Geometrical and conformational preferences of the 9-fluorenylmethoxycarbonyl-amino moiety.

Structural parameters, originating from x-ray crystallographic data, have been compiled for 13 derivatives of amino acids, peptides and related compounds, which contain a total of 14 Fmoc-NH- moieties. For these moieties, molecular geometries and conformations--described by the omegao, theta1, theta2 and theta3' torsion angles--were analysed and compared with the corresponding parameters for the Z-NH- and Boc-NH-moieties (290 and 553, respectively). To gain a deeper insight into the conformational features of the Fmoc-NH- moiety, ab initio free molecule calculations were performed for fully relaxed minima. Also the potential energy surface as a function of the torsion angles (theta3', theta2) was generated. The conformational features of the Fmoc-NH- moiety: (i) two possible values for the angle omegao (approximately 180 degrees or, rarely, approximately theta degrees) and (ii) the angle theta1 = 180 degrees +/- 15 degrees, are common to the Z-NH- and Boc-NH- systems. By contrast, the theta2 and theta3 angles in the Fmoc, Z and Boc groups differ essentially. In the Fmoc groups theta2 mostly has values of 180 degrees +/- 30 degrees and values up [115 degrees] seem to be forbidden, whereas fewer than half of the Z groups adopt theta2 approximately 180 degrees and the remainder have theta2 in the range of [90 degrees +/- 20 degrees]. On the other hand, the Boc methyl groups are staggered. The theta3 values observed for Fmoc are limited to the regions of 180 degrees +/- 20 degrees and 160 degrees +/- 20 degrees], while for the Z group a variety of theta3 occurs. The orientation of the fluorenyl vs the urethane function is mostly trans. Our results suggest a lower conformational flexibility for the Fmoc group compared with that of the Z group. Our calculations confirm that the observed conformational features for the Fmoc-NH- moiety are inherent properties. The Fmoc-NH-moiety in crystals involves the participation of its O=C-NH functionality in hydrogen bonds.     

Structural and conformational properties of (Z)-beta-(1-naphthyl)- dehydroalanine residue

To understand how chemical structure of beta-substituted alpha, beta-dehydroalanine (particularly size and pi conjugation of beta substituent) affects conformational property, x-ray crystallographic analysis was performed on Boc-Ala-Delta(Z) Nap-Val-OMe [Boc: t-butoxycarbonyl; Delta(Z) Nap: (Z)-beta-(1-naphthyl)dehydroalanine; OMe: methoxy] having the naphthyl group as a bulky beta substituent. Single crystals were grown by slow evaporation from an ethanol solution in the triclinic space group P1 with a = 9.528 (3) A, b = 12.410(4) A, c = 5.975(2) A, alpha = 96.77(3) degrees, beta = 102. 81(2) degrees, gamma = 88.74(3) degrees, V = 684.1(4) A3, and Z = 1. Phase determination was carried out by a direct method (SHELEXS), and the final structure was refined to R = 8.1% and R(w) = 9.0% for 1964 observed reflections. The bond lengths and bond angles of the Delta(Z)Nap residue, characterized by a sp(2) hybridized C(alpha) atom, did not differ from those of other dehydroresidues such as Delta(Z) Phe, Delta(Z) Leu, and DeltaVal essentially. The peptide backbone took a type II beta-turn conformation involving an intramolecular hydrogen bond between CO(Boc) and NH(Val), similar to di- or tripeptides containing a Delta(Z) Phe or Delta(Z) Leu residue in the second positions. Here the naphthyl group was found to be nonplanar [chi(2) = 55(1) degrees ] relative to the C(alpha)==C(beta)==C(gamma) plane. The nonplanarity was supported by conformational energy calculation. The molecular packing was stabilized by two kinds of intermolecular hydrogen bonds and van der Waals interactions. Naphthyl groups were arranged in a partially overlapped face-to-face orientation with a center-to-center distance of 5.97 A. For additional information, peptide Boc-(Ala-Delta(Z) Nap-Leu)(2)-OMe was synthesized and its solution conformation was investigated by (1)H-NMR spectroscopy. The hexapeptide showed the tendency to form a 3(10)-helical conformation in solution essentially. Conformational properties of Delta(Z) Nap residue, characterized by a type II beta-turn and 3(10)-helix, were supported by a conformational energy contour map of the Delta(Z)Nap residue.     

AAF linked to the guanine amino group: a B-Z junction.

