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  • Articles: DFG German National Licenses  (73)
  • 1995-1999  (71)
  • 1980-1984  (2)
  • 11
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 69 (1996), S. 3587-3589 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The transverse Peltier effect is investigated on the top-seeded melt texture superconductor YBa2Cu3O7−δ (YBCO). By restricting the heat absorbing or evolving on one of the sample's surfaces, the Peltier heat flow is converted into a temperature difference for measurement. The temperature difference is found proportional to the current applied, which is in accordance with the prediction of transverse Peltier effect. Based on a simplified model, the difference of the Seebeck coefficients between the ab plane and the c axis, |Sab−Sc|, is about 35 μV/K. It is in good agreement with that of large single crystal [I. Terasaki, Y. Sato, S. Tajima, S. Miyamoto, and S. Tanaka, Physica C 235-240, 1413 (1994)]. The transverse Peltier effect is verified. This supports the idea that the off-diagonal thermoelectric effect is responsible for the anomalously high laser-induced transient transverse voltage on the oriented YBCO superconducting thin films. © 1996 American Institute of Physics.
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  • 12
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 8 (1996), S. 704-714 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: At high Reynolds numbers, the process leading to dynamic stall on airfoils initiates in the leading-edge region. For thin airfoils, the local motion near rounded leading edges can be represented as flow past a parabola and when the mainstream flow is at an angle of attack to the airfoil, a portion of the boundary layer will be exposed to an adverse pressure gradient. Once the angle of attack exceeds a certain critical value, it is demonstrated that unsteady boundary-layer separation will occur in the leading-edge region in the form of an abrupt focused boundary-layer eruption. This process is believed to initiate the formation of the dynamic stall vortex. For impulsively-started incompressible flow past a parabola, a generic behavior is found to occur over a range of angles of attack, and a limit solution corresponding to relatively large angles is found. The separation in the leading-edge region develops in a zone of relatively limited streamwise extent over a wide range of angles of attack. This suggests that localized control measures (such as suction) may possibly be effective at inhibiting separation. © 1996 American Institute of Physics.
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  • 13
    Electronic Resource
    Electronic Resource
    Oxford [u.a.] : International Union of Crystallography (IUCr)
    Acta crystallographica 52 (1996), S. 2830-2832 
    ISSN: 1600-5759
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Type of Medium: Electronic Resource
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  • 14
    Electronic Resource
    Electronic Resource
    Oxford [u.a.] : International Union of Crystallography (IUCr)
    Acta crystallographica 55 (1999), S. 0-0 
    ISSN: 1600-5759
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Type of Medium: Electronic Resource
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  • 15
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 52 (1996), S. 989-998 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: The new inclusion complexes tetraethylammonium nitrate–thiourea (1:3), (C2H5)4N+.NO3−. 3(NH2)2CS (1), tetra-n-propylammonium nitrate–thiourea–water (1:3:1), (n-C3H7)4N+.NO3−.3(NH2)2CS.H2O (2), tetramethylammonium nitrate–thiourea (1:1), (CH3)4N+.NO3−.(NH2)2CS (3), tetra-n-propylammonium nitrate–thiourea (1:1), (n-C3H7)4N+.NO3−. (NH2)2CS (4), and tetra-n-butylammonium nitrate–thiourea (1:1), (n-C4H9)4N+.NO3−.(NH2)2CS (5) have been prepared and characterized by X-ray crystallography. Crystal data, Mo Kα: (1), space group P{\bar 1}, a = 10.300 (2), b = 14.704 (3), c = 15.784 (4) Å, α = 75.30 (3), β = 86.98 (3), γ = 72.25 (3)°, Z = 4 and RF = 0.039 for 5034 observed data; (2), space group P21/n, a = 8.433 (2), b = 9.369 (2), c = 34.361 (7) Å, β = 91.01 (3)°, Z = 4 and RF = 0.050 for 2475 observed data; (3), space group Pnma, a = 15.720 (3), b = 8.218 (2), c = 8.709 (2) Å, Z = 4 and RF = 0.073 for 579 observed data; (4), space group P21/n, a = 8.784 (2), b = 14.421 (3), c = 15.078 (3) Å, β = 92.31 (3)°, Z = 4 and RF = 0.046 for 2507 observed data; (5), space group Pna21, a = 19.934 (3), b = 12.680 (2), c = 9.092 (3) Å, Z = 4 and RF = 0.047 for 1646 observed data. In the crystal structure of (1) infinite chains each composed of an alternate arrangement of a twisted thiourea trimer and a nitrate ion are cross-linked to form a puckered layer and further hydrogen bonding between such layers leads to a channel host framework for accommodation of the cationic guests. In the crystal structure of (2) two independent thiourea molecules are used to construct a hydrogen-bonded puckered layer normal to the c axis, whereas the remaining thiourea molecule, together with the nitrate ion and water molecule, generate another puckered layer that is parallel to the first. Hydrogen bonding between these two types of layers gives rise to a channel system running parallel to the [100] direction and the cations are stacked regularly within each column. Compounds (3), (4) and (5) have closely related crystal structures in which the cations are separated by one-dimensional, infinitely extended thiourea–nitrate composite ribbons in a sandwich-like packing arrangement.
