Conformational geometry and vibrational frequencies of nucleic acid chains.

Normal coordinate analysis of diethyl phosphate has been made, which predicts all observed Raman frequencies in the range 170–1300 cm^?1. The force constants from this calculation have been transferred to a vibrational calculation for a simplified model of the backbone of nucleic acids, which also involves the ? O? PO₂^?? O phosphate group and the ? C₅′? C₄′? C₃′? linkage of the ribose. The coordinates of these atoms are those recently given by Arnott and Hukins, which place the ribose ring of B-DNA in a C₃′-exo conformation. This simple polymer model appears to be able to describe adequately the frequency-dependent changes observed in the Raman spectra arising from the backbone vibrations of nucleic acid in going from the B- to A-form. The symmetric ? O? P? O? diester stretch increases in frequency from about 787 cm^?1 in the B-form to 807 cm^?1 in the A-form. The increased frequency characteristic of the A-form is due to the combining of the diester stretch with vibrations involving the C₅′, C₄′, and C₃′ nuclei. The frequency of the symmetric ? O? P? O? diester stretch is shown to be very dependent on the conformation of the ribose ring, indicating that in polynucleotides the ribose ring takes on one of two rigid conformations: C₃′-endo for A-form or C₃′-exo for B-form and “disordered” polynucleotides. The calculation lends confirmation to the atomic coordinates of Arnott and Hukins since the use of other geometries with the same force constants failed to give results in agreement with experimental evidence. The calculations also demonstrate the lowering effect of hydration on the anionic PO stretching frequencies. Experimental results show that the 814-cm^?1 band observed in the spectra of 5′GMP gel arises from a different vibrational mode than that of the 814-cm^?1 band of A-DNA.     

Multinuclear magnetic resonance studies of monomers and dimers containing 2'-fluoro-2'-deoxyadenosine

A series of 2′-fluorinated adenosine compounds, dAfl, dAflp, pdAfl, dAfl-A, A-dAfl, and dAfl-dAfl, have been investigated by nmr spectroscopies. The ¹H-, ¹⁹F-, and ³¹P-nmr data provide structural information from different parts of these moleucles. The pK_a of the phosphate group of these two 2′-fluoro-2′-deoxyadenosine monophosphates was found to be the same as that of hte parent adenosine monophosphate. As for the pentose conformation, the ³E population is greatly increased as a result of the fluorine substitution at the C_2′ position. However, the populations of conformers of gg (C_4′-C_5′) and g′g′ (C_5′-O_5′) and the average angle ?′(C_3′-O_3′) of the 2′-fluoro compounds remain unchanged as compared to the natural riboadenosine monomer and dimer (A-A). Thefefore, the backbone conformation of the 2′-fluoro-2′-deoxy-adenosine, its monophosphates and dimers, resembles that of RNA. The extent of base-base overlapping in these 2′-fluoro-2′-deoxy-adenosine-containing dimers is also found to be similar to or even greater than A-A. Thus, the conformations of these compounds can be considered as those in the RNA family. These fluorocompounds also serve as models for a careful study on the ¹⁹F-nmr in nucleic acid. The ¹⁹F chemical-shift values are sensitive to the environment of the fluorine atom such as ionic structure of the neighboring group(s) (phosphate of base), solvation, and ring-ruccent anisotropic effect from the base(s). Qualitatively, the change of the ¹⁹F chemical-shift values (up to 2 ppm) is much larger than that of ¹H-nmr (up to 0.5 ppm) in the dimers. Using dAfl·poly(U), poly(dAfl)·poly(dAfl), and poly(dAfl)·poly(U) helix–coil transition as model systems, the linewidth of ¹⁹F in dAfl- residues reflects effectively the mobility of the unit in the nucleic acid complex as calibrated by uv data and by ¹H-nmr. Therefore, application of ¹⁹F-nmr spectroscopy on fluorine-substituted nucleic acid can also be used to detect nucleic acid-nucleic acid interaction in complicated systems.     