Minimized conformational potential energy calculations have been performed for AAF linked to dCpdG at the guanine amino group. This is a model for the minor AAF adduct observed in DNA, whose conformational influence has been difficult to ascertain. A global minimum energy conformation was computed with torsion angles like those of the dCpdG residue of Z-DNA. This conformation was incorporated into a larger polymer model at a B-Z junction, with the carcinogen residing in the groove in the Z direction. Local minimum energy conformations of the B type were also computed. In addition, two minima were found with fluorenecytidine stacking. These results suggest that existing B-Z junctions may be vulnerable to modification by AAF at the guanine amino group, or that such junctions may be induced by the carcinogen if the base sequence is appropriate. Otherwise the carcinogen can be located in the minor groove of the B helix (5, 10, 11) or covalently intercalated (13-15).     

Effect of lengthening of peptide backbone by insertion of chiral beta-homo amino acid residues: conformational behavior of linear peptides containing alternating L-leucine and beta-homo L-leucine residues

The synthesis and the solution behavior of the linear peptides containing a beta-homo (beta-H) leucine residue-Boc-Leu-beta-HLeu-Leu-OMe, Boc-beta-HLeu-Leu-beta-HLeu-Leu-OMe, and Boc-Leu-beta-HLeu-Leu-beta-HLeu-Leu-OMe-as well as the solid structure of the tripeptide, are reported. The conformational behavior of the peptides was investigated in solution by two-dimensional nmr. Our data support the existence in solution with different families of conformers in rapid interchange. The crystals of the tripeptide are orthorhombic, space group P2(1)2(1)2, with a = 15.829(1) A, b = 29.659(1) A, c = 6.563(1) A, and Z = 4. The structure has been solved by direct methods and refined to final R1 and wR2 indexes of 0.0530 and 0.1436 for 2420 reflections with I > 2sigma(I). In the solid state, the tripeptide does not present intramolecular H bonds, and the peptide backbone of the two leucine residues adopts a quasi-extended conformation. For the beta-HLeu residue, the backbone conformation is specified by the torsion angles straight phi(2) = -120.9(4) degrees, mu(2) = 56.7(4) degrees, psi(3) = -133.2(4) degrees. The side chains of the three residues assume the same conformation (g(-), g(-), trans), and all peptide bonds, except the urethane group at the N-terminus, are in the trans conformation. Preliminary conformational energy calculations carried out on the Ac-NH-beta-HAla-NHMe underline that the conformations with mu angle equal to 180 degrees and 60 degrees assume lower energy with respect to the others. In addition, we found a larger conformational freedom for the psi angle with respect to the straight phi angle.     

Consistent force field calculations on 2,5-diketopiperazine and its 3.6-dimethyl derivatives

The minimum energy conformations are calculated for 2, 5-diketopiperazine (DKP) and its 3,6-dimethyl derivatives (DL-DMDKP and LL-DMDKP), using a consistent force field approach developed previously. The energy function parameters that were not required in earlier calculations on alkanes, amides, mid lactams are fitted to spectral and conformational data on the diketopiperazines. Vibrational assignments are suggested for DKP. Conformational energies are also determined over a range of selected values for ring dihedral angles, and the shape of the potential energy functions is examined over deviations from planarity. DKP and LL-DMDKP are found to have non-planar minimum energy conformations, separated from planar by less than a kcal/mole. DL-DMKP exhibits a nearly flat trough about the planar conformation. Calculations of minimum energies with one dihedral angle coordinate constrainted show a coupling between bond angles and dihedral angles in agreement with recent suggestions of Benedetti.     

Statistical and energetic analysis of side-chain conformations in oligopeptides

The distributions of side-chain conformations in 258 crystal structures of oligopeptides have been analyzed. The sample contains 321 residues having side chains that extend beyond the C beta atom. Statistically observed preferences of side-chain dihedral angles are summarized and correlated with stereochemical and energetic constraints. The distributions are compared with observed distributions in proteins of known X-ray structures and with computed minimum-energy conformations of amino acid derivatives. The distributions are similar in all three sets of data, and they appear to be governed primarily by intraresidue interactions. In side chains with no beta-branching, the most important interactions that determine chi 1 are those between the C gamma H2 group and atoms of the neighboring peptide groups. As a result, the g- conformation (chi 1 congruent to -60 degrees) occurs most frequently for rotation around the C alpha-C beta bond in oligopeptides, followed by the t conformation (chi 1 congruent to 180 degrees), while the g+ conformation (chi 1 congruent to 60 degrees) is least favored. In residues with beta-branching, steric repulsions between the C gamma H2 or C gamma H3 groups and backbone atoms govern the distribution of chi 1. The extended (t) conformation is highly favored for rotation around the C beta-C gamma and C gamma-C delta bonds in unbranched side chains, because the t conformer has a lower energy than the g+ and g- conformers in hydrocarbon chains. This study of the observed side-chain conformations has led to a refinement of one of the energy parameters used in empirical conformational energy computations.     

