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In this paper equilibrium models for the calculation of the excess Gibbs free energy of binary liquid mixtures are developed, the component A of which undergoes chain-forming self-association whilst the component B acts as an 'inert' solvent. It is shown that the extension of the well-known chain-association model of Mecke and Kempter, in which the probability of chain prolongation is assumed to be independent of chain length, is unable to establish satisfactory results because it does not exhibit sufficient unsymmetry. Reduction of the probability of chain growth with in-creasing chain length leads to an improved model with the geometric series replaced by the exponential series. This model, in which only two parameters are used, i. e. the equilibrium constants K for mutual solvation of A and B, and ρ for self-association of A, allows fitting of isothermal experimental GE /R T literature data on cycloalkanol-cycloalkane, alkanol-alkane, and NMF -CCl4 systems within the limits of experimental error. Compared with the two-parameter Wilson equation which gives equally small standard deviations, our equilibrium model has the advantage of allowing passage from GE to HE data and of being applicable to liquid-liquid equilibria.
The enthalpies of mixing at 25° of diethyl ether, di-n-propyl ether, di-n-butyl ether, di-isopropyl ether, propylene oxide, tetrahydrofuran, and tetrahydropyran with chloroform are determined by an isothermal titration method. As a result, the functions HM-f(N CHCl3) are obtained with a step width of 0.025 of the mole fraction and a relative accuracy of 1 per cent or better. Evaluation of the heat of mixing data by means of equilibrium models ("ideal associated mixture") shows that the systems of aliphatic ethers with chloroform behave rather precisely as one-step equilibria of the type A + B = AB (A = ether; B = chloroform). In the systems of cyclic ethers with chloroform, a second equilibrium step, AB + B = AB2 , must be considered, the importance of which decreases with increasing ring size of the ether. The equilibrium data calculated for the seven ether-diloroform systems are discussed.
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.
A thermodynamic theory of liquid mixtures based on a simple molecular model is developed which describes the equilibrium state as the result of a coupling between a "chemical" and a "statistical" equilibrium. The intermolecular interactions are taken into account by considering "complexes" formed between a given molecule and its z nearest neighbours. The equilibrium mole fractions of these complexes are calculated by application of the ideal law of mass action to an appropriate set of "exchange equilibria". Formulae for the excess functions GE and HE and for the activities of the components are derived for the cases z=1 and z=4. GE depends on an equilibrium constant K describing the deviation from random distribution of the equilibrium mole fractions of the complexes. HE depends on K and on an energy parameter w which is related to differences of pair interactions. K and w are independent parameters, and there is no limitation in respect to amount and sign of the excess functions. The conditions for the existence of a critical solution point are formulated; at this point GE has a value of about 0.56 R T. If a model with two equilibrium constants is used allowing for instance competition between "self-association" and "complex-formation", the existence of closed miscibility gaps becomes possible. Closed miscibility curves are calculated and the conditions for their appearance are discussed. The relations between this theory and Guggenheim's statistical lattice theory of symmetrical mixtures are pointed out.
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.
LANGEVIN equations of the type dn× (t)/dtn+...+c × (t)=K (t) constitute the starting point of a phenomenological fluctuation theory of irreversible processes. These equations are not constructed from transport equations (as in the older theory), but via a generalized MASTER equation from phase space mechanics. The MARKOFF processes of first and higher order defined by the various LANGEVIN equations are studied by the prediction theory of stationary stochastic processes. Instead of the variation principle of the ONSAGEB–MACHLUP theory one has the minimization of the prediction error. The mean relaxation path and the entropy of the considered processes are calculated. It is shown that the entropy consists of one part which is given by the relaxation path and another which is determined by the prediction error.
The relations of the theory of real gases which have first been derived by Mayer and his co-workers can be obtained in a simple way by the functional method. In this case the assumption of the pairwise additivity of the intermolecular potential can be dropped. Apart from some new relations for distributions functions the expansion of the direct correlation functions is obtained as a power series in density with coefficients consisting of integrals over Husimi functions.
