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  • 1
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 31 (1975), S. 203-211 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 27 (1971), S. 1337-1344 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 21 (1966), S. 177-180 
    ISSN: 0001-5520
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences
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  • 4
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 20 (1966), S. 214-219 
    ISSN: 0001-5520
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 17 (1964), S. 396-403 
    ISSN: 0001-5520
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 17 (1964), S. 282-289 
    ISSN: 0001-5520
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 51 (1995), S. 318-330 
    ISSN: 1399-0047
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The oxidized recombinant flavodoxin from the cyanobacterium Anabaena 7120 has been crystallized in a trigonal form. The recombinant protein has an identical primary structure to that purified directly from Anabaena, which functions as a substitute for ferredoxin in an iron-deficient environment for electron transfer from photosystem I to ferredoxin–NADP+ reductase. X-ray data to 1.40 Å were collected on a Siemens area detector. Of the 311 379 reflections collected, 36069 reflections were unique in space group P3121 (a = 55.36, c = 102.59 Å) with an Rmerge of 3.8%. The structure was solved by molecular replacement using coordinates from the wild-type monoclinic structure previously solved in this laboratory [Rao, Shaffie, Yu, Satyshur, Stockman & Markley (1992). Protein Sci. 1, 1413–1427]. The structure was refined with X-PLOR and SHELXL93 to a crystallographic R-factor of 13.9% for 32963 reflections with I〉 2σ(I). The final structure contains 2767 atoms including 31 flavin mononucleotide (FMN) atoms, 299 water molecules, and one sulfate ion. The protein is comprised of a central five-stranded β-sheet surrounded by five helices and binds a single molecule of FMN at the C-terminus of the sheet. The trigonal protein structure and the crystal packing are compared with the monoclinic wild-type protein. Helix α3 in this structure is less distorted than in the monoclinic structure and shows additional hydrogen bonds in the N-terminal portion of the helix. The trigonal structure is extensively hydrogen bonded in three major areas with neighboring molecules compared with five regions in the monoclinic structure, but using significantly fewer hydrogen bonds to stabilize the lattice. There are several hydrogen bonds to the amide groups from water molecules several of which stabilize and extend the ends of the β-sheet.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 38 (1982), S. 827-835 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Abstract A direct method for structural interpretation of small-angle scattering data by monodisperse isotropic systems is presented. The spherical harmonics technique proposed by Stuhrmann [Acta Cryst. (1970), A26, 297-306] is used to choose the class of possible solutions. The method enables one to decompose scattering intensity into partial amplitudes corresponding to different multipole components of scattering density using the space and value density restrictions. If a particle possesses a rotational symmetry, its structure may be restored directly using the method; if not, additional information is required to get a set of possible solutions. The method is stable with respect to experimental errors. The efficiency of the procedure is shown in model examples. The application of the method to interpret the small-angle X-ray scattering curve of bacteriophage T7 produced a map of electron density with a resolution of about 12 Å.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 40 (1984), S. 137-142 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: An iterative procedure for the determination of the signs of scattering amplitudes is considered. It is assumed that the scattering density is a one-dimensional antisymmetric function with a limited range of definition. The convergence of the method to a rigorous solution is proved. The stability of the procedure with respect to various experimental errors is shown in model examples. The proof can be generalized for a one-dimensional phase determination of a continuous intensity distribution.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : International Union of Crystallography (IUCr)
    Acta crystallographica 41 (1985), S. 244-251 
    ISSN: 1600-5724
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The established procedure for analyzing molecular vibrations in terms of normal modes has been adapted so that experimental anisotropic thermal parameters can be used to study low-frequency internal vibrations of simple molecules in crystals. This involves quasinormal modes, which are linear combinations of selected low-frequency internal modes such as the torsional librations about individual bonds. Higher-frequency modes are neglected, since their contribution to the atomic mean-square displacements should be small. The force constants for selected low- frequency internal modes, together with the tensor components (T,L,S) that describe the overall molecular vibration, become the variables in an iterative least-squares refinement in which the observations are the atomic Uij values. As a result, the concerted motion of the atoms for each quasinormal mode is defined and also its vibrational frequency. Corrections to bond lengths and angles due to internal vibrations can be calculated. In tests involving two different lipid crystal structures, the internal motions were introduced as torsions about two or three bonds occurring near the junction of an extended hydrocarbon chain with a relatively rigid massive atomic grouping. Compared with the simple rigid-body model, there were highly significant improvements in agreement between experimental and calculated Uij values. Force constants for torsion about three C-S bonds were also in agreement [26 (5), 23 (6) and 22 (6) J mol-1 deg-2]. In one of the crystal structures (determined at 123 K), the six C-C bonds of a paraffin chain have average lengths 1.526 (2) Å before correction, 1.527 (3) Å after correction for simple rigid-body libration and 1.536 (4) Å after corrections including the quasinormal vibrations. The latter agrees with the electron diffraction value 1.542 (4) Å for n-hexadecane.
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