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  • 16
    Electronic Resource
    Electronic Resource
    [s.l.] : Macmillan Magazines Ltd.
    Nature 392 (1998), S. 906-909 
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] Many large-scale applications of high-temperature superconductors depend crucially on the ability to achieve high critical-current densities Jc (of the order of 105 A cm−2). Existing silver-sheathed ...
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  • 17
    Electronic Resource
    Electronic Resource
    Chester : International Union of Crystallography (IUCr)
    Journal of synchrotron radiation 6 (1999), S. 749-751 
    ISSN: 1600-5775
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
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  • 18
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 53 (1997), S. 252-261 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: New inclusion complexes tetra-n-butylammonium hydrogen oxalate–thiourea (1/2), (n-C4H9)4N+.HC2O4−.2[(NH2)2CS] (1), tetramethylammonium hydrogen fumarate–thiourea (1/1), (CH3)4N+.HC4H2O4−.(NH2)2CS (2), di(tetraethylammonium) fumarate–thiourea (1/2), [(C2H5)4N+]2.C4H2O42−.2[(NH2)2CS] (3) and tetra-n-propylammonium hydrogen fumarate–thiourea–water (1/1/2), (n-C3H7)4N+.HC4H2 O4−.(NH2)2CS.2H2O (4) have been prepared and characterized by X-ray crystallography. Crystal data, Mo Kα radiation: (1), space group P21/n, a = 8.854 (6), b = 9.992 (3), c = 32.04 (2) Å, β = 97.34 (3), Z = 4, RF = 0.055 for 2261 observed data; (2), space group P\overline 1, a = 6.269 (2), b = 8.118 (4), c = 14.562 (8) Å, α = 104.79 (4), β= 91.72 (4), γ = 101.30 (4)°, Z = 2, RF = 0.078 for 1543 observed data; (3), space group P21/n, a = 11.340 (2), b = 9.293 (6), c = 14.619 (2) Å, β = 102.41 (2)°, Z = 2, RF = 0.050 for 1856 observed data; (4), space group P2/n, a = 16.866 (4), b = 8.311 (1), c = 17.603 (2) Å, β = 104.94 (1)°, Z = 4, RF = 0.048 for 2785 observed data. In the crystal structure of (1) the tetra-n-butylammonium ions are sandwiched between puckered layers, which are constructed from thiourea-hydrogen oxalate ribbons. In the crystal structure of (2), zigzag O--H...O and C--H...O hydrogen-bonded hydrogen fumarate ribbons are linked by thiourea dimers to form a wide puckered ribbon and the crystal structure is built of a packing of these thiourea–anion composite ribbons and the cationic columns. In the layer-type crystal structure of (3) a series of thiourea–fumarate layers match the (002) planes and the (C2H5)4N+ cations occupy the intervening space. In the crystal structure of (4) the thiourea, hydrogen fumarate ions and water molecules are connected by hydrogen bonds to form wide puckered ribbons, which are crosslinked to generate a three-dimensional host framework containing open channels aligned parallel to the a axis, with the tetra-n-propylammonium cations accommodated in a single column within each channel.