Proton and phosphorus magnetic relaxation studies on the dynamic structure of single-stranded polyriboadenylic acid

Proton and phosphorus-31 nuclear spin-lattice relaxation times (T₁) have been measured with the Fourier-transform method at 100 and 40.5 MHz, respectively, on single-stranded polyriboadenylic acid (poly(A)) in a neutral D₂O solution in the temperature range of 14–82°C. T₁ minimum is observed around 35–45°C for H(8), H(1′), and phosphorus resonances. Rotational correlation times have been deduced from the T₁ data, which indicate that the sugar–phosphate backbone as well as the base–sugar segment is undergoing rapid internal motion of 10^?8–10^?10 sec range. The molecular motion of the sugar–phosphate backbone as deduced from the phosphorus relaxation is well-characterized by a single activation enthalpy of 8.1 kal/mole for the whole temperature range of 14–82°C. Activation enthalpies of similar magnitude have been obtained for the motion of the adenine–ribose moiety from H(8) and H(1′) relaxation. The relative magnitude of T₁ for H(8) and H(1′) infers that the poly(A) nucleotide exists on the average as anti in the single-stranded form. The phosphorus T₁ value is consistent with a conformation such that both C(4′)–C(5′) and C(4′)–C(3′) bonds are nearly trans to their connected O–P bonds.     

The role of water in the crystal structure of N-acetyl-L-4-hydroxyproline

The crystal structure of N-acetyl-L -4-hydroxyproline (Hyp) was determined by direct methods. (The crystal is orthorhombic with the space group P2₁2₁2₁.) The acetyl group is in the trans conformation and the pyrrolidine ring puckers at C^γ (C^sC^γ envelope), as in most Hyp residues. According to the rotation angle ψ = ?30°, the N-acetyl-L -4Hyp has the same conformation as an α-helix of prolyl residues. The crystal packing is stabilized by hydrogen bonds between three different molecules and the same molecule of water. One of the water bridges involves the carbonyl of the N-acetyl group of one molecule and the hydrogen atom of the 4-OH group of another. Such an arrangement has been proposed to explain the high stability of (Gly-L -Pro-L -4Hyp)_n. A second bridge involves the two hydrogens of the water molecule and the carbonyl groups of two neighbouring molecules, as already proposed in a dihydrated model of collagen. These experimental features, which are discussed in relation to the different models of collagen, allow us to propose an hypothetical arrangement for the water molecule which is strongly retained in the triple helix of (Gly-L -Pro-L -4Hyp)_n.     

Nuclear magnetic resonance study of ring conformations of cyclic tetradepsipeptide AM-toxins and related peptides

Cyclic tetradepsipeptides, AM-toxin I and II, are the host-specific phytotoxins of Alternaria mali. In order to elucidate conformation-toxicity relationships, we analyzed the 270-MHz proton nmr spectra of AM-toxins and hydrogenated analogs, (D -Ala²)AM-toxin I (toxic) and (L -Ala²)AM-toxin I (not toxic), in (C²H₃)₂SO. These cyclic tetradepsipeptides do not contain N-substituted amino acid residues, and all the peptide and ester groups have been found to be transoid. Two conformers with very unequal populations have been found for AM-toxin I and II; the C^β?C^α? C?O conformations of the Dha² residues are nonplanar S-trans in the major conformer and nonplanar S-cis in the minor conformer. Only one ring conformation has been found for each of (L -Ala²) and (D -Ala²)AM-toxin I. (L -Ala²)AM-toxin I takes a C₄-type ring conformation; all the C?O groups and C^α-H bonds are oriented to the same side of the ring. (D -Ala²)AM-toxin I takes a new ring conformation; the side chain and C?O group of the L -Amp¹ residue are oriented to the same side of the ring. This new conformation is also found for the major conformers of AM-toxin I and II and thus appears to be required for the toxicity. The ring conformations of Tyr(OCH₃)¹-bearing analog tetradepsipeptides have been found to be much the same as those of Amp¹-bearing depsipeptides. Furthermore, on the basis of the two distinct conformations of (D -Ala²) and (L -Ala²)AM-toxin I, an empirical rule is proposed for the stable ring conformations of cyclic tetra-D ,L -peptides, not containing N-substituted amino acid residues.     