Conformational energy refinement of horse-heart ferricytochrome c.

The reported X-ray structure of horse-heart ferricytochrome c has been refined by conformational energy calculations, using a three-stage computational procedure. In stage I, the atomic positions are adjusted to conform to idealized bond lengths and bond angles characteristic of small amino acid derivatives, while yet remaining as close as possible to the X-ray coordinates. In stage II, atomic overlaps are eliminated by adjusting the backbone and side-chain dihedral angles to minimize the nonbonded energy, hydrogen-bonded energy, and rotational energy contributions. In the final stage of refinement, the electrostatic energy and a more accurate hydrogen-bonded energy treatment are considered, in addition to the energy contributions of stage II. A "fitting potential" of gradually decreasing strength is imposed in both stages II and III, in order to keep the computed structure as similar to the x-ray structure as is consistent with a low-energy conformation. The final computed structure of cytochrome c exhibits a very low conformational energy (-504 kcal/mol) and also closely resembles the X-ray structure (RMS deviation = 0.77 A for all atoms). However, a special treatment was required in order to alter the location of the phenyl ring of phenylalanine-82. In contrast to the originally published X-ray structure, which shows the phenyl ring pointing away from the heme, the phenyl ring in the computed structure is tucked into the heme crevice, in a position similar to that observed in the reduced form of tuna cytochrome c, in the oxidized form of Rhodospirillum rubrum cytochrome c2, and also in the recently determined structure of oxidized tuna cytochrome c.     

Determination of productive conformations of acetylcholinesterase substrates using theoretical conformational analysis

All equilibrium conformations of twenty-three acetylcholinesterase effectors were calculated by the molecular mechanics method, nonbonded interactions, torsion energy and energy of bond angles deformation being taken into account. In a series of conformationally flexible derivatives of acetylcholine the correlation was found between hydrolysis rate and population of the completely extended tt-conformation. In a series of cyclic analogues of acetylcholine the high hydrolysis rate occurs only for substrates sterically corresponding to tt-conformation of acetylcholine with regard to disposition of ammonium group, carbonyl oxygen and carbonyl carbon. The hydrolysis rate of acetylcholine derivatives with elongated chain between acetyl and cationic groups is directly proportional to the population of the conformations similar to tt-conformation of acetylcholine. It is concluded that tt-conformation of acetylcholine is productive for acetylcholinesterase hydrolysis.     

Stereochemical effects of non-ionic methylphosphonates on nucleotide conformations.

The preferred conformations of deoxyribo and ribonucleoside 3'-methylphosphonates are analysed by minimizing the conformational energy as a function of all the major parameters including the sugar ring for both the S- and R-isomers. The results show that neither the substitution nor the nature of the diastereomer affects significantly the preferred conformations compared to the naturally occurring nucleoside 3'-phosphates. The preferred range of C3'-O3' bond torsions or the phase angles of pseudorotation (P) of the sugar are unaffected. The chiral substitution on the phosphate always adopts a conformation distal to the secondary C3' carbon atom in the minimum energy conformational state. Further, it introduces certain restrictions on the preferred range of P-O3' torsions depending on the methylphosphonate configuration. Methylphosphonate, especially the S-isomer, renders the normal gauche- range of P-O3' bond torsions responsible for the stacked helical duplexes to be energetically unfavourable besides introducing a high energy barrier between trans and gauche conformations. Therefore it is suggested that duplexes with S-methylphosphonate may favour extended phosphodiester conformations. These factors explain the observed lower melting temperature as well as the downfield shifts in the 31P signals in duplexes containing the S-isomer.     

