Crystal structure and molecular conformation of achatin-I (H-Gly-D-Phe-Ala-Asp-OH), an endogenous neuropeptide containing a D-amino acid residue.

In order to investigate the active conformation of achatin-I (H-Gly-D-Phe-Ala-Asp-OH), an endogenous neuropeptide from the Achatina fulica ganglia, its crystal structure and molecular conformation were analysed by the X-ray diffraction method. Crystals from methanol/dioxane are monoclinic, space group P2(1) with a = 5.083(1), b = 9.125(1), c = 20.939(3) A, beta = 94.73(1) degrees. The structure was solved by direct methods and refined to R = 0.051 for 1714 independent reflections with /Fo/ greater than sigma (Fo). The molecule exists as a zwitterion with the Gly N-terminal end protonated and Asp beta-carboxyl deprotonated; the C-terminal of Asp is in a neutral state. The molecule takes a kind of beta turn structure with the D-Phe-Ala residues at the corner of the bend. This turn conformation is primarily formed by the strong intramolecular hydrogen bonds of NH(Gly)...O delta 1 (Asp) and NH(Asp)...O delta 1 (Asp) pairs, thus forming a 15-membered ring structure. Judging from the published data concerning the structure-activity relationship, this turn conformation may reflect an important feature related to the neuroexcitatory activity of achatin-I.     

NMR study on the binding of neuropeptide achatin-I to phospholipid bilayer: the equilibrium, location, and peptide conformation

Molecular mechanism of the binding of neuropeptide achatin-I (Gly-D-Phe-Ala-Asp) to large unilamellar vesicles of zwitterionic egg-yolk phosphatidylcholine (EPC) was investigated by means of natural-abundance (13)C and high-resolution (of 0.01 Hz order) (1)H NMR spectroscopy. The binding equilibrium was found to be sensitive to the ionization state of the N-terminal NH(3)(+) group in achatin-I; the de-ionization of NH(3)(+) decreases the bound fraction of the peptide from approximately 15% to nearly none. The electrostatic attraction between the N-terminal positive NH(3)(+) group and the negative PO(4)(-) group in the EPC headgroup plays an important role in controlling the equilibrium. Analysis of the (13)C chemical shifts (delta) of EPC showed that the binding location of the peptide within the bilayer is the polar region between the glycerol and ester groups. The binding caused upfield changes Delta delta of the (13)C resonance for almost all the carbon sites in achatin-I. The changes Delta delta for the ionic Asp at the C-terminus are more than five times as large as those for the other residues. The drastic changes for Asp result from the dehydration of the ionic CO(2)(-) groups, which are strongly hydrated by electrostatic interactions in bulk water. The side-chain conformational equilibria of the aromatic d-Phe and ionic Asp residues were both affected by the binding, and the induced changes in the equilibria appear to reflect the peptide-lipid hydrophobic interactions.     

Structure and conformation of peptides containing the sulfonamide junction. II. Synthesis and conformation of cyclo[-MeTau-Phe-DPro-]

By applying the method of amino-acyl incorporation to sulfonamido peptides, cyclo(-MeTau-Phe-DPro-) 3 has been synthesized in high yield starting from Z-MeTau-Phe-Pro-OH. The crystal structure and the molecular conformation of 3 have been determined. Crystals are orthorhombic, s.g. P2(1)2(1)2(1), with a = 5.454, b = 13.486, c = 24.025 A. The structure has been solved by direct methods and refined to R = 0.039 for 1974 reflections with I greater than 1.5 sigma (I). The 10-measured cyclopeptide adopts a backbone conformation in the crystals characterized by Phe-DPro and DPro-MeTau peptide bonds in trans and cis conformation, respectively. Both the peptide bonds deviate significantly from planarity and the corresponding [delta omega[ values are ca. 12 degrees. The sulfonamide SO2NH junction adopts a cisoidal conformation with a C alpha 1-S1-N2-C alpha 2 torsion angle of 70.8 degrees. 13C n.m.r. data show that the trans geometry at the Phe-DPro junction found in the crystals is retained in DMSO solution. The 10-membered ring of 3 is characterized by a pseudo mirror-plane passing through the Phe nitrogen and the DPro carbonylic carbon. The DPro ring adopts a half-chair conformation. The Phe side chain conformation corresponds to the statistically most favored g- rotamer (chi 1 = -68.6 degrees). The crystal packing is characterized by a weak intermolecular hydrogen bond between NH group and the MeTau O1' oxygen.     