Crystal structure and solution conformation of 1-N-acetyl-β-D-glucopyranosyl amine: A model for the glycopeptide linkage

The crystal structure of the title compound, a model for the glycosyl linkage between the asparagine side chain and N-acetyl glucosamine in glycoproteins, has been determined and compared to other model structures. The pyranose ring in the crystal is in the ⁴C₁ chair conformation and the amide functions at C₁ and at C₂ are both oriented such that the amide protons are nearly trans to their respective sugar-ring protons. Coupling constants determined from the fully assigned proton nmr spectrum in aqueous solution are consistent with the conformation in the crystal.     

Crystal structure and conformation of a cyclic tetrapeptide cyclo(L-Pro-Sar)2 containing all-cis peptide units

The crystal structure and conformation of the synthetic cyclic tetrapeptide, cyclo(L -Pro-Sar)₂, was determined by x-ray analysis. The peptide crystallizes in the orthorhombic space group P2₁2₁2₁ with cell parameters a = 9.277(1), b = 12.884(1), and c = 15.581(2) Å. The crystal structure was solved by the symbolic addition procedure for direct phase determination and least-squares refinement using 1796 reflections, which led to the final R value of 0.043. This structure provides the first example observed in a crystal of a cyclic tetrapeptide in which all four peptide units have been found in the cis conformation with ω angles deviating slightly by 2°–10° from the ideal value of 0°. It was also found that the two Pro C^α-CO single bonds assumed a trans′ (ψ = 159.6° and 158.4°) conformation. Adjoining average planes of the peptide groups fall at nearly right angles to each other. The pyrrolidine ring conformations of the two prolyl residues are in the envelope form, with C^γ carbon out of the least-squares planes for the remaining four atoms.     

Conformational studies of a bicyclic,lactam‐constrained parathyroid hormone‐related protein‐derived agonist

The N‐terminal 1–34 segments of both parathyroid hormone (PTH) and parathyroid hormone‐related protein (PTHrP) bind and activate the same membrane receptor in spite of major differences in their amino acid sequence. The hypothesis was made that they share the same bioactive conformation when bound to the receptor. A common structural motif in all bioactive fragments of the hormone in water/trifluoroethanol mixtures or in aqueous solution containing detergent micelles is the presence of two helical segments at the N‐ and C‐termini of the sequence. In order to stabilize the helical structures, we have recently synthesized and studied the PTHrP(1–34) analog [(Lys13–As p¹⁷, Lys26–As p³⁰)]PTHrP(1–34)NH₂, which contains lactam‐constrained Lys‐Asp side chains at positions i, i+4. This very potent agonist exhibits enhanced helix stability with respect to the corresponding linear peptide and also two flexible sites at positions 12 and 19 in 1:1 trifluoroethanol/water. These structural elements have been suggested to play a critical role in bioactivity. In the present work we have extended our conformational studies on the bicyclic lactam‐constrained analog to aqueous solution. By CD, 2D‐NMR and structure calculations we have shown that in water two helical segments are present in the region of the lactam bridges (13–18, and 26–31) with high flexibility around Gly¹² and Arg¹⁹. Thus, the essential structural features observed in the aqueous‐organic medium are maintained in water even if, in this solvent, the overall structure is more flexible. Our findings confirm the stabilizing effect of side‐chain lactam constraints on the α‐helical structure. Copyright © 1999 European Peptide Society and John Wiley & Sons, Ltd.     

Conformational Preferences of Modified Nucleoside N(4)-Acetylcytidine, ac4C Occur at “Wobble” 34th Position in the Anticodon Loop of tRNA

