolidine rings. The set of parameters determining the structure consists of 14 independent variables (8 dihedral and 6 bond angles). As starting points for the energy optimization, conformations produced by scanning and some structures from previous work were used. The final structures (practically the same for both polymers) have helix parameters h = 0.285 nm and t = 52°, which are in excellent agreement with the 7/2 symmetry of diffraction data. The conformations of the pyrrolidine rings are of the B type, i.e., C₂-C^β-exo-C^γ-endo. For both polypeptides, the conformations of imino acids in position 3 of the triplet are the same; in position 2, however, they are slightly different. The difference in diffraction patterns for the 7/2 and 10/3 helices is discussed.     

Physicochemical analysis of (Pro-Pro-Gly)n with defined molecular weight--temperature dependence of molecular weight in aqueous solution

Sequenced polytripeptides, (Pro-Pro-Gly)_n, (n = 10, 15, 20), with defined molecular weights were synthesized by the solid-phase method. Conformational changes of these sample as a function of temperature were studied by measurements of optical rotation and sedimentation equilibrium. The temperature dependence of optical rotation was shown similar to thermal transition of collagen molecule. Each of these polymers existed as a timer at lower temperature. (Pro-Pro-Gly)₁₀ existed as a monomer at higher temperature, and the others were expected to behave analogously.     

Conformational analysis of polytripeptides (Gly-Pro-Ala)n, (Gly-Ala-Hyp)n,and (Gly-Ala-Ala)n in connection with the problem of collagen structure

Conformational analysis of triple helics of a type of collagen was performed with typical collagen tripeptide sequences based on Gly-Pro-Ala, Gly-Ala-Hyp, and Gly-Ala-Ala. During energy minimization, the possibility of continual deformation of the pyrrolidine cycle was taken into account in order to achieve better accuracy in the resulting structure. The (Gly-Pro-Ala)_n structure is almost isomorphic to the (Gly-Pro-Hyp)_n structure obtained in the previous work [Tumanyan, V. G. & Esipova, N.G. (1982) Biopolymers 21 , 475–497]. For a collagen-type structure, the optimal conformation of (Gly-Ala-Hyp)_n tends to have a decreased unit twist (t = 15°), although the energy advantage with respect to the conformation with t = 45° is not so significant. A similar situation is observed for (Gly-Ala-Ala)_n. In this case, the energy decrease during unwinding to t = 15° from t = 45° is quite small. The conformations of (Gly-Ala-Hyp)_n and (Gly-Ala-Ala)_n with t = 15° exhibit a similarity with a triple complex of polyproline II helices—a noncoiled coil such as (Gly-Pro-Hyp)_n and (Gly-Pro-Ala)_n. A similar structure may be postulated for subcomponent cq1 of the first component of a human complement containing substantial Gly-X-Pro and Gly-X-Y tripeptide derivatives in the primary structure (X, Y = any amino acid). The results suggest that the observed helical symmetry of collagen (t = 36°) is a consequence of superposition of diffraction patterns (for sufficiently long segments) from various helices (t varies from ～15° for Gly-X-Hyp and Gly-X-Y to ～56° for Gly-Pro-Ala). For short alternating segments, some unification of different helical structures is possible.     

Hydroxylation of (Pro-Pro-Gly)5 and (Pro-Pro-Gly)10 by prolyl hydroxylase. Evidence for an asymmetric active site in the enzyme.

Previous studies with 14C-labeled synthetic peptides demonstrated that prolyl hydroxylase, which synthesizes the hydroxyproline in collagen, preferentially hydroxylates the fourth triplet from the NH-terminal end of the peptide (Pro-Pro-Gly)5. In the experiments reported here, the prolyl hydroxylase reaction was investigated further by preparing chemically modified derivatives of (Pro-Pro-Gly)5 and by synthesizing 14C-labeled preparations of (Pro-Pro-Gly)10. Essentially, the same kcat value was found for the hydroxylation of (Pro-Pro-Gly)5, N-acetyl-(Pro-Pro-Gly)5, (Pro-Pro-Gly)5 methyl ester, (Pro-Pro-Gly)10, and for larger polypeptide substrates of the enzyme. It appeared therefore that preferential hydroxylation of specific triplets in peptides of the structure (Pro-Pro-Gly)n cannot be explained by differences in the kinetic constants for individual triplets. Hydroxylation of 14C-labeled preparations of (Pro-Pro-Gly)10 demonstrated that the ninth triplet was preferentially hydroxylated over any other triplet. The results were best explained by the hypothesis that prolyl hydroxylase has an asymmetric active site in which binding subsites are located adjacent to but not symmetrical with the catalytic subsite.     