Es werden allgemeine Gleichungen zur Berechnung der Verteilung der Nullstellen von der großen kanonischen Verteilungsfunktion Ξ (y) eines Gittergases in der komplexen Ebene der Fugazität y in Bethescher Näherung angegeben, die nach einem graphischen Verfahren gelöst werden können. Für das zweidimensionale, quadratische Gitter und das dreidimensionale, kubische Gitter werden die Bestimmungsgleichungen für die Nullstellenverteilung mit Hilfe des graphischen Verfahrens explizit gelöst. Die Nullstellenverteilung von Ξ (y) des eindimensionalen Gittergases wird in geschlossener Form angegeben.
The cooperative problem for a lattice gas on a plane, square lattice and on a simple cubic lattice is solved by a system of two coupled, transcendental equations, derived by a combinatorial method, which describes a homogeneous or periodical particle density on the lattice as a function of the temperature and the chemical potential of the lattice-gas.
For the particle interaction a Hard-Core potential (nearest neighbour exclusion) with a soft long-range tail is assumed. The zero-component of the Fourier-transform of this long-range interaction part can be positive or negative.
The system of transcendental equations is solved by a graphic method. As a result, the complete pressure-density state diagram and the pressure-temperature phase diagram can be drawn.
The lattice-gas exists in three stable phases: gas, liquid and solid. Three phase changes are possible: condensation, crystallization and sublimation.
Critical points of condensation and freezing are examined. The number of possible phases and phase changes at a fixed temperature depends on the geometric structure of the particle interaction.
Die „Selbstenergien“ Gn in 1 wurden durch näherungsweise Auswertung einer größeren Klasse von Selbstenergiediagrammen approximativ berechnet. Das Gleichungssystem (3.3) in 1 für die renormierten Semiinvarianten wurde umgeformt und durch zusätzliche Näherungsannahmen vereinfacht. Durch Näherungsansätze für die Semiinvarianten M2, M3,... konnten einfache Gleichungen für die Magnetisierung M1 hergeleitet werden. Diese Gleichungen wurden numerisch gelöst. Auf der Grundlage der Beziehungen (3.5) und (4.8) in 1 wurden ferner die innere Energie, die freie Energie und die Atomwärme des zweidimensionalen Ising-Ferromagneten sowie die Druck-Dichte-Isothermen des zweidimensionalen Gittergases numerisch ausgerechnet.
Die FOURIER-Nullkomponente der Bindungsmatrix Gij G(0) in 1 Beziehung (5.16) wurde durch Summation spezieller Diagramme in der sogen. „Kettenapproximation“ und der „Wassermelonenapproximation“ näherungsweise berechnet. Auf der Basis von (5.16) in 1 wurde in der Kettenapproximation und der Wassermelonenapproximation die magnetische Suszeptibilität und die Magnetisierung des dreidimensionalen ISING-Modells bestimmt. In der Kettenapproximation wurden ferner die freie Energie, die innere Energie und die Atomwärme des dreidimensionalen ISING-Ferromagneten sowie die Druck-Dichte-Isothermen des dreidimensionalen Gittergases ausgerechnet.
A theory of the luminescence lifetime of a radiation-damped classical electrical point dipole near a plane interface to a medium with different optical constants is given. The influence of the interface on the lifetime of the dipole is calculated in first approximation with the methods of molecular optics. Theoretical and experimental results for a purely dielectric interface are compared.
Excitation of CO molecules into the lowest vibrational level of the B1Σ+ electronic state by absorption of the (B 1Σ+υ′=0 →X 1Σ+ ,υ′′=0) resonance band at 1150 Å has been studied under various experimental conditions by observing the steady state fluorescence of the (B 1Σ+→A1Π) Angstrom bands. Stern-Volmer plots of the fluorescence intensities at the addition of various foreign gases yielded straight lines whose slopes k̃qм = kqм · τeff were strongly dependent on the CO sample pressure. This effect was found to be due to changes of the effective radiative lifetime of the B 1Σ+υ′=0 because of resonance trapping of the (0,0) band of the (B → X) fluorescence. The CO(B 1Σ+υ′=0) molecules are found to be quenched by He, Ne, Ar, H2 and D2 with effective collision cross sections of 0.23, 0.48, 22.4, 10.7, and 11.4 Å2, respectively, at 298 °K. In addition, an approximate value for the ratio ABA/ (ABA+ABX)of the radiative transition probabilities of the (B → A) and (B → X) transitions could be derived from the measurements.