Conformational preferences of modified nucleoside, N(4)-acetylcytidine, ac⁴C have been investigated using quantum chemical semi-empirical RM1 method. Automated geometry optimization using PM3 method along with ab initio methods HF SCF (6-31G**), and density functional theory (DFT; B3LYP/6-31G**) have also been made to compare the salient features. The most stable conformation of N(4)-acetyl group of ac⁴C prefers “proximal” orientation. This conformation is stabilized by intramolecular hydrogen bonding between O(7)···HC(5), O(2)···HC2′, and O4′···HC(6). The “proximal” conformation of N(4)-acetyl group has also been observed in another conformational study of anticodon loop of E. coli elongator tRNA^Met. The solvent accessible surface area (SASA) calculations revealed the role of ac⁴C in anticodon loop. The explicit molecular dynamics simulation study also shows the “proximal” orientation of N(4)-acetyl group. The predicted “proximal” conformation would allow ac⁴C to interact with third base of codon AUG/AUA whereas the ‘distal’ orientation of N(4)-acetyl cytidine side-chain prevents such interactions. Single point energy calculation studies of various models of anticodon–codon bases revealed that the models ac⁴C₍₃₄₎(Proximal):G₃, and ac⁴C₍₃₄₎(Proximal):A₃ are energetically more stable as compared to models ac⁴C₍₃₄₎(Distal):G₃, and ac⁴C₍₃₄₎(Distal):A₃, respectively. MEPs calculations showed the unique potential tunnels between the hydrogen bond donor–acceptor atoms of ac⁴C₍₃₄₎(Proximal):G₃/A₃ base pairs suggesting role of ac⁴C in recognition of third letter of codons AUG/AUA. The “distal” conformation of ac⁴C might prevent misreading of AUA codon. Hence, this study could be useful to understand the role of ac⁴C in the tertiary structure folding of tRNA as well as in the proper recognition of codons during protein biosynthesis process.     

The conformation of tetrafluorinated methyl galactoside anomers: crystallographic and NMR studies

The first single-crystal X-ray diffraction study of tetrafluorinated monosaccharide derivatives is presented. Both α- and β-methyl 2,3-dideoxy-2,2,3,3-tetrafluoro-d-galactopyranoside anomers adopt the ⁴C₁ conformation. The values for the C1–O1 and C1–O5 bond lengths and the O5–C1–O1–CH₃ dihedral angles are in line with what can be expected from the anomeric and exo-anomeric effects. The chair conformations are slightly distorted, presumably due to repulsion between 1,3-diaxial C–O and C–F bonds. The asymmetric unit of both compounds contains up to three independent molecules, which differ in the conformation of the hydroxymethyl group (including in one case a ‘forbidden’ gg rotamer). The molecular packing of the β-anomer shows a clear segregation between fluorinated and hydrophilic domains, while for the α-anomer the regions of fluorine segregation are broken by interleafing of OMe groups. There is one close OH?F contact, which is likely to arise from the crystal packing. NMR studies show that the two anomers also adopt a ⁴C₁ conformation in solution (D₂O, CDCl₃).     

Flexibility of DNA and RNA upon Binding to Different Metal Cations. An Investigation of the B to A to Z Conformational Transition by Fourier Transform Infrared Spectroscopy

Abstract

The interaction of DNA and RNA with Cu(II), Mg(II), [Co(NH₃)₆]³⁺ [Co(NH₃)₅Cl]²⁺ chlorides and, cis- and trans-Pt(NH₃)₂Cl₂ (CIS-DDP, trans-DDP) has been studied by Fourier Transform Infrared (FT-IR) spectroscopy and a correlation between metal-base binding and conformational transitions in the sugar pucker has been established. It has been found that RNA did not change from A-form on complexation with metals, whereas DNA exhibited a B to Z transition. The marker bands for the A-form (C′₃-endo-anti conformation) were found to be near 810–816 cm^?1, while the bands at 825 and 690 cm^?1 are marker bands for the B- conformation (C′₂-endo, anti), The B to Z (C₃′-endo, syn conformation) transition is characterized by the shift of the band at 825 cm^?1 to 810–816 cm^?1 and the shift of the guanine band at 690 cm^?1 to about 600–624 cm^?1.     

Microcalorimetric studies of solvent-induced conformational change of sodium and cesium salts of poly(L-glutamic acid) in aqueous media

Organic solvent-induced coil → helix conformational change of poly(sodium) L -glutamate (NaPLG) and poly(cesium L -glutamate) (CsPLG) in solution in aqueous mixed solvents have been studied at 25°C. Heats of dilution of NaPLG in the water–dioxane pair have been measured as a function of polymer concentration and solvent composition. The results indicate that the overall chain conformation in the disordered form is not too different from that in the α-helical form. Heat capacity measurements by flow microcalorimetry have also been done. The apparent monomolar heat capacity at constant pressure of the polymer, C_{p, ?}, decreases with dilution similarly to other strong polyelectrolytes in aqueous media. In the water–dioxane pair, C_{p, ?} increases with the dioxane content due to partial desolvation of ionic species resulting from increasing ionic association. In the case of the water-2-chloroethanol (CE) pair, the transition takes place at low CE content and results show a fast decrease in C_{p, ?} when the α-helical conformation predominates. It is believed carboxylate groups and CE molecules associate themselves into a complex formation responsible for the transition. The size of the cation plays a significant role in the thermodynamic properties of these polyelectrolytes in solution since sodium ions are more strongly bound to the chain than cesium ions.     