Location of proline derivatives in conformational space. I. Conformational calculations; optical activity and NMR experiments

In order to develop methods of analysis applicable to the determination of the conformation of biological polymers in solution, a series of proline derivatives was studied. The steric constraints of the pyrrolidine ring limit these compounds to a relatively small set of conformations. This set was further reduced by eliminating conformations with large computed conformational energy. Computations revealed that the conformational energy of the proline derivatives fits into one of three classes, depending on the bulk and the polarity of the C-terminal group. Three analogous classes of optical activity were observed. The optical activity data were analyzed in terms of conformations computed to be of low energy. In some cases qualitative theoretical considerations enabled molecular groups to be located. For example, solvent-dependent isomerization of the carboxyl hydrogen of N-acetyl-L -proline was detected. Nuclear magnetic resonance provided an experimental measure of the fraction of molecules which had cis unsymmetrically-substituted tertiary amide groups. This information aided and confirmed the other measures of molecular conformation.     

β-Turn conformations in crystal structures of model peptides containing α,α-Di-n-propylglycine and α,α-Di-n-butylglycine

The crystal state conformations of three peptides containing the α,α-dialkylated residues. α,α-di-n-propylglycine (Dpg) and α,α-di-n-butylglycine (Dbg), have been established by x-ray diffraction. Boc-Ala-Dpg-Alu-OMe (I) and Boc-Ala-Dbg-Ala-OMe (III) adopt distorted type II β-turn conformations with Ala (1) and Dpg/Dbg (2) as the corner residues. In both peptides the conformational angles at the Dxg residue (I: ? = 66.2°, ψ = 19.3°; III: ? = 66.5°. ψ = 21.1°) deviate appreciably from ideal values for the i + 2 residue in a type II β-turn. In both peptides the observed (N…O) distances between the Boc CO and Ala (3) NH groups are far too long (1: 3.44 Å: III: 3.63 Å) for an intramolecular 4 → 1 hydrogen bond. Boc-Ala-Dpg-Ata-NHMe (II) crystallizes with two independent molecules in the asymmetric unit. Both molecules HA and HB adopt consecutive β-turn (type III-III in HA and type III-I in IIB) or incipient 3₁₀-helical structures, stabilized by two intramolecular 4 → 1 hydrogen bonds. In all four molecules the bond angle N-C^α-C′ (τ) at the Dxg residues are ≥ 110°. The observation of conformational angles in the helical region of ?,ψ space at these residues is consistent with theoretical predictions. © 1995 John Wiley & Sons, Inc.     

Simulation of conformational possibilities of DNA via calculation of nonbonded interactions of complementary dinucleoside phosphate complexes

Using classical potential functions, we carried out potential-energy calculations on the complementary deoxydinucleoside phosphate complexes dApdA:dUpdU, dUpdA:dUpdA, and dApdU:dApdU. All dihedral and bond angles, except those of the nitrogen bases, were varied. The resulting minimum-energy conformations of the complexes are close to DNA A- and B-family conformations, with a typical arrangement of the nitrogen bases. The dihedral and bond angles of one of the molecules forming the complex can thereby differ by several degrees from those of the other molecule. For different base sequences, some dihedral and bond angles may vary over a range of several degrees without appreciably changing the total energy of the complex. Some low-energy conformations of the complexes corresponding to other regions of the conformational space are also found. The biological consequences of possible changes in dihedral and bond angles, occurring on interaction with other molecules, are discussed.     

The conformational analysis of adenosine triphosphate by classical potential energy calculations

The conformational analysis of adenosine triphosphate was conducted by using classical potential energy calculations. All rotatable bonds were examined, i.e., no dihedral angles were fixed at predetermined conformations except for the ribofuranose ring, which was held in the C(3′)-endo conformation—the conformation observed for adenosine in the crystal state. The energy terms included in the total energy expression consist of nonbonded pairwise interaction, electrostatic pairwise interaction, free energy of solvation, and torsional bond potentials. Two separate approaches were used in the conformational analyses. The first consisted of a sequential fragment approach were four bonds were rotated simultaneously at 30° increments. Each fragment overlapped the preceding one by at least one bond. All rotors were then simultaneously examined at their minima and at ±15°. The second approach consisted of a coarse grid search where all rotors were examined simultaneously, but only at staggered positions. The low-energy conformations thus obtained were then used as starting conformations for a minimization routine based on the method of conjugate directions. The first approach required about 40 hr of central processing unit (CPU) computer time, while the coarse grid/minimization approach required about 4 hr of CPU time. Both the sequential fragment approach and the minimization approach yielded lowest-energy conformations which are remarkably similar to the solid-state conformation of C(3′)-endo ATP.     