Polypeptide models of collagen: Properties of (Pro-Pro-betaAla)n.

We have synthesized (Pro-Pro-βAla)_n as a model for collagen. The synthetic polytripeptide, mol wt 6500, exhibits a large negative optical rotation with a very strong negative Cotton effect centered at 216 nm. The optical rotatory dispersion of (Pro-Pro-βAla)_n followed a single-term Drude equation and the λ_c was 195 nm. The rotation decreased markedly on heating with the midpoint of the broad transition at 55°C. Preliminary studies also showed loss of structure in guadinine HCl. The circular dichroism spectrum of the polymer exhibited a deep trough at 190 nm. The marked similarities of solution properties of (Pro-Pro-βAla)_n to (Pro-Pro-Gly)_n suggest that β-alanine can replace glycine in generating collagen-like helix in solution.     

Conformational studies on sequential polypeptides Part VI. Structural investigations on (Pro-Leu-Gly)10, (Pro-Leu-Gly)n and (Leu-Pro-Gly)n.

The conformational properties of (Pro-Leu-Gly)10, (Pro-Leu-Gly)n and (Leu-Pro-Gly)n were investigated both in solution and in solid state. By circular dichroism studies it was possible to demonstrate the formation of an ordered collagen-like structure for (Pro-Leu-Gly)n in hexafluroisopropanol-water mixtures and in ethylene glycol; (Leu-Pro-Gly)n assumes an ordered conformation only in ethylene glycol; (Pro-Leu-Gly)10 is unordered under all the conditions studied. X-ray diffraction patterns indicated that (Pro-Leu-Gly)n and (Leu-Pro-Gly)n assume a triple helical structure in solid state. In addition, the investigation of (Pro-Leu-Gly)n strongly suggests that this type of structure is a single chain triple helix. The X-ray patterns of (Pro-Leu-Gly)10 do not allow us to ascertain a collagen or polyproline II-like structure for this decatripeptide.     

Correlation between Raman and X-ray crystallography data of (Pro-Pro-Gly)10

Model biopolymers are powerful tools to guide the interpretation of physical properties in complex systems. (Pro-Pro-Gly)(10), (PPG)(10), is a collagen-model peptide, whose structure is known at high resolution. Herein, Raman microscopy data of (PPG)(10) powders and single crystals are reported. The spectra interpretation leads to an accurate assignment of three well-resolved amide bands corresponding to the three peptide bonds (PP, PG and GP) present in the (PPG)(10) structure. These data together with the availability of torsional angles phi and psi derived from the high-resolution crystal structure, provide the opportunity to test the validity of theoretical equations for the calculation of non-canonical amide III bands and represent a reference for theoretical calculations of vibrational spectra and for polyproline II detection in complex proteins. Spectroscopic data do not support the indication of two distinct and equally populated up and down conformations of the pyrrolidine rings observed in the (PPG)(10) crystal structure.     

Conformational studies on sequential polypeptides. Part V. Synthesis and characterization of (Pro-Leu-Gly)10, (Pro-LeuqGly)n and (Leu-Pro-Gly)n.

Syntheses of (Pro-Leu-Gly)n and (Leu-Pro-Gly)n, two synthetic polytripeptide analogues of the non-polar regions of collagen, via the corresponding tripeptide p-nitrophenyl-esters are described. The sequential polypeptide (Pro-Leu-Gly)10 was also obtained by solid-phase synthesis. In the following paper, conformational investigations on these polymers, both in solution and in solid state, will be described.     

Crystal and molecular structure of a collagen-like polypeptide (Pro-Pro-Gly)10

(Pro-Pro-Gly)₁₀ forms single crystals, providing X-ray diffraction data to 0.22 nm resolution. In the crystals, the polypeptides form triplexes that aggregate end-to-end in quasi-infinite helices with axial translation per tripeptide h = 0.287 nm and the corresponding rotation t = ?102.9 °. The structure, which may be an allomorph of collagen, has been refined by the linked-atom least-squares procedure. In addition, three water molecules per tripeptide have been detected by Fourier difference syntheses. One of them forms an intrachain hydrogen-bonded bridge O(Pro₂) - - - W - - - O(Gly). There are also interchain hydrogen bonds (Gly)NH - - - O(Pro₁) within the triplex.     