The mass spectra and the ion molecule reactions of methylphosphine, dimethylphosphine and dimethyldeuterophosphine have been studied by ion cyclotron resonance spectrometry. About 50 ion molecule reaction are observed for each compound. The product ions can be classified as ions with two phosphorus atoms: P2R5+, P2R3+, P2R2+ and P2R+ (R = CH3 or H), as phosphonium and phosphinium ions and ions resulting from collision dissociations and charge exchange reactions. Tertiary ions with three phosphorus atoms like CH3P3H2+ (from CH3PH2) and (CH3)4P3H2 (from (CH3)2PH) have also been detected. The mechanisms of the ion molecule reactions, rearrangements, P -H- and C-H-reactivities and product ion structures are discussed, using in the case of dimethylphosphine the results obtained with the deuterated compound. Rate constants of formation of the more abundant product ions from the molecular ion and the CH3P+ ion, both odd electron particles, have been determined. The reactions with dimethylphosphine have much smaller rate constants than the reactions with methylphosphine.
The triplet state of acridine orange dissolved in methanol/water matrix was investigated by ESR. In absence of oxygen a strong temperature dependence of the spectra was observed. At low temperature (100 °K) the zero-field splitting parameters calculated from the triplet spectrum are: X/hc = 0.0050 cm-1, Y/hc= 0.0342 cm-1, Z/hc=0.0387 cm-1 , at higher temperature (140 °K) : X*(hc=0.0056 cm-1, Y*/hc=0.0206 cm-1, Z*/hc = 0.0262 cm-1 . It was assumed that the low temperature spectrum is caused by isolated molecules in the triplet state while the high temperature spectrum must be attributed to the triplet exciton state of the acridine orange dimer. From the theory of the ESR triplet exciton spectra it can be shown that in the dimer state of acridine orange the molecular planes form an angle of 50° or 130°. However, it cannot be excluded that the dimer configuration differs in the ground or excited singlet state from the triplet state.
Excimerenfluoreszenz oligomerer Assoziate von 3,4-Benzpyren in wäßrigen Lauryl-Sulfonat-Lösungen
(1969)
An Lösungen von 3,4-Benzpyren in wäßrigen Na-Laurylsulfonatlösungen wird etwa bei der doppelten kritischen Konzentration der Mizellbildung eine langwellige Fluoreszenz beobachtet, deren spektrale Zusammensetzung innerhalb der Toleranz der spektralen Zusammensetzung der Fluoreszenz des festen Kohlenwasserstoffs gleicht.
Wegen der eigenartigen Konzentrationsabhängigkeit wird diese Emission Excimeren zugeschrieben, die sich - in Analogie zum Excimeren-Mechanismus der Festkörperfluoreszenz von 3,4-Benz pyren - aus im Grundzustand vorliegenden Assoziaten bilden, die nach der Excimeren-Emission wieder zurückgebildet werden.
The electron paramagnetic resonance of copper (II)-tetrammine nitrate in solution of methanol and water has been investigated. The data obtained from the spectra at room temperature and 97 °K together with the optical transition energies determined from single crystal polarized absorption spectra at 77 °K by other authors were used to calculate the LCAO-MO bonding parameters. The bonding orbital of the ammonia molecule cannot be described by the concept of sp2 hybridization which was exclusively used in the theory. Therefore a calculation of the overlap integral S(n) for α bonding and of the superhyperfine splitting was carried out in terms of an arbitrary hybridization parametern. For ammonia, n was taken from the Duncan-Pople hybrid wave function for the lone pair orbital. The o bonding and the out-of-plane π bonding appear to have a moderate degree of covalency (α = Ϭ = 0.91; α’= 0.49). The covalent in-plane n bonding is somewhat stronger (β = 0.87) but is by no means so strongly covalent as is observed in compounds with ligands which do not exclusively coordinate through the lone pair electrons.