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  • 19
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 54 (1998), S. 180-192 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: New inclusion complexes tetra-n-propylammonium fluoride–urea–water (2/7/3), 2(n-C3H7)4N+F−.7(NH2)2CO.3H2O (1), tetra-n-propylammonium chloride–urea (1/2), (n-C3H7)4N+Cl−.2(NH2)2CO (2), tetra-n-propylammonium chloride–urea (1/3), (n-C3H7)4N+Cl−.3(NH2)2CO (3), tetra-n-propylammonium bromide–urea–water (1/3/1), (n-C3H7)4N+Br−.3(NH2)2CO.H2O (4), and tetra-n-propylammonium iodide–urea–water (1/3/1), (n-C3H7)4N+I−.3(NH2)2CO.H2O (5), have been prepared and characterized by X-ray crystallography. Crystal data, Mo Kα radiation: (1), space group P21/c, Z = 4, a = 8.560 (2), b = 16.301 (3), c = 37.004 (7) Å, β = 92.31 (3)°, RF = 0.075 for 3945 observed data; (2), space group P21/n, Z = 4, a = 9.839 (2), b = 15.160 (3), c = 14.583 (3) Å, β = 108.82 (3)°, RF = 0.058 for 1770 observed data; (3), space group P21/c, Z = 4, a = 9.866 (2), b = 16.274 (3), c = 15.277 (3) Å, β = 103.36 (3)°, RF = 0.060 for 2272 observed data; (4), space group P1¯, Z = 2, a = 8.857 (2), b = 10.639 (2), c = 15.115 (3) Å, α = 88.01 (3), β = 75.02 (3), γ = 66.72 (3)°, RF = 0.064 for 2694 observed data; (5), space group P1¯, Z = 2, a = 9.045 (2), b = 10.781 (2), c = 15.169 (3) Å, α = 87.98 (3), β = 76.00 (3), γ = 65.73 (3)°, RF = 0.052 for 4973 observed data. In the crystal structure of (1) an alternate crisscross arrangement of urea ribbons, which are cross-bridged by other urea molecules, water molecules and fluoride ions, generates a three-dimensional host lattice containing an open-channel system running parallel to the b axis, with the (n-C3H7)4N+ cations accommodated in a zigzag column within each channel. In the crystal structure of (2) the cations are sandwiched between puckered layers resulting from parallel urea ribbons that are cross-bridged by chloride anions. In (3) the (n-C3H7)4N+ cations are accommodated in a channel-type host lattice built of planar arrays of twisted ribbons constructed from three independent urea molecules, which are cross-linked by bridging chloride ions. Complexes (4) and (5) are isomorphous with the same channel host framework built of parallel corrugated urea layers that are interlinked by cyclic (H2O.X−)2 tetramers.
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  • 20
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Acta crystallographica 53 (1997), S. 262-271 
    ISSN: 1600-5740
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Chemistry and Pharmacology , Geosciences , Physics
    Notes: Air-sensitive selenourea inclusion complexes tetraethylammonium chloride–selenourea (1/2), (C2H5)4N+.C1−.2[(NH2)2CSe] (1), tetra-n-propyl-ammonium chloride–selenourea (1/3), (n-C3H7)4N+.C1−.3[(NH2)2CSe] (2), tetra-n-propylammonium bromide–selenourea (1/3), (n-C〈inf/〉3H7)4N+.Br−.3[(NH2)2CSe] (3), and tetra-n-propylammonium iodide–selenourea (1/1), (n-C3H7)4N+.I−.(NH2)2CSe (4), have been prepared and characterized by X-ray crystallography. Crystal data, Mo Kα radiation: (1), space group P21/n, Z = 4, a = 8.768 (5), b = 11.036 (6), c = 19.79 (1) Å, β = 96.92 (1)°, RF = 0.055 for 1468 observed data; (2), space group Cc, Z = 4, a = 18.091 (4), b = 13.719 (3), c = 11.539 (2) Å, β = 111.93 (3)°, RF = 0.051 for 1187 observed data; (3), space group Cc, Z = 4, a = 18.309 (4), b = 13.807 (3), c = 11.577 (2) Å, β = 112.45 (3)°, RF = 0.049 for 1592 observed data; (4), space group P21/n, Z = 4, a = 8.976 (1), b = 14.455 (2), c = 15.377 (3) Å, β = 94.16(1)°, RF = 0.062 for 1984 observed data. In the crystal structure of (1) the parallel alternate arrangement of selenourea–chloride ribbons and selenourea chains generates a puckered layer and the cations are sandwiched between them. In the isomorphous complexes (2) and (3) wide selenourea–halide double ribbons are crosslinked by bridging selenourea molecules via N—H...Se and N—H...X hydrogen bonds [average N...Se = 3.521 (8) and 3.527 (7), N...Cl = 3.354 (8) and N...Br = 3.500 (7) Å in (2) and (3), respectively] to form a channel-like three-dimensional network and the cations are accommodated in a single column within each channel. In the crystal structure of (4) the selenourea molecules are joined in the shoulder-to-shoulder fashion via N—H...Se hydrogen bonds [N...Se = 3.529 (7) and 3.534 (7) Å] to generate a ribbon and each selenourea molecule also forms a pair of chelating N—H...I hydrogen bonds [N...I = 3.567 (7) and 3.652 (7) Å] to an adjacent iodide ion.
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