L-Leucinamide hydrogensquarate: spectroscopic and structural elucidation

The hydrogensquarate [LeuNH(2)] (HSq) of L-leucinamide has been synthesized and its structure has been determined by single crystal X-ray diffraction. A three dimensional network is formed by hydrogen bonds with participation of the O=C-NH(2) function, the hydrogensquarate ion and the N(+)H(3) group [NH(2)...O=C((Sq)) (2.840 and 2.749 A), ((Sq))OH...O=C(NH(2)) (2.618 A), NH(3) (+)...O=C((Sq)) (3.246, 2.804 and 2.823 A)], respectively. A theoretical approximation of the electronic structure was carried out by means of ab initio UMP2 and MP2 level of theory at the 6-311++G** basis set. The IR-spectroscopic assignment in the solid-phase was obtained by linear-polarized IR-spectroscopy of oriented samples as colloid suspensions in a nematic host and application of the reducing-difference procedure for the interpretation of polarized IR-spectra.     

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.     

Switching of turn conformation in an aspartate anion peptide fragment by NH . . . O- hydrogen bonds

Aspartic acid protease model peptides Z-Phe-Asp(COOH)-Thr-Gly-Ser-Ala-NHCy (1) and AdCO-Asp(COOH)-Val-Gly-NHBzl (3), and their aspartate anions (NEt4)[Z-Phe-Asp(COO-)-Thr-Gly-Ser-Ala-NHCy] (2) and (NEt4)[AdCO-Asp(COO-)-Val-Gly-NHBzl] (4), having an invariant primary sequence of the Asp-X(Thr,Ser)-Gly fragment, were synthesized and characterized by 1H-NMR, CD, and infrared (IR) spectroscopies. NMR structure analyses indicate that the Asp O(delta) atoms of the aspartate peptide 2 are intramolecularly hydrogen-bonded with Gly, Ser, Ala NH, and Ser OH, supporting the rigid beta-turn-like conformation in acetonitrile solution. The tripeptide in the aspartic acid 3 forms an inverse gamma-turn structure, which is converted to a beta-turn-like conformation because of the formation of the intramolecular NH . . . O- hydrogen bonds with the Asp O(delta) in 4. Such a conformational change is not detected between dipeptides AdCO-Asp(COOH)-Va-NHAd (5) and (NEt4)[AdCO-Asp(COO-)-Val-NHAd] (6). The pK(a) value of side-chain carboxylic acid (5.0) for 3 exhibits a lower shift (0.3 unit) from that of 5 in aqueous polyethyleneglycol lauryl ether micellar solution. NMR structure analyses for 3 in an aqueous micellar solution indicate that the preorganized turn structure, which readily forms the NH . . . O- hydrogen bonds, lowers the pK(a) value and that resulting hydrogen bonds stabilize the rigid conformation in the aspartate anion state. We found that the formation of the NH . . . O- hydrogen bonds involved in the hairpin turn is correlated with the protonation and deprotonation state of the Asp side chain in the conserved amino acid fragments.     

Crystal structure of haloalkane dehalogenase LinB from Sphingomonas paucimobilis UT26 at 0.95 A resolution: dynamics of catalytic residues