Spectroscopic studies on the structure of poly(8-bromoadenylic acid): Effect of glycosidic torsion angle on the conformation and flexibility in polyribonucleotides

The helix–coil transition and conformational structure of poly(8-bromoadenylic acid) [poly(8BrA)] have been investigated using ¹H- and ¹³C-nmr, CD, and ir spectroscopy. The results have been compared with the structure of the related 5′-mono- and polynucleotides. The chemical shifts of H(2′), H(3′), C(2′), and C(3′) nmr signals show an interesting correlation with both the puckering of ribose ring and glycosidic bond torsion angle. Poly(8BrA) shows an upfield shift of the C(3′) signal and a downfield shift of the H(3′) signal compared to the chemical shifts in poly(A). These shifts are consistent with a C(3′) endo-syn conformation for poly(8BrA). A similar effect has been reported previously and is also observed here on the C(2′) and H(2′) signals when the preferred conformation is C(2′)endo-syn (e.g., in 5′-8BrAMP). The chemical-shift parameters thus act as a probe for studying syn ? anti and N ? S equilibria in solutions. The three-bond ¹H-′¹³C coupling constants between H(1′) and C(8) and C(4) have been measured in poly(8BrA) and 5′-8BrAMP and their structural implications have been discussed. The observed preference of a C(3′)endo-syn conformation for poly(8BrA), coupled with other evidence, throws doubt on the validity of a correlation previously reported whereby a syn conformation is associated with a C(2′)endo ribose pucker. The backbone conformation of randomly coiled poly(8BrA) is very similar to the structures found in polyribonucleotides: poly(A) and poly(U). All three polymers show strong preferences for the backbone angles found in RNA helices. The CD spectrum of poly(8BrA) has a striking relationship to that of poly(A). The signs of all extrema are inverted, and the magnitudes are related by a constant factor. We suggest that these differences result from a change in the angle between coupled transition moment vectors in the two polymers. Infrared spectra of poly(8BrA) in H₂O and D₂O solution are reported for the frequency range below 1400 cm^?1. The antisymmetric >PO stretching vibration is observed at an unusually low frequency in the helix (1214 cm^?1). The symmetric >PO stretch occurs at ～1095 cm^?1 but is not resolved from a ring vibration near this frequency. A conformationally sensitive band, characteristic of helical RNA structures, is observed at 817 cm^?1 and disappears when the helix is melted. This observation confirms the conclusion that ordered poly(8BrA) has a regular helical structure with an RNA backbone conformation. A stereochemical explanation is provided for the failure of poly(8BrA) (or other syn polymers) to form double helices with anti-polyribonucleotides.     

Conformational effects on peptide aggregation in organic solvents: spectroscopic studies of two chemotactic tripeptide analogs

The aggregation behavior of the chemotactic peptide analogs, Formyl-Met-Leu-Phe-OMe ( 1 ) and Formyl-Met-Aib-Phe-OMe ( 2 ), has been studied in chloroform and dimethylsulfoxide over the concentration range of 0.2–110 mM by ¹H-nmr spectroscopy. Both peptides associate in CDCl₃ at concentrations ≥ 2 mM, while there is no evidence for aggregation in (CD₃)₂SO. Analog 1 adopts an extended conformation in both solvents favoring association to form β-sheet structures. A folded, γ-turn conformation involving a 3 → 1 hydrogen bond between Met CO and Phe NH is supported by ¹H-, ¹³C-nmr, and ir studies of analog 2 . The influence of backbone conformation on the ease of peptide aggregation is demonstrated by ir studies in CHCl₃ and CD studies in dioxane.     