Necessary conditions for avoiding incorrect polypeptide folds in conformational search by energy minimization

Low energy conformations have been generated for melittin, pancreatic polypeptide, and ribonuclease S-peptide, both in the vicinity of x-ray structures by energy refinement and by an unconstrained search over the entire conformational space. Since the structural polymorphism of these medium-sized peptides in crystal and solution is moderate, comparing the calculated conformations to x-ray and nmr data provides information on local and global behavior of potential functions. Local analysis includes standardization calculations, which show that models with standard geometry can approximate good resolution x-ray data with less than 0.5 Å rms deviation (RMSD). However, the atomic coordinates are shifted up to 2 Å RMSD by local energy minimization, and thus 2 Å is generally the smallest RMSD value one can target in a conformational search using the same energy evaluation models. The unconstrained search was performed by a buildup-type method based on dynamic programming. To accelerate the generation of structures in the conformational search, we used the ECEPP potential, defined in terms of standard polypeptide geometry. A number of low energy conformations were further refined by relaxing the assumption of standard bond lengths and bond angles through the use of the CHARMM potential, and the hydrophobic folding energies of Eisenberg and McLachlan were calculated. Each conformation is described in terms of the RMSD from the native, hydrogen-bonding structure, solvent-acessible surface area, and the ratio of surfaces corresponding to nonpolar and polar residues. The unconstrained search finds conformations that are different from the native, sometimes substantially, and in addition, have lower conformational energies than the native. The origin of deviations is different for each of the three peptides, but in all examples the refined x-ray structures have lower energies than the calculated incorrect folds when (1) the assumption of standard bond lengths and bond angles is relaxed; (2) a small and constant effective dielectric permittivity (ε < 10) is used; and (3) the hydrophobic folding energy is incorporated into the potential. © 1993 John Wiley & Sons, Inc.     

Synthetic and conformational studies on dehydroalanine-containing model peptides

Three model dipeptides containing a dehydroalanine residue (delta Ala) at the C-terminal, Boc-X-delta Ala-NHCH3 [X = Ala, Val, and Phe,] have been synthesized and their solution conformations investigated by 1H-NMR, IR, and CD spectroscopy. NMR studies on these peptides in CDCl3 clearly indicate that the NH group of dehydroalanine is involved in an intramolecular hydrogen bond. This conclusion is supported by IR studies also. Nuclear Overhauser effect (NOE) studies are also accommodative of an inverse gamma-turn-type of conformation that is characterized by conformational angles of phi approximately -70 degrees and psi approximately +70 degrees around the X residue, and a C alpha i + 1 H-Ni + 2H interproton distance of 2.5 A. It appears that unlike dehydrophenylalanine or dehydroleucine, which tend to stabilize beta-turn type of structures occupying the i + 2 position of the turn, dehydroalanine favors the formation of an inverse gamma-turn, centered at the preceding L-residue in such solvents as CDCl3 and (CD3)2SO. A comparison of solution conformation of Boc Val-delta Ala-NHCH3 with the corresponding saturated analogue, Boc-Val-Ala-NHCH3, is also presented and shows that dehydroalanine is responsible for inducing the turn structure. It may be possible to design peptides with different preferred conformations using the suitable dehydroamino acid.     

Conformational analysis of the anomeric forms of kojibiose, nigerose, and maltose using MM3

Energy surfaces were computed for relative orientations of the relaxed pyranosyl rings of the two anomeric forms of kojibiose, nigerose, and maltose, the (1 → 2)-, (1 → 3)-- and (1 → 4)--linked -glucosyl disaccharides, respectively. Twenty-four combinations of starting conformations of the rotatable side-groups were considered for each disaccharide. Optimized structures were calculated using MM3 on a 20° grid spacing of the torsional angles about the glycosidic bonds. The energy surfaces of the six disaccharides were similar in many respects but differed in detail within the low-energy regions. The maps also illustrate the importance of the exo-anomeric effect and linkage type in determining the conformational flexibility of disaccharides. Torsional conformations of known crystal structures of maltosyl-containing molecules lie in a lower MM3 energy range than previously reported.     