We present the structure of LinB, a 33-kDa haloalkane dehalogenase from Sphingomonas paucimobilis UT26, at 0.95 A resolution. The data have allowed us to directly observe the anisotropic motions of the catalytic residues. In particular, the side-chain of the catalytic nucleophile, Asp108, displays a high degree of disorder. It has been modeled in two conformations, one similar to that observed previously (conformation A) and one strained (conformation B) that approached the catalytic base (His272). The strain in conformation B was mainly in the C(alpha)-C(beta)-C(gamma) angle (126 degrees ) that deviated by 13.4 degrees from the "ideal" bond angle of 112.6 degrees. On the basis of these observations, we propose a role for the charge state of the catalytic histidine in determining the geometry of the catalytic residues. We hypothesized that double-protonation of the catalytic base (His272) reduces the distance between the side-chain of this residue and that of the Asp108. The results of molecular dynamics simulations were consistent with the structural data showing that protonation of the His272 side-chain nitrogen atoms does indeed reduce the distance between the side-chains of the residues in question, although the simulations failed to demonstrate the same degree of strain in the Asp108 C(alpha)-C(beta)-C(gamma) angle. Instead, the changes in the molecular dynamics structures were distributed over several bond and dihedral angles. Quantum mechanics calculations on LinB with 1-chloro-2,2-dimethylpropane as a substrate were performed to determine which active site conformations and protonation states were most likely to result in catalysis. It was shown that His272 singly protonated at N(delta)(1) and Asp108 in conformation A gave the most exothermic reaction (DeltaH = -22 kcal/mol). With His272 doubly protonated at N(delta)(1) and N(epsilon)(2), the reactions were only slightly exothermic or were endothermic. In all calculations starting with Asp108 in conformation B, the Asp108 C(alpha)-C(beta)-C(gamma) angle changed during the reaction and the Asp108 moved to conformation A. The results presented here indicate that the positions of the catalytic residues and charge state of the catalytic base are important for determining reaction energetics in LinB.     

Crystal structure and conformation of 5-fluorouridine: conformational preferences for 5-fluorinated pyranosides

Crystals of 5-fluorouridine (5FUrd) have unit cell dimensions a = 7.716(1), b = 5.861(2), c = 13.041(1)A, alpha = gamma = 90 degrees, beta = 96.70 degrees (1), space group P2(1), Z = 2, rho obs = 1.56 gm/c.c and rho calc = 1574 gm/c.c The crystal structure was determined with diffractometric data and refined to a final reliability index of 0.042 for the observed 2205 reflections (I > or = 3sigma). The nucleoside has the anti conformation [chi = 53.1(4) degrees] with the furanose ring in the favorite C2'-endo conformation. The conformation across the sugar exocyclic bond is g+, with values of 49.1(4) and -69.3(4) degrees for phi(theta c) and phi (infinity) respectively. The pseudorotational amplitude tau(m) is 34.5 (2) with a phase angle of 171.6(4) degrees. The crystal structure is stabilized by a network of N-H...O and O-H...O involving the N3 of the uracil base and the sugar 03' and 02' as donors and the 02 and 04 of the uracil base and 03' oxygen as acceptors respectively. Fluorine is neither involved in the hydrogen bonding nor in the stacking interactions. Our studies of several 5-fluorinated nucleosides show the following preferred conformational features: 1) the most favored anti conformation for the nucleoside [chi varies from -20 to + 60 degrees] 2) an inverse correlation between the glycosyl bond distance and the chi angle 3) a wide variation of conformations of the sugar ranging froni C2'-endo through C3'-endo to C4'-exo 4) the preferred g+ across the exocyclic C4'-C5' bond and 5) no role for the fluorine atom in the hydrogen bonding or base stacking interactions.     

Role of water molecules in the crystal structure of gly-L-ala-L-phe: A possible sequence preference for nucleation of α-helix?

The synthetic peptide Gly-L-Ala-L-Phe (C14H19N3O4.2H2O; GAF) crystallizes in the monoclinic space group P2I1), with a = 5.879(1), b = 7.966(1), c = 17.754(2) A, beta = 95.14(2) degrees, Dx = 1.321 g cm-3, and Z = 2. The crystal structure was solved by direct methods using the program SHELXS-86 and refined to an R value of 0.031 for 1425 reflections (greater than 3 sigma). The tripeptide exists as a zwitterion in the crystal and assumes a near alpha-helical backbone conformation with the following torsion angles: psi 1 = -147.8 degrees; phi 2, psi 2 = -71.2 degrees, 33.4 degrees; phi 3, psi 3 = -78.3 degrees, -43.3 degrees. In this structure, one water molecule bridges the COO- and NH3+ terminii to complete a turn of an alpha-helix and another water molecule participates in head-to-tail intermolecular hydrogen bonding, so that the end result is a column of molecules that looks like an alpha-helix. Thus, the two water molecules of crystallization play a major role in stabilizing the near alpha-helical conformation of each tripeptide molecule and in elongating the helix throughout the crystal. An analysis of all protein sequences around regions containing a GAF fragment by Chou-Fasman's secondary structure prediction method showed that those regions are likely to assume an alpha-helical conformation with twice the probability they are likely to adopt a beta-sheet conformation. It is conceivable that a GAF fragment may be a good part of the nucleation site for forming alpha-helical fragments in a polypeptide, with the aqueous medium playing a crucial role in maintaining such transient species.     

