Crystal and molecular structure of sym-homospermidine monohydrate.

Sym-homospermidine, [formula; see text] is a naturally occurring rare-polyamine found in relatively large concentration in sandal leaves. As part of our studies on structure and interactions of polyamines, sym-homospermidine was purified from sandal leaves and its structure was determined by single crystal X-ray diffraction technique. The phosphate salt of the molecule crystallized in the triclinic space group P1- with a = 8.246(1)A, b = 8.775(1)A, c = 15.531(2)A, alpha = 74.20(1) degrees, beta = 88.36(1) degrees and gamma = 65.41(1) degrees. The structure was determined by direct methods and refined to a final R factor of 5.4% for 2087 reflections with magnitude of F(obs) greater than 5 sigma [F(obs)]. The amine exists in its most favourable all trans conformation. For each amine molecule three phosphate groups exist in the crystal structure, suggesting that two of the oxygens of each phosphate group are protonated. There is also a single water molecule in the asymmetric unit in contrast to that of spermidine phosphate which has 3 water molecules. These differences probably reflect the hydrogen bonding properties of mono-ionic and di-ionic phosphate groups. The structure is predominantly stabilized by a network of hydrogen bonds.     

Determination of molecular weight and molecular structure of rat-liver pyruvate carboxylase.

The molecular weight of pyruvate carboxylase isolated from pigeon and rat liver mitochondria was examined using analytical ultracentrifugation and electron microscopy. The enzyme molecule appeared as a tetramer with the four subunits arranged at the corners of a square. Sedimentation studies in the analytical ultracentrifuge, extrapolated to infinite dilution, showed the tetramer to have a molecular weight Mc=0r of 280 000 and an So20,w of 12.7 S. The tetramer could be dissociated into trimers and dimers of lower specific enzymic activity by storage at 4 degrees C or incubation at -- 20 degrees C at low protein concentrations. The isolated trimers and dimers had a molecular weight Mc=0r of 210 000 and 140 000, respectively, and an So20,w of 10.85 S and 7.55 S, respectively. Incubation with 2 M urea at 20 degrees C yielded enzymically inactive subunits (Mc=0r = 70 000; So20,w = 4.95 S). The molecular weights (for pyruvate carboxylase and its subunits), as calculated from the subunit diameter observed in the electron microscope, were consistent with the values obtained from sedimentation studies.     

Crystal and molecular structure of L-valyl-L-lysine hydrochloride.

L-Valyl-L-lysine hydrochloride, C11N3O3H23 HCl, crystallizes in the monoclinic space group P2(1) with a = 5.438(5), b = 14.188(5), c = 9.521(5) A, beta = 95.38(2) degrees and Z = 2. The crystal structure, solved by direct methods, refined to R = 0.036, using full matrix least-squares method. The peptide exists in a zwitterionic form, with the N atom of the lysine side-chain protonated. The two gamma-carbons of the valine side-chain have positional disorder, giving rise to two conformations, chi 1(11) = -67.3 and 65.9 degrees, one of which (65.9 degrees) is sterically less favourable and has been found to be less popular amongst residues branching at beta-C. The lysine side-chain has the geometry of g- tgt, not seen in crystal structures of the dipeptides reported so far. Interestingly, chi 2(3) (63.6 degrees) of lysine side-chain has a gauche+ conformation unlike in most of the other structures, where it is trans. The neighbouring peptide molecules are hydrogen bonded in a head-to-tail fashion, a rather uncommon interaction in lysine peptide structures. The structure shows considerable similarity with that of L-Lys-L-Val HCl in conformational angles and H-bond interactions [4].     

The molecular structure of palmitylcarnitine chloride.

The structure of palmitylcarnitine chloride has been studied by single crystal X-ray diffraction techniques. The final structure of this molecule shows that the carnitine moiety has a conformation similar to that of acetylcarnitine and acetylcholine. The molecular packing of this compound is interesting and rarely found in solid structures of amphipathic molecules.     

The crystal and molecular structure of 9-alpha-D-arabinofuranosyladenine.

The glycosyl torsional angles in two crystallographically-independent molecules of alpha-araA are -73 and -64 degrees, both of which are in the "anti" region. The sugar conformations are C(3')-endo and C(2')-exo-C(3')-endo.     

Relationships between molecular structure and excretion of drugs.

Drugs and their metabolites are usually eliminated from the body by excretion in the urine or bile or sometimes both, but other pathways may be used, such as milk, saliva, sweat or the expired air. The excretion can take place by passive or by active processes, and is influenced by the physico-chemical properties of the drug.     

Crystal and molecular structure of 6,2'-anhydro-1-beta-D-arabinofuranosylctyosine.

The crystal and molecular structure of the title compound has been determined by X-ray diffraction method. The compound crystallizes in monoclinic system with the space group P2₁ and Z=2; the unit cell dimensions are a=10.491, b=7.255, c=6.858 A and β=103.55°. The structure was refined to an R-index of 0.051. The glycosyl torsion angle X_CN is 111.4° (syn-anti) and the arabinose ring forms an exo-conformation, in which C(4′) is displaced by 0.61 A out of the plane of remaining four atoms. The orientation of the C(5′)O(5′) bond is the gauche-gauche as similar as that found frequently in many nucleosides.     