The crystal state conformation of Aib-rich segments of peptaibol antibiotics

Ac-(Aib-Ala)₃-OH (a protected segment of the peptaibols gliodeliquescin and paracelsin), Z-Leu-Aib-Val-Aib-Gly-OtBu (a segment of [Leu]⁷-gliodeliquescin), Z-Val-Aib-Aib-Gln-OtBu (a common segment of alamethicin, paracelsin, and hypelcin), and Ac-Aib-Pro-(Aib-Ala)₂-OMe and Z-Aib-Pro-(Aib-Ala)₂-OMe, which represent differently N^α-protected 1–6 segments of alamethicin and hypelcin, have been synthesized by solution methods. The crystal-state conformations of these five Aib-containing peptides have been determined by X-ray diffraction analysis. We have confirmed that the 3₁₀-helical structure is preferentially adopted by Aib-rich short peptides. An experimentally unambiguous proof for the 3₁₀→α-helix conversion has been provided by the two differently N-blocked -Aib-Pro-(Aib-Ala)₂-OMe hexapeptides. The β-bend ribbon conformation, commonly observed in the (Aib-Pro)_n sequential oligopeptides, is not found in the -Aib-Pro-Aib-Ala-Aib-Ala- sequence. As expected on the basis of the l -configuration of the C^α-monoalkylated residues, a right-handed helix screw sense was found in all peptides investigated. © 1998 European Peptide Society and John Wiley & Sons, Ltd.     

Conformations of cyclic peptide/calcium complexes in solution

Synthetic cyclic octapeptides of general structure cyclo[Glu(γOBzl)-Sar-Gly-(N-R)Gly]₂ (R = n-hexyl and cyclohexyl) transport calcium ions selectively across organic phases and phospholipid membranes. We have now used proton nmr spectroscopy (360 MHz) to study the solution conformation(s) of their calcium complexes. When Ca(ClO₄)₂ was added to solutions of these peptides in CDCl₃, nmr spectra of the resulting calcium complexes were characteristic of a single C₂-symmetric conformer. From a Karplus-Bystrov analysis of vicinal coupling constants in both the peptide backbone and Glu side chain (treated as an ABCC′MX spin system), in conjuction with model-building studies, a structure was proposed in which the calcium ion is bound in an octahedral-type complex by the four (coplanar) carbonyl groups of the (all-trans) Glu-Sar and Gly-(N-R)Gly peptide bonds. Occurrence of preferred rotamers about Glu side chain C^α–C^β bonds indicated that restricted rotation in peptide side chains arises upon calcium binding.     

Conformational behaviour of A cyclolinopeptide a analogue: Two-dimensional NMR study of cyclo(Pro1-Pro-Phe-Phe-Ac6c-IIe-ala-Val8)

The cyclic octapeptide cyclo[-Pro¹-Pro-Phe-Phe-Ac₆c-Ile-ala-Val⁸-] [C₈-Ac₆c], containing the Pro¹-Pro-Phe-Phe sequence, followed by a bulky helicogenic C^α,α-dialkylated glycine residue Ac₆c (1-aminocyclohexane-1-carboxylic acid), and a _D-Ala residue at position 7 has been synthesized. This cyclic peptide is a deletion analogue of the naturally occurring cyclic nonapeptide cyclolinopeptide A (CLA). It has been designed with the aim of studying the role that the Ac₆c and _D-Ala residues play on the conformational behaviour of the whole molecule and their influence on the conformation of the Pro¹-Pro-Phe-Phe sequence when compared with cyclolinopeptide A. C₈Ac₆c has been investigated in chloroform and acetonitrile solutions by 2D NMR techniques. Only one set of sharp signals is observed in both solvents. This evidence strongly supports the hypothesis that only one conformational state exists in the chosen solvents. The interpretation of the experimental data points to the existence for C₈-Ac₆c of a very rigid structure stabilized by intramolecular hydrogen bonds. The measured NOE effects allow the calculation of internuclear distances, which have been used as restraints in molecular dynamic calculations. The proposed conformation of the molecule shows that the Pro-Pro-Phe segment retains the conformation observed in natural CLA both in solution and in the solid state and that the Ac₆c residue indeed reinforces the ring rigidity not permitting the formation of any appropriate cavity in which inorganic cations could be complexed.     

