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Über das Verhalten von silicium- und zinnorganischen Verbindungen bei der Synthese von Heterocyclen
(1977)
The isocyanates of silicon (CH3)2Si(NCO)2 and Si(NCO)4 react with CH3N[Sn(CH3)3]2 and N[Sn(CH3)3]3 to yield the cyclic derivatives 2a-2b as well as the spiro compound 3. The structures of the compounds are discussed on the basis of 1H NMR and IR data. Mass spectra are not conclusive for assigning a certain structure. SO2(NCO)2 and (CH3)3Si-S-Si(CH3)3 form a cyclic compound 4 which contains two sulfur atoms of coordination number two and four. The results of the mass spectra can be interpreted by assuming that a rearrangement occurred. 4 hydrolyses under formation of 5.
CH3P(S)(NCO)2 reacts with [(CH3)3Si]2N-CH3, [(CH3)3SiNCH3]2CO and [(CH3)3Sn]3N to give the cyclic compounds 2a-2c. The structures are discussed on the basis of NMR and IR data. In 2 a and 2 b the (CH3)3Si-groups are easily and quantitatively replaced by protons with water under formation of (CH3)3Si-O-Si(CH3)3. By the reaction of CH3P(S)(NCO)2 with [(CH3)3Si]2S 4 is obtained, a cyclic compound with a sulfur atom of coordination number 2.
FP(S)(NCS)2 was used to investigate the scope of these reactions. With [(CH3)3Si]2NCH3 and FP(S)(NCS)2 5 is obtained, which reacts with S2Cl2 to yield 6, a bridged disulfur compound. This method may be useful for the systematic investigation of new cyclic compounds.
As[N(CH3)2]3 reacts with the following isocyanates: FSO2NCO, n-C4F9SO2NCO, SO2(NCO)2 and (CH3)3SiNCO. The products which result from reaction of FSO2NCO and n-C4F9SO2NCO are the acyclic tri- and bisubstituted arsines [xxx]
In contrast, SO2(NCO)2 and (CH3)3SiNCO form eight- and four-membered ring compounds, where the skeleton consists of the atoms As2S2N4 (3) and As2N2 (4). The new compounds were characterized by NMR and mass spectra.
Die Gewichte des Natur- und Vogelschutzes haben sich in den letzten Jahrzehnten verlagert. Anstelle der Wald-, Gebüsch- und Trockenrasenformationen rücken heute FeuchtIandbiotoe in den Mittelpunkt der Schutzanstrengungen: Die Erkenntnis setzt sich durch, daß deren Bewohner zu den gefährdetsten Elementen unserer Pflanzen- und Tierwelt gehören.
Zwei Rubus-Arten werden erstmals beschrieben: Rubus amisiensis Weber (Ems-Brombeere, zur Ser. Silvatici F. gehörig), der im Emsland, in der Grafschaft Bentheim und in den Niederlanden verbreitet ist. Die zweite Art, Rubus conothyrsoides Weber, wächst vor allem im Hügelland im Raum zwischen Bielefeld und Lingen und ist hier streckenweise eine der häufigsten Arten. Sie gehört zu der hier neu aufgestellten Serie Anisacanthi Weber, die sich durch eine große Variabilität der Bestachelung und des Drüsenbesatzes auf dem Schößling auszeichnet. Die Holotypen der Arten sind abgebildet, die Verbreitung ist in Rasterkarten dargestellt.
Die Autorin untersucht den Einfluß typischer Traumen auf die Entwicklung von Kafkas Begabung. Am Beginn seiner neurotischen Entwicklung standen offenbar der frühe Tod seiner beiden Brüder und die darauf folgende depressive Abkehr der Mutter. Angst und Einsamkeitsgefühle, innere Leere und sadomasochistische Phantasien begleiteten Kafka sein Leben lang. Seine Versuche, dauerhafte Beziehungen zu Frauen einzugehen, mußten scheitern, sofern sie der utopischen Suche nach einer alles verstehenden, bewundernden und schützenden Mutter galten. Einzig im Schreiben, in der literarischen Gestaltung seiner Ängste und Wünsche, in der Herstellung einer Kommunikation mit potentiellen Lesern, fand Kafka Erleichterung und Befriedigung.
Phasentrennung als Folge der Konkurrenz zwischen "statistischer" und "chemischer" Vermischung
(1977)
The fact that common thermodynamic conditions are valid for all known types of critical phases (liquid-liquid, liquid-gas, and "gas-gas") suggests that a common principle for the interpretation of material phase instability from a molecular point of view must exist. In this paper we show that the principle of competition between "statistical mixing" (i. e. random mixing) and "chemical mixing" (i. e. mixing effected under the influence of chemical interactions) can give this common inter pretation. If the equilibrium states resulting from both types of mixing are sufficiently different, phase separation occurs. We refer to our earlier papers (since 1972) in which we have applied this principle to describe liquid-liquid phase equilibria by "chemical" models, using the equilibrium constants of exchange equilibria between nearest-neighbour complexes as a measure of "chemical" mixing. In this paper we show that the well-known reduced gas-liquid coexistence curve, T/Tc =f(q/qc), can accurately be fitted by a very simple "mixture" model of molecules A with "vacan cies", provided that the contributions of both statistical and chemical mixing are incorporated into the formula for GE. From a discussion of the application to "gas-gas" phase equilibria in the hyper critical region it results that the weight factor r, by which the contribution of statistical mixing enters into GE, must depend on the density of the gas mixture. Phase separation can only occur if, by increasing pressure, the contributions to GE of statistical and chemical mixing have reached the same order of magnitude. From an attempt to apply the same principle to solid-liquid equilibria it is shown under which external conditions a critical point for this type of phase transition can be expected.
As we have shown in a recent paper, the principle of competition between "statistical" and "chemical" mixing represents a molecular thermodynamic approach to all known types of phase separation. This principle is effective if the contributions of two independent spontaneous processes enter into the thermodynamic potential by which the resulting equilibrium state of the system is determined. This is equivalent with the statement that two different forms of entropy exist which are not interchangeable, and for which the law of increasing entropy independently must be valid. As "cooperativity" is introduced by this principle, critical phenomena may be described by simple equilibrium models in which only nearest-neighbour interactions are considered.
Starting from the molar Gibbs free energy GM of the most simple binary equilibrium model z = 1 with nearest-neighbour pairs, nonclassical critical-point exponents α = 0.33 of the molar heat capacity, β = 0.33 of the coexistence curve, γ = 1.33 of the isothermal compressibility, and δ = 4.33 of the critical isotherm, are derived, which are consistent with the well-known exponent in equalities. These non-classical critical-point exponents are independent of the chemical nature of the particles because they are obtained by applying thermodynamic arguments on the coupling constant τ, by which the contribution of "statistical mixing" to GM is weighted.