Crystal-state structural analysis of two gamma-lactam-restricted analogs of Pro-Leu-Gly-NH2

The crystal structures of two analogs of Pro-Leu-Gly-NH2 (1), containing a gamma-lactam conformational constraint in place of the -Leu-Gly- sequences, are described. The highly biologically active (S,R)-diastereomer 2a is semi-extended at the C-terminus, with the N-terminal Pro residue in the unusual "C5" conformation [psi 1 = -0.8(15) degrees] stabilized by a (peptide)N-H...N(amino) intramolecular H-bond [the N(3)...N(4) separation is 2.687(11)A]. Conversely, the N,N'-isopropylidene aminal trihydrate of the (S,S)-diastereomer 2b, compound 3, adopts a beta-bend conformation at the C-terminus, as already reported for 1. However, the backbone torsion angles [phi 2 = 57.4(4), psi 2 = -129.9(3) degrees; psi 3 = -92.3(4), phi 3 = 6.4(5) degrees] lie close to the values expected for the corner residues of an ideal type-II' beta-bend. A weak intramolecular 4----1 H-bond is seen between the Gly carboxyamide anti-NH and Pro C = O groups. In the newly formed 2,2,3,4-tetraalkyl-5-oxo-imidazolidin-1-yl moiety the psi 1 torsion angle is 12.9(4) degrees and the intramolecular N(3)...N(4) separation is 2.321(4)A.     

Amide hydrogen exchange rates of peptides in H2O solution by 1H nuclear magnetic resonance transfer of solvent saturation method. Conformations of oxytocin and lysine vasopressin in aqueous solution.

The NH exchange rates in aqueous media of oxytocin and 8-lysine vasopressin (LVP) have been measured by using transfer of solvent saturation method. The data are consistent with a "highly motile" dynamic equilibrium between folded and highly solvated conformations. The highly-motility limit applies to the exchange of NH hydrogens of oxytocin and LVP. Folded structures are more prevalent in oxytocin than in LVP. Partial shielding is indicated for peptide hydrogens of Asn5 and perhaps also Cys6 of oxytocin and for Cys6 of LVP. It is tentatively proposed that the folded conformation of oxytocin in aqueous media may contain a parallel beta-structure in the tocinamide ring consisting of two hydrogen bonds: one between the Tyr2 C = O and Asn5 peptide NH as originally proposed for the preferred conformation of oxytocin in dimethyl sulfoxide (D. W. Urry and R. Walter), and the second between he Cys1 C = O and the Cys6 NH. In LVP the hydrogen bond between the Tyr2 C = O and Asn5 peptide NH appears to be absent. The acylic tripeptide sequences (-Pro-X-Gly-NH2) of both hormones appear to be predominantly solvated. The second-order rate constants for acid catalyzed exchange of the primary amide hydrogens of Gln4, Asn5, and Gly9 of oxytocin are consistently greater for the trans NH than for the corresponding cis NH. This observation can be rationalized in terms of mechanisms involving protonation of either the amide oxygen, or the amide nitrogen, but with limited rotation about the C - N bond.     

Helix-forming tendencies of amino acids depend on the restrictions of side-chain rotamer conformations: crystal structure of the tripeptide GAI in two crystalline forms.