Experimental investigations on the backbone folding of proline-containing model tripeptides

Some proline-containing tripeptides with the general formulas R⁰CO-L -Pro-X-NHR³ (X = Gly,Sar,L -Ala,D -Ala) and R⁰CO-X-L -Pro-NHR³ (X = Gly,L -Ala,D -Ala) have been investigated in solution by ir and ¹H-nmr spectroscopies. Their favored conformational states depend mainly on both the primary structure and the chiral sequence of the molecules. In inert solvents the βII-folding mode is the most favored conformation for the L -Pro-D -Ala and L -Pro-Gly tripeptides, while the βII′-turn is largely preferred by D -Ala-L -Pro derivatives. Under the same conditions only about one-third of the whole conformers of L -Pro-L -Ala molecules adopts the βI-folding mode. Semiopened C₇C₅ and C₅C₇ conformations are appreciably populated in the L -Pro-L -Ala sequence, on the one hand, and in the Gly-L -Pro and L -Ala-L -Pro derivatives, on the other hand. In L -Pro-Sar and X-L -Pro models, the cis–trans isomerism around the middle tertiary amide function is observed. Thus cis L -Pro-Sar and L -Ala-L -Pro conformers are folded by an intramolecular i + 3 → i hydrogen bond, whereas cis D -Ala-L -Pro and Gly-L -Pro molecules accommodate an open conformation. In dimethylsulfoxide the βII- and βII′-folding modes are not essentially destabilized, as contrasted with the βI conformation, which is less populated. In water solution all the above-mentioned conformations, with the possible exception of the βII′-folding mode for D -Ala-L -Pro molecules, seem to vanish. Solute conformations are also compared with the crystal structures of four proline-containing tripeptides.     

Crystal structures of diketopiperazines containing α-aminoisobutyric acid: Cyclo(Aib-Aib) and cyclo(Aib-L-Ile)

The crystal and molecular structures of two α-aminoisobutyric acid (Aib)-containing diketopiperazines, cyclo(Aib-Aib) 1 and cyclo(Aib-L -Ile) 2 , are reported. Cyclo(Aib-Aib) crystallizes in the space group P1 with a = 5.649(3), b = 5.865(2), c = 8.363(1), α = 69.89(6), β = 113.04(8), γ = 116.0(3), and Z = 1, while 2 occurs in the space group P2₁2₁2₁ with a = 6.177(1), b = 10.791(1), c = 16.676(1), and Z = 4. The structures of 1 and 2 have been refined to final R factors of 0.085 and 0.086, respectively. In both structures the diketopiperazine ring shows small but significant deviation from planarity. A very flat chair conformation is adopted by 1, in which the C^α atoms are displaced by 0.07 Å on each side of the mean plane, passing through the other four atoms of the ring. Cyclo(Aib-Ile) favors a slight boat conformation, with Aib C^α and Ile C^α atoms displaced by 0.11 and 0.05 Å on the same side of the mean plane formed by the other ring atoms. Structural features in these two molecules are compared with other related diketopiperazines.     

Molecular dynamics study of iduronate ring conformation

Molecular dynamics (MD) simulations of the conformation of the iduronate ring in a methyl glycoside and as the central residue in a trisaccharide have been carried out. Separate simulations were carried out with initial ¹C₄, ²S₀, and ⁴C₁ iduronate ring conformations. Simulations were followed by observing the time development of the Cremer–Pople ring puckering parameters θ,?₂. Starting with chair geometries gave trajectories showing only ring oscillations close to the initial geometry. Simulations were performed with a ²S₀ starting geometry using explicit water and in vacuum with dielectric constants (ε) of 1 and 80, as well as with distance-dependent dielectric functions of 2r and 4r. In both the explicit water simulation and the vacuum (ε = 80) simulations, extensive pseudorotational motion was observed in which boat and twist-boat ring conformers interconvert. The overall range of ?₂2 variation in the trisaccharide was about half of that observed in the methyl glycoside. The Haasnoot procedure for calculating H-H coupling constants in saccharides was applied to structures obtained from MD trajectories. Using MD time averaged couplings along with experimental data allowed the relative fractions of chair and boat/twist-boat forms to be derived. © 1993 John Wiley & Sons, Inc.