New methodology for computer-aided modelling of biomolecular structure and dynamics. 1. Non-cyclic structures

A general methodology is proposed for the conformational modelling of biomolecular systems. The approach allows one: (i) to describe the system under investigation by an arbitrary set of internal variables, i.e., torsion angles, bond angles, and bond lengths; it offers a possibility to pass from the free structure to a completely fixed one with the number of variables from 3N to zero, respectively, where N is the number of atoms; (ii) to consider both, a single molecule and a complex of many molecules, (e.g., proteins, water, ligands, etc.) in terms of one universal model; (iii) to study the dynamics of the system using explicit analytical Lagrangian equations of motion, thus opening up possibilities for investigations of slow concerted motions such as domain oscillations in proteins etc.; (iv) to calculate the partial derivatives of various functions of conformation, e.g., the conformational energy or external constraints imposed, using a standard efficient procedure regardless of the variables and the structure of the system. The approach is meant to be used in various investigations concerning the conformations and dynamics of biomacromolecules.     

Parallel and antiparallel aggregation of alpha-helices. Crystal structures of two apolar decapeptides X-Trp-Ile-Ala-Aib-Ile-Val-Aib-Leu-Aib-Pro-OMe (X = Boc, Ac)

An apolar helical decapeptide with different end groups, Boc- or Ac-, crystallizes in a completely parallel fashion for the Boc-analog and in an antiparallel fashion for the Ac-analog. In both crystals, the packing motif consists of rows of parallel molecules. In the Boc-crystals, adjacent rows assemble with the helix axes pointed in the same direction. In the Ac-crystals, adjacent rows assemble with the helix axes pointed in opposite directions. The conformations of the molecules in both crystals are quite similar, predominantly alpha-helical, except for the tryptophanyl side chain where chi 1 congruent to 60 degrees in the Boc- analog and congruent to 180 degrees in the Ac-analog. As a result, there is one lateral hydrogen bond between helices, N(1 epsilon)...O(7), in the Ac-analog. The structures do not provide a ready rationalization of packing preference in terms of side-chain interactions and do not support a major role for helix dipole interactions in determining helix orientation in crystals. The crystal parameters are as follow. Boc-analog: C60H97N11O13.C3H7OH, space group Pl with a = 10.250(3) A, b = 12.451(4) A, c = 15.077(6) A, alpha = 96.55(3) degrees, beta = 92.31(3) degrees, gamma = 106.37(3) degrees, Z = 1, R = 5.5% for 5581 data ([F] greater than 3.0 sigma(F)), resolution 0.89 A. Ac-analog: C57H91N11O12, space group P2(1) with a = 9.965(1) A, b = 19.707(3) A, c = 16.648(3) A, beta = 94.08(1), Z = 2, R = 7.2% for 2530 data ([F] greater than 3.0 sigma(F)), resolution 1.00 A.     

Role of N-t-Boc group in helix initiation in a novel tetrapeptide.

Protecting groups in N- and C-terminal positions play a decisive role in the conformational preference of smaller peptides. Conformational analysis of tetrapeptide derivatives containing Ala, Ile and Gly residues was performed. Peptide 1, Boc-Ala-Ile-Ile-Gly-OMe (Boc: tert-butyloxycarbonyl) has a predominantly helical turn conformation in all the alcoholic solvents studied, whereas in the solid state it has a beta-sheet conformation. In contrast, peptide 2, Ac-Ala-Ile-Ile-Gly-OMe (Ac: acetyl) has a random coil conformation in solution. The FTIR spectrum of peptide 1 shows a lower frequency of urethane carbonyl, indicating involvement of the carbonyl group in hydrogen bonding in the helical turn.     

Solid-state geometry and conformation of linear,diastereoisomeric oligoprolines

We have carried out a systematic analysis of the solid-state conformational preferences of a number of linear homo-oligoprolines (to the tetramer) by ir absorption and x-ray diffraction. The peptides present different chiral sequences (tacticities), various types (urethane and amide) of N-protecting groups, and free and blocked C-termini (which imply different capabilities of forming H-bonds). The following conclusions can be drawn: (i) values for the geometry of the prolyl residue and the peptide bond in the cis and in the trans conformations are proposed; (ii) in general the conformational angles φ and ψ in the linear homo-oligoprolines have values appropriate for the polyproline II structure (conformation F); (iii) the pyrrolidine ring shows various types of puckering with no apparent relation to the backbone conformation; (iv) Pro-Pro peptide bonds generally take the trans conformation, the few cases of cis conformation being formed by Pro residues of different chirality; (v) the single H-bond donor — OH, when present, is always bonded to H-acceptors, which can be either the urethane or the amide or the peptide carbonyl but never the carbonyl group of the — COOH moiety.