In our attempts to design crystalline alpha-helical peptides, we synthesized and crystallized GAI (C11H21N3O4) in two crystal forms, GAI1 and GAI2. Form 1 (GAI1) Gly-L-Ala-L-Ile (C11H21N3O4.3H2O) crystals are monoclinic, space group P2(1) with a = 8.171(2), b = 6.072(4), c = 16.443(4) A, beta = 101.24(2) degrees, V = 800 A3, Dc = 1.300 g cm-3 and Z = 2, R = 0.081 for 482 reflections. Form 2 (GAI2) Gly-L-Ala-L-Ile (C11H21N3O4.1/2H2O) is triclinic, space group P1 with a = 5.830(1), b = 8.832(2), c = 15.008(2) A, alpha = 102.88(1), beta = 101.16(2), gamma = 70.72(2) degrees, V = 705 A3, Z = 2, Dc = 1.264 g cm-3, R = 0.04 for 2582 reflections. GAI1 is isomorphous with GAV and forms a helix, whereas GAI2 does not. In GAI1, the tripeptide molecule is held in a near helical conformation by a water molecule that bridges the NH3+ and COO- groups, and acts as the fourth residue needed to complete the turn by forming two hydrogen bonds. Two other water molecules form intermolecular hydrogen bonds in stabilizing the helical structure so that the end result is a column of molecules that looks like an incipient alpha-helix. GAI2 imitates a cyclic peptide and traps a water molecule. The conformation angles chi 11 and chi 12 for the side chain are (-63.7 degrees, 171.1 degrees) for the helical GAI1, and (-65.1 degrees, 58.6 degrees) and (-65.0 degrees, 58.9 degrees) for the two independent nonhelical molecules in GAI2; in GAI1, both the C gamma atoms point away from the helix, whereas in GAI2 the C gamma atom with the g+ conformation points inward to the helix and causes sterical interaction with atoms in the adjacent peptide plane. From these results, it is clear that the helix-forming tendencies of amino acids correlate with the restrictions of side-chain rotamer conformations. Both the peptide units in GAI1 are trans and show significant deviation from planarity [omega 1 = -168(1) degrees; omega 2 = -171(1) degrees] whereas both the peptide units in both the molecules A and B in GAI2 do not show significant deviation from planarity [omega 1 = 179.3(3) degrees; omega 2 = -179.3(3) degrees for molecule A and omega 1 = 179.5(3) degrees; omega 2 = -179.4(3) degrees for molecule B], indicating that the peptide planes in these incipient alpha-helical peptides are considerably bent.     

Solid state and solution conformations of a hybrid alphagammaalphaalphagammaalpha hexapeptide. Characterization of a backbone expanded analog of the alpha-polypeptide 3(10)-helix

The stereochemically constrained gamma amino acid residue gabapentin (1-(aminomethyl)cyclohexaneacetic acid, Gpn) has been incorporated into a host alpha-peptide sequence. The structure of a hybrid alphagammaalphaalphagammaalpha peptide, Boc-Leu-Gpn-Aib-Leu-Gpn-Aib-OMe in crystals reveals a continuous helical conformation stabilized by three intramolecular 4 --> 1 C(12) hydrogen bonds across the alphagamma/alphagamma segments and one C(10) hydrogen bond across the central alphaalpha segment. This conformation corresponds to an expanded analog of the canonical all-alpha polypeptide 3(10)-helix, with insertion of two additional backbone atoms at each gamma residue. Solvent dependence of NH chemical shifts in CDCl(3) solution are consistent with conformation in which the NH groups of Aib (3), Leu (4), Gpn (5), and Aib (6) are hydrogen bonded, a feature observed in the solid state. The nonsequential NOEs between Gpn (2) NH <--> Leu (4) NH and Gpn (2) NH <--> Gpn (5) NH support the presence of additional conformations in solution. Temperature-dependent line broadening of NH resonances confirms the occurrence of rapid exchange between multiple conformations at room temperature. Two conformational models which rationalize the observed nonsequential NOEs are presented, both of which contain three hydrogen bonds and are consistent with the known stereochemical preferences of the Gpn residue.     

Crystal structure and solution conformation of S,S'-bis(Boc-Cys-Ala-OMe): intramolecular antiparallel beta-sheet conformation of an acyclic cystine peptide

The conformation of the acyclic biscystine peptide S,S'-bis(Boc-Cys-Ala-OMe) has been studied in the solid state by x-ray diffraction, and in solution by 1H- and 13C-nmr, ir, and CD methods. The peptide molecule has a twofold rotation symmetry and adopts an intramolecular antiparallel beta-sheet structure in the solid state. The two antiparallel extended strands are stabilized by two hydrogen bonds between the Boc CO and Ala NH groups [N...O 2.964 (3) A, O...HN 2.11 (3) A, and NH...O angle 162 (3) degrees]. The disulfide bridge has a right-handed conformation with the torsion angle C beta SSC beta = 95.8 (2) degrees. In solution the presence of a twofold rotation symmetry in the molecule is evident from the 1H- and 13C-nmr spectra. 1H-nmr studies, using solvent and temperature dependencies of NH chemical shifts, paramagnetic radical induced line broadening, and rate of deuterium-hydrogen exchange effects on NH resonances, suggest that Ala NH is solvent shielded and intramolecularly hydrogen bonded in CDCl3 and in (CD3)2SO. Nuclear Overhauser effects observed between Cys C alpha H and Ala NH protons and ir studies provide evidence of the occurrence of antiparallel beta-sheet structure in these solvents. The CD spectra of the peptide in organic solvents are characteristic of those observed for cystine peptides that have been shown to adopt antiparallel beta-sheet structures.     

Pex, analytical tools for PDB files. II. H-Pex: noncanonical H-bonds in alpha-helices

We use the H-Pex (Thomas et al., this issue) to analyze the main chain interactions in 131 proteins. In antiparallel beta-sheets, the geometry of the N...O bond is: median N...O distances, 2.9 SA, C==O...N angles at 154 degrees and the C alpha--C==O...H angles are dispersed around 3 degrees. In some instances, the other side of the C==O axis is occupied by a HC alpha. As recently supported by Vargas et al. (J Am Chem Soc 2000;122:4750-4755) C alpha H...O and NH...O could cooperate to sheet stability. In alpha-helices, the main chain C==O interact with the NH of their n + 4 neighbor on one side, and with a C beta H or C gamma H on the other side. The median O...N distance (3.0 A) and C==N angle (147 degrees) suggest a canonical H-bond, but the C alpha--C==O...H dihedral angle invalidates this option, since the hydrogen attacks the oxygen at 122 degrees, i.e., between the sp(2) and pi orbitals. This supports that the H-bond is noncanonical. In many instances, the C gamma H or the C beta H of the n + 4 residue stands opposite to the NH with respect to the oxygen. Therefore, we propose that, in alpha-helices, the C gamma H or C beta H and the NH of the n + 4 residue hold the oxygen like an electrostatic pincher. Proteins 2001;43:37-44.     

Photo-oxygenation sensitized by dyes

This paper discusses the mechanism of photooxygenation reactions sensitized by dyes, such as: rose bengal, methylene blue, tetraphenylporphin and chlorophyll a. First it is shown more particularly that: the quantum yields of singlet oxygen O2(1 delta g) production gamma delta, and of intersystem crossing singlet S1-triplet T1, gamma is, are not always equal and that the possibilities gamma delta greater than or less than gamma is may occur or are observed; the processes S1 + O2(3 sigma)----T1 + O2(3 sigma) and T1 + O2(3 sigma)----S0 + O2(1 delta g) are mainly if not fully responsible for the quenching of the singlet and triplet excited states of the sensitizer by oxygen. Thereafter, clear indication is given of the considerable complication of the photooxygenation which may arise from particular properties of the investigated substrate A (or of other compounds present in the reaction medium) and which may result in a decrease of the oxygenation quantum yield phi O2. It is shown that this lowering of phi O2 is due to that of gamma delta and/or of phi A, (the probability that O2(1 delta g) yields an oxygenation product AO2) since phi O2 = gamma delta phi A. The latter effect can be induced by the quenching of singlet oxygen by the dye, a process which is quite general and which must be always taken into account in kinetic studies.     

Structure and conformation of peptides involving prolyl residue. IV. L-Prolyl-L-leucine monohydrate

The dipeptide, L-prolyl-L-leucine monohydrate (C11H20N2O3.H2O, molecular weight, 246.3) crystallizes in the monoclinic space group P2(1), with cell constants: a = 6.492(2)A, b = 5.417(8)A, c = 20.491(5)A, beta = 96.59(2) degrees, Z = 2, Do = 1.15 g/cm3, and Dc = 1.142 g/cm3. The structure was solved by SHELX-86 and refined by full matrix least squares methods to a final R-factor of 0.081 for 660 unique reflections (I greater than 2 sigma (I)) measured on an Enraf Nonius CAD-4 diffractometer (CuK alpha, lambda = 1.5418 A, T = 293 K). The peptide linkage exists in the trans conformation. The pyrrolidine ring exists in the envelope conformation. The values of the sidechain torsion angles are: chi 1 = -59.3(13) degrees, chi 21 = -63.1(16) degrees and chi 22 = 174.8(15) degrees for leucine (C-terminal). The crystal structure is stabilised by a three-dimensional network of N-H ... O, O-H ... O, and C-H ... O hydrogen bonds.     

Variability in the backbone conformation of cyclic pentapeptides. Crystal structure of cyclic(Gly-L-Pro-D-Phe-Gly-L-Ala)

All the peptide bonds in cyclic(Gly-L-Pro-D-Phe-Gly-L-Ala) are in the trans conformation; however, the peptide bond C'5-N1 is twisted by 19 degrees from planarity (omega 5 = -161 degrees). A Type II beta-turn encompasses the L-Pro-D-Phe residues. Carbonyl oxygens O2, O4 and O5 are directed to the same side of the average plane through the backbone ring and they form hydrogen bonds with N3, N5 and N1, respectively, in adjacent molecules in a stacked column where the adjacent molecules are related by one translational unit. The conformation of the backbone is different from that established in other molecules with the DLDDL chirality sequence. The P21 cell contains two molecules of C21H26N5O5 with a = 4.836(2) A, b = 18.346(8) A, c = 12.464(5) A and beta = 100.05(4) degrees. The R factor for 1382 data with [F0[ greater than 1 sigma is 7.0%.     

A comparative conformational study of thymidylyl(3'----5')-thymidine, thymidylyl(3'----5')-5'-thio-5'- deoxythymidine and thymidinylacetamido-[3'(O)----5'(C)]-5'-deoxythymidine

A comparative 270 MHz NMR spectroscopic study on the solution structure of the dimer d(TpT) 1, and its two analogues, namely, d(TpST) 2, and NH2d(TcmT) 4 has been reported. Analysis of chemical shifts and coupling constants indicate that: (i) The sugar moieties of the constituent nucleotides are not affected by modification of the internucleotide linkages and adopt preferentially an S-type conformation. (ii) The C4'-C5' bond in the pT part of the modified dimers 2 and 4 shows a large conformational freedom (gamma+ = 32% and 35%, respectively) compared to 1 (gamma+ = 75%). (iii) The population of the trans conformer about C5'-O5' is less important in d(TpST) 2 compared to d(TpT) 1. (iv) The C3'-O3' bond in 2 adopts a trans conformation as in 1. (v) The glycosidic bonds in the modified dimers 2 and 4 showed preferential syn conformation. UV and CD data show that the modified dimers 2 and 4 have poor tendency to stack intramolecularly, they also base pair less efficiently with d(ApA) as compared to d(TpT) 1.     

Distensibility characteristics of caval veins and empirical exponential formulae

The stress-strain curves of the vena cava have been measured of vena cava superior, and the intrathoracic and abdominal portions of vena cava inferior excised from dogs. The stress sigma is expressed by the exponential function of the strain gamma as follows: sigma = sigma 0[exp (gamma/gamma 0) - 1] in the longitudinal direction, and sigma = sigma 1[exp(gamma/gamma 1) - 1] + sigma 2 [exp(gamma/gamma 2) - 1] in the circumferential one for all the three kinds of veins. The constants sigma 0, gamma 0, sigma 1, gamma 1, sigma 2 and gamma 2 are determined by a nonlinear least squares method.