Metal—metal bonding in dinuclear complexes of platinum(I). The crystal and molecular structure of carbonyl(chloro)-bis-μ-[bis(diphenylphosphino)methane]diplatinum hexafluorophosphate

The structure of [Pt₂Cl(CO) (μ-Ph₂PCH₂PPh₂)₂] [PF₆] was determined by $\text{X}$-ray methods and refined to $\text{R}$ = 0.082, using diffractometric intensities of 5646 independent reflections. The crystals are monoclinic, space group $\text{P}$2₁/$\text{n}$, $\text{a}$ = 12.919(3), $\text{b}$ = 15.576(6), $\text{c}$ = 25.151(5)Å, β = 94.82(3)°, $\text{Z}$ = 4. They are built of octahedral hexafluorophosphate anions and dinuclear platinum(I) cations. The latter contain PtCl and PtCO fragments linked to one another by a PtPt σ-bond and by two bridging bis(diphenylphosphino)methane ligands. The platinum atoms are in square planar environments and the dihedral angle between the two coordination planes is 40.1°. Selected bond lengths are: PtPt 2.620(1), PtCl 2.384(5), PtC 1.89(3) and PtP 2.291(5) – 2.308(5)Å.     

Stereochemistry of organophosphorus cyclic compounds—II : Stereospecific synthesis of cis- and trans 2-halogeno-2-oxo-4-methyl-1,3,2-dioxaphosphorinans and their chemical transformations

cis- and trans-2-Chloro-2-oxo-4-methyl-1,3,2-dioxaphosphorinans have been obtained by stereospecific reactions of diastereomerically pure 2-methoxy-4-methyl-1,3,2-dioxaphosphorinans or 2-hydrogen-2-oxo-4-methyl-1,3,2-dioxaphosphorinans with chlorine and sulphuryl chloride, respectively. Similarly, the action of the corresponding brominating agents on isomeric phosphites and phosphonates afforded pure cis- and trans-2-bromo-2-oxo-4-methyl-1,3,2-dioxaphosphorinans. It has been shown that halogenolysis proceeds with retention of configuration at the P atom. On the basis of the ¹H- and ³¹P-NMR spectra conformation of the halogenoanhydrides obtained has been discussed briefly.It has been also found that model nucleophilic substitution reactions occur with inversion of configuration at the P atom in the cyclic halogenoanhydrides.     

Kinetics of successive seeding of monodisperse polystyrene latexes. II. Azo initiators with and without inhibitors

Oil soluble azo initiators in combination with water soluble inhibitors were used to extend the particle size limit in studies of the kinetics of successive seeding of monodisperse polystyrene latexes. Monodisperse latexes were prepared up to 2.5 μm in diam using 4.0 mM AMBN and 14.5 mM hydroquinone with a constant 15% emulsifier (Aerosol–MA) surface coverage throughout the seven step sequence. The polymerization kinetics were measured in a piston/cylinder dilatometer designed for microgravity experiments. The Interval III kinetics were dominated by the gel effect although these were affected by the nature of the inhibitor. In general, the overall polymerization rate decreased with increasing particle size (decreasing N_p) up to a size of about 1 μm. Thereafter, the kinetics were independent of these variables, exhibiting Smith-Ewart Case 3 (bulk) kinetics. The initiator efficiencies were found to be of the order of 10%, considerably lower than reported for bulk polymerizations.     

Resonances Introduced by Discretization

This paper examines the effect of spatially discretizing thenon-linear equation chosen to model the integro-differential equations governinginterfacial vortex sheets. Here H is the Hilbert transform and is a spatial average. It is shown numerically and analyticallythat small-amplitude travelling-wave solutions of the discretizedmodel equation are subject to instabilities whose growth rateis proportional to the amplitude and depends in a complicatedway on the number of mesh points per wavelength. The mechanismof the instability is shown to be a resonance not present inthe continuous system and present in the discrete system becausethe frequency of waves with wavelength equal to twice the meshspacing is zero.     

A Conformal Mapping Problem Arising in Elasticity, II

Suppose that B is an infinite right cylinder over a horizontalbase , which is a Jordan domain bounded by a smooth curve .We suppose that a normal pressure p₁(x, y) and a tangentialpressure p₂(x, y) are applied at every point of the boundaryof B, where p₁, p₂ lie in the plane of the cross-section andare independent of the vertical co-ordinate. It was shown by Cassisa (1982) that in this situation, givenan arbitrary normal pressure p₁, the tangential pressure p₂can be so chosen, that a purely plane stress tensor existswith the above hypotheses, provided that a certain 3 ? 3 matrixM, depending only on the curve , is non-singular. In a previous paper (Hayman, 1982) the author showed that thesingular case can occur and further that an arbitrary pointsymmetric curve can be approximated by singular point symmetriccurves. In the present paper it is shown that M can have rank1, 2 or 3. In the case of rank 2 p₁ must satisfy one additionalintegral condition and in the case of rank 1 two such conditions.If these conditions are satisfied p₂ can be chosen to dependon one or two arbitrary parameters respectively. Some geometrical conditions for the various cases are obtained.Thus for curves with line symmetry the rank can be two but notone, whereas curves with point symmetry can yield matrices ofrank 1, 2 or 3.     