At low temperature nine ligand nuclear superhyperfine structure lines corresponding to the interaction of four magnetically equivalent nitrogen nuclei have been observed. The value of α' derived from the superhyperfine splitting is in excellent agreement with that obtained from the copper nucleus hyperfine structure.
Expectation values of kinetic and potential energy are calculated for some lower antibonding orbital states of simple diatomic molecules using H2+ and HeH2+ as test cases. Common LCAO-MO theory and a scaling procedure are applied which allow an analysis of atomic orbital interactions in terms of RUEDENBERG'S1 promotion and interference effect at various internuclear distances. Contributions to the total energy at different regions of interatomic separations are discussed in detail. A characteristic increase of the kinetic energy is observed for antibonding linear combinations at distances where chemical bonding occurs.
Farbzentren mit Absorptionen im Bereich des sichtbaren Lichtes entstehen bei Röntgen-Bestrahlung in Calcitkristallen, wenn die Kristalle durch Verformung eine hohe Störstellenkonzentration erhalten haben. Die Absorptionsspektren solcher Farbzentren werden ausgemessen und mit röntgenographisch bestimmten Störungsgraden verglichen. Die Bildung und die thermische Ausheilung der für die Entstehung von Farbzentren erforderlichen Störstellen wird quantitativ untersucht. Dabei wird festgestellt, daß mindestens zwei verschiedene Farbzentren auftreten, deren Konzentrationsverhältnis von der Temperaturvorbehandlung der gestörten Calcitproben abhängt.
Within the framework of the eigenchannel reaction theory above the two-particle thresholdcluster channels are introduced. The eigenchannels of the S-matrix are used, i. e. continuum stateswhich diagonalize both the S-matrix and the nuclear Hamiltonian and represent for each reactionenergy a discrete set of coupled channel wave functions with a common (eigen-) phase. Especiallythe emission of a deuteron is discussed. It is shown that the cluster channels supplement the energy-correlated channels describing the energy partition £1 + e2 = E —Ef and that asymptotic channelorthogonality holds. The characteristic feature of the cluster channels as compared to the energy-correlated channels is that their final state interaction is not limited to a finite matching volumecomparable to nuclear sizes.
The rotational spectrum of several isotopic species of HSiCl3 and CH3SiCl3 was studied in the region from 8 to 40 Gc. From the derived rotational constants the following structural parameters were obtained using KRAITCHMAN'S equations: dSi-H= (1.4655±0.0002) A, dSi-Cl= (2.0118±0.0009) A, ∢ Cl—Si—Cl= (110,60±0.25)°. Furthermore the constants for centrifugal distortion DJ= (1.2 ± 0.4) kc for HSiCl3 and DJ= (0.19 ± 0.04) kc for CH3SiCl3, for the quadrupole coupling e Q Vzz= + 12.8 Mc and the dipole moment μ= (0.86 ± 0.01) D for HSiCl3 and μ= (1.91 ± 0.01) D for CH3SiCl3 were determined. The interaction of the overall-rotation with the internal rotation is discussed for CH3SiCl3, and the hindering barrier is estimated to be less than 200 cm-1.
The microwave spectrum of CF3CCl3 has been investigated in the region from 15 to 40 GHz. A least squares analysis of the rotational constants gave the following structural parameters: dC–C= (1,5394 ± 0,001) A, dC–F= (1,330 ±0,001) A, dC-Cl = (1,7710 ± 0,0009) A, ∢ C—C—F = (109,55 ± 0,25) °, ∢ C—C—Cl= (109,55 ± 0,25) °. The splitting of the torsional satellite may be explained by the theory of KOEHLER and DENNISON.
The microwave spectra of SiFBr3 and CH3SiBr have been investigated in the region from 30 to 40 GHz. Assuming reasonable values for dSi-F, dSi-C and the methyl group a least squares analysis of the rotational constants yields dSi-Br ≮Br—Si—Br SiFBr3 (2,171 ± 0,001) A (111,36 ± 0,15)°, CH3SiBr3 (2,175±0,001) A (111,09±0,15)°. A barrier to internal rotation of about 1 kcal