Two types of tripeptide conformation in collagen. Calculation of the structure of (Gly-Pro-Ser)n and (Gly-Val-Hyp)n polytripeptides

Conformational analysis of polypeptides (Gly-Pro-Ser)n and (Gly-Val-Hyp)n was carried out for collagen-like triple helical complexes (coiled coils with screw symmetry). The lowest energy structure of the first polymer (helical parameters t 52,8, h 0,282 nm) is very close to that of (Gly-Pro-Hyp)n. The hydroxyl group of a serine residue does not form any intramolecular hydrogen bonds in this structure. (Gly-Val-Hyp)n triple complex is shown to unwind to t 7,7, h 0,297 nm as a result of optimization procedure. These findings confirm the assumption, made earlier on the basis of conformational analysis of (Gly-Pro-Hyp)n, (Gly-Pro-Ala)n, (Gly-Ala-Hyp)n, (Gly-Ala-Ala)n, that the collagen triple helix contains stable wound triplets with proline in the second position, while the absence of imino acid in the 2nd position facilitates the unwinding of the triple helix. Thus, a collagen helix appears to have different parameters for the sites differing in the amino acid sequence. The values measured in the X-ray experiments (h 0,29 nm, t' 36) should be considered as a result of averaging. The model allows to reconcile the X-ray data for collagen and crystalline (Gly-Pro-Pro)10 oligomer.     

Stabilization of (dG-dC)n.(dG-dC)n in the Z conformation by a crosslinking reaction

(dG-dC)n.(dG-dC) was converted to the Z conformer by heating in the presence of Mn++n. Reaction of this preparation with the crosslinking reagent, DL-diepoxybutane (DEB), stabilized this conformer so that it retained its structure even when returned to conditions that favored reversion to the B conformation. Treatment of the crosslinked Z conformer with periodate caused scission of the crosslink, allowing reversion to the B conformer. Reaction of (dG-dC)n.(dG-dC)n in the B conformation with DEB did not prevent conversion to the Z conformer in 4M NaC1; dialysis of the high salt solution against low ionic strength buffer allowed return to the B conformer. The Z in equilibrium B transitions were followed by circular dichroism studies and immunochemical procedures. The results suggest the feasibility of stabilizing Z sequences of DNA in chromatin by crosslinking, so that they could then be identified after DNA isolation.     

The energy of formation of internal loops in triple-helical collagen polypeptides

The sequence-dependent local destabilization in the interior of the collagen triple helix has been evaluated by means of conformational energy computations. Using a model poly(Gly-Pro-Pro) triple helix as the reference state, a method was developed for generating local loops, i.e., internal deformations, and analyzing their conformations. A seven-residue Gly-Pro-Pro-Gly-Pro-Pro-Gly fragment was replaced by the Gly-Pro-Ala-Gly-Ala-Ala-Gly sequence in one, two, or all three of the strands of the loop region. A set of loop conformations was generated in which the ends of the loop were initially fixed in the triple-helical structure. The potential energy of the entire deformed triple helix was then minimized, resulting in a variety of structures that contained deformed loops. The conformations of the triple helices at the two ends of the loops remained essentially unchanged in many of the low-energy conformations. In numerous high-energy conformations, however, the triple-helical segments were also partially or totally disrupted. The minimum-energy conformations of the whole structures were compared in terms of rms deviations of atomic coordinates with respect to the original triple helix, and of the shapes of the loops (using a distance function derived from differential geometry). Three new geometrical parameters—stretch S, kink K, and unwinding U—were defined to describe the changes in the overall orientation of the triple helices at the two ends of the loop. It is shown that, when the number of Pro residues in a short fragment is reduced, the triple helical structure can accomodate internal loops (i.e., distortions) within a 5 kcal/mol cutoff from the essentially unperturbed triple helical structure. For structures with a Gly-Pro-Ala-Gly-Ala-Ala-Gly sequence in all three strands, the probability of finding conformations with internal loops is small, i.e., 0.06. Internal loops affect the overall orientation of these structures, as measured by the helix-distortion parameters S, K, and U. © 1995 John Wiley & Sons, Inc.