Activation analytical determination of129I in bovine thyroid glands

The continued erection of nuclear installations which is expected in the future involves a greater production of long-lived fission products, which result in a concentration increase in the biosphere, the hydrosphere and the atmosphere. In the frame of a broad survey program, a routine method has been developed with the help of the European Communities to investigate the¹²⁹I content of thyroid glands of cows. It is the purpose of this project to determine the present concentration situation of this nuclide, which in the Federal Republic of Germany mainly concerns the North German low plains. Between autumn '76 and summer '77 18 cows have been investigated with respect to¹²⁹I, and thyroid glands have been taken at different times in November '76 and August '77. Without exception, the animals were 13-month old bulls, part of which has pastured, while the other part has been fed. The detection limit of the method is 20fCi of¹²⁹I.     

ESR investigation of Ti3+ compounds supported on inorganic gels

CpTiCl₂-M-surface complexes (M=Al, Si, Mg, Cp=cyclopentadienyl) supported on Al₂O₃, SiO₂, MgO gels are reduced by Et₃Al, C₃H₅MgBr and BuLi to Ti³⁺ surface compounds which exhibit ESR signals. The g and g values and asymmetry of these signals depend on the kind of gel and reducing agent.

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CpTiCl₂-M ( M=Al, Si, Mg Cp=), Al₂O₃, SiO₂ MgO, Et₃Al, C₃H₅MgBr, BuLi (Et=–C₂H₅ Bu=–C₄H₉) Ti⁺³, . g g .

     

Röntgenkleinwinkeluntersuchungen an Lösungen eines Polystyrolpräparates mit enger Molekulargewichtsverteilung

Zusammenfassung Es wurde das Streuverhalten von Polystyrol im thermodynamisch schlechten Lösungsmittel Cyclohexan zwischen Entmischungstemperatur und-Temperatur untersucht. Beim -Punkt und nahe dabei liegt das Verhalten eines statistisch verknäuelten Fadenmoleküls vor. Unterhalb der-Temperatur beginnt eine Aggregation. Knapp oberhalb der Entmischungstemperatur entspricht das Molekulargewicht etwa einer Verhängung zweier Fadenmoleküle. Ein Auftreten von kompakten Polymerknäueln ist bei dieser Temperatur nicht festzustellen. Der Einfluß des Fadenquerschnitts auf die Streukurve ist beträchtlich, da der Querschnitt nicht viel kleiner als die Persistenzlänge ist. Trotzdem läßt sich die Persistenzlänge (a=12,2 Å) aus dem Übergangspunkt zwischen den etwa 1/(2)² und 1/(2) proportionalen Bereichen bestimmen, da der Knick im Übergangsbereich infolge der großen Anzahl von Persistenzlängen pro Molekül sehr ausgeprägt ist.

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X-Ray small-angle investigations on solutions of a polystyrene sample with a narrow molecular weight distribution

Investigations were made of the scattering behaviour of polystyrene in the thermodynamically bad solvent cyclohexane between precipitation-temperature and-temperature. At the-point and close to it the behaviour of a statistically coiled chain molecule is found. Below-temperature an aggregation is beginning. Just above precipitation-temperature the molecular weight corresponds to an entanglement of two chain molecules. Appearance of compact polymer coils could not be noted at this temperature. The influence of the chain crosssection upon the scattering curve is considerable as the crosssection is not much smaller than the persistence length. Nevertheless, the persistence length (a=12.2 Å) may be determined from the transition point between the ranges roughly proportional to 1/(2)² and 1/(2) as the break within the transition range is very distinct on account of the great number of persistence lengths per molecule.

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Mit 3 Abbildungen

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Herrn Prof. Dr.E. Broda zum 60. Geburtstag gewidmet.     

Optical properties of ZnO and ZnO:In nanorods assembled by sol-gel method

Self-assembled zinc oxide (ZnO) and indium-doping zinc oxide (ZnO:In) nanorod thin films were synthesized on quartz substrates without catalyst in aqueous solution by sol-gel method. The samples were characterized by x-ray diffraction (XRD), scanning electron microscope (SEM), Raman-scattering spectroscopy, room-temperature photoluminescence (PL) spectra, and temperature-dependent PL spectra measurements. XRD and Raman spectra illustrated that there were no single In2O3 phase in ZnO lattice after indium doping. The PL spectra of ZnO showed a strong UV emission band located at 394 nm and a very weak visible emission associated with deep-level defects. Indium incorporation induced the shift of optical band gap, quenching of the near-band-edge photoluminescence and enhanced LO mode multiphonon resonant Raman scattering in ZnO crystals at different temperatures. Abnormal temperature dependence of UV emission integrated intensity of ZnO and ZnO:In samples is observed. The local state emission peak of ZnO:In samples at 3.37 eV is observed in low-temperature PL spectra. The near-band-edge emission peak at room temperature was a mixture of excitons and impurity-related transitions for both of two samples.