Synthesis, crystal structure and molecular conformation of N-Ac-dehydro-Phe-L-Val-OH.

The peptide N-Ac-dehydro-Phe-L-Val-OH (C16H20N2O4) was synthesized by the usual workup procedure. The peptide crystallizes from its solution in acetonitrile at 4 degrees in hexagonal space group P6(5) with a = b = 11.874(2)A, c = 21.856(9) A, V = 2668(1) A3, Z = 6, dm = 1.151(3) g cm-3, dc = 1.136(4) g cm-3, CuK alpha = 1.5418 A, mu = 0.641 mm-1, F(000) = 972, T = 293 K. The structure was solved by direct methods and refined by least-squares procedure to an R value of 0.074 for 1922 observed reflections. In the dehydro-residue, the C1 alpha-C1 beta distance is 1.35(1) A while the bond angle C1 alpha-C1 beta-C1 gamma is 131.2(9) degrees. The backbone torsion angles are: omega 0 = 172(1) degrees, phi 1 = -60(2) degrees, psi 1 = -31(2) degrees, omega 1 = -179(1) degrees, phi 2 = 59(2) degrees. These values suggest that the peptide tends to adopt an alternating right-handed and left-handed helical conformation. The side chain torsion angles are: chi 1(1) = -6(2) degrees, chi 1(2.1) = -1(2) degrees, chi 1(2.2) = -178(2) degrees, chi 2(1.1) = 63(2) degrees and chi 2(1.2) = -173(1) degrees. These values show that the side chain of dehydro-Phe is planar whereas the valyl side chain adopts a sterically most preferred conformation. The molecules, linked by intermolecular hydrogen bonds and van der Waals forces, are arranged in helices along the c-axis. The helices are held side-by-side by van der Waals contacts.     

Aspects of the molecular structure and dynamics of neuropeptide Y.

Human neuropeptide Y (hNPY) and the Q34-->P34 mutant (P34-hNPY) have been characterized by CD spectroscopy. hNPY self-associates in aqueous solution with a dimerization constant in the micromolar range. The self-association correlates with an increase in secondary-structure content which was studied as a function of concentration, temperature and pH. The effects of temperature were measured in water (5-84 degrees C) and in ethanediol/water (2 : 1) (-90 degrees to +90 degrees C). A single-residue mutation, Q34-->P34, affects the pH, thermal and self-association properties of NPY. The CD results are correlated with photochemically induced dynamic nuclear polarization NMR experiments which show that the tyrosines at the interface between two monomer units present limited accessibility to a photoreactive dye. An equilibrium state is described, involving a PP-fold monomer form and a handshake dimer form, that accommodates the physicochemical properties of NPY.     

Crystal and molecular structure of the dehydropeptide Ac-delta Phe-Val-delta Phe-NH-Me.

The dehydropeptide Ac-delta Phe-L-Val-delta Phe-NH-Me, containing two dehydrophenylalanine (delta Phe) residues, crystallizes from methanol/water in space group P212121, with a = 12.622 (1), b = 12.979 (1), and c = 15.733 (1) A. In the solid state, the molecular structure is characterized by the presence of two intramolecular hydrogen bonds which form two consecutive beta-bends. The (phi, psi) torsion angles of the three residues are very similar and close to the standard values of type III beta-bends, so the molecular conformation corresponds to an incipient right-handed 3(10)-helix, only slightly distorted. In the crystal, the molecules are linked by head-to-tail hydrogen bonds, thus forming continuous helical columns packed in antiparallel mode. There are no lateral hydrogen bonds; the only interactions are hydrophobic contacts between the apolar side chains of neighboring helical columns.     

Modeling of the structure of bacteriorhodopsin. A molecular dynamics study.

Secondary structure predictions for membrane proteins are relatively reliable and permit the construction of model structures that may serve as initial conformations for molecular dynamics simulations. This might provide a scheme to predict the three-dimensional structures of membrane proteins. The feasibility of such an approach is tested for bacteriorhodopsin. We were not able to fully predict the kidney-shaped structure of bacteriorhodopsin. However, features compatible with this structure developed in a simulation starting from a circular arrangement of the seven predicted helices. When instead we started from the kidney shape, assigning the seven predicted helices in different ways to those on the structure, we could distinguish between the different assignments on the basis of energy and tilt of the helices. In this way we could select the correct assignment from a few others. For the correct assignment, the helices spontaneously adopted a tilt that agrees remarkably well with the experimental model structure derived by others. The root-mean-square deviation between our best molecular dynamics structure and the experimental model structure is 3.8 A, caused mainly by deviations in the internal degrees of freedom of the helices.     

Biosynthesis of chick type VI collagen. I. Intracellular assembly and molecular structure

A monospecific rabbit antiserum to pepsin-extracted chick gizzard type VI collagen was used to characterize the intact forms of type VI collagen in tissues and cultured cells. Immunoblotting of gizzard extracts revealed polypeptides of Mr ranging from 260,000 to 140,000. Components of about Mr = 260,000, 150,000, and 140,000, each with a different peptide profile, were immunoprecipitated from labeled matrix-free chick embryo cells. Cleavage of the immunoprecipitated polypeptides with pepsin generated pepsin-resistant fragments of about Mr = 70,000, 55,000, and 45,000 that represent the alpha 1(VI), alpha 2(VI), and alpha 3 (VI) fragments. Immunoblotting with affinity-purified antibodies indicated that the Mr = 150,000 is the intact parent polypeptide of the alpha 1(VI) pepsin; the Mr = 140,000 of the alpha 2(VI) pepsin, and the Mr = 260,000 of the alpha 3(VI) pepsin. Association of the three parent chains was studied by pulse-chase experiments and sodium dodecyl sulfate-polyacrylamide gel electrophoresis analysis under nonreduced conditions. A complex of Mr = 500,000 is already present intracellularly at the end of a 7-min pulse and increases considerably with time while the three unassembled chains show a comparable decrease. After 5-15 min of chase larger forms appeared along with small amounts of aggregated material that did not enter the gel. Analysis of the immunoprecipitate by diagonal electrophoresis indicated that the component of Mr = 500,000 and the larger forms dissociated into the Mr = 260,000, 150,000, and 140,000 polypeptides. Sedimentation profile of a labeled cell extract on a 5-20% sucrose gradient under nondenaturing conditions confirmed the presence of three different peptides in the complex.     

The molecular structure of human erythrocyte spectrin. Biophysical and electron microscopic studies.

Molecules of human erythrocyte spectrin have been examined by electron microscopy after low-angle shadowing. Spectrin heterodimers and tetramers were first purified and characterized by polyacrylamide gel electrophoresis and analytical ultracentrifugation under conditions which minimize proteolysis and aggregation. The heterodimers and tetramere were separated for low-angle shadowing by gel filtration in ammonium acetate buffer at physiological ionic strength, in which they showed sedimentation coefficients of 8.9 S and 12.5 S, respectively, similar to those values reported for heterodimers and tetramers in non-volatile buffers. The ammonium acetate buffer promoted the dissociation of spectrin tetramers into heterodimers under conditions in which tetramers in NaCl or KCl buffers are stable. When visualized by low-angle unidirectional and rotary shadowing, spectrin heterodimers appeared as long flexible molecules with a mean shadowed length of 97 nm. Each heterodimer, composed of the two polypeptide chains, band 1 (240,000 M_r) and band 2 (220,000 M_r), often appeared as two separate strands which lay partially separated from one another or coiled round each other in a loose double helix. The association between these polypeptides appears to be weak, except at both ends of the molecule where there are sites of strong binding. Tetramers are formed by the end-to-end association of two spectrin heterodimer molecules without measurable overlap, and have a mean shadowed length of 194 nm. This association to form tetramers probably involves head-to-head binding of the heterodimers, since the higher oligomers to be expected from a head-to-tail binding mode are not observed. The molecular shape of spectrin is quite distinct from that of myosin, to which it has often been likened.     

Predicting physiological concentrations of metabolites from their molecular structure.

Physiological concentrations of metabolites can partly be explained by their molecular structure. We hypothesize that substances containing certain chemical groups show increased or decreased concentration in cells. We consider here, as chemical groups, local atomic configurations, describing an atom, its bonds, and its direct neighbor atoms. To test our hypothesis, we fitted a linear statistical model that relates experimentally determined logarithmic concentrations to feature vectors containing count numbers of the chemical groups. In order to determine chemical groups that have a clear effect on the concentration, we use a regularized (lasso) regression. In a dataset on 41 substances of central metabolism in different organisms, we found that the physical concentrations are increased by the occurrence of amino and hydroxyl groups, while aldehydes, ketones, and phosphates show decreased concentrations. The model explains about 22% of the variance of the logarithmic mean concentrations.     

Computational complexity of a problem in molecular structure prediction.

The computational task of protein structure prediction is believed to require exponential time, but previous arguments as to its intractability have taken into account only the size of a protein's conformational space. Such arguments do not rule out the possible existence of an algorithm, more selective than exhaustive search, that is efficient and exact. (An efficient algorithm is one that is guaranteed, for all possible inputs, to run in time bounded by a function polynomial in the problem size. An intractable problem is one for which no efficient algorithm exists.) Questions regarding the possible intractability of problems are often best answered using the theory of NP-completeness. In this treatment we show the NP-hardness of two typical mathematical statements of empirical potential energy function minimization of macromolecules. Unless all NP-complete problems can be solved efficiently, these results imply that a function minimization algorithm can be efficient for protein structure prediction only if it exploits protein-specific properties that prohibit the simple geometric constructions that we use in our proofs. Analysis of further mathematical statements of molecular structure prediction could constitute a systematic methodology for identifying sources of complexity in protein folding, and for guiding development of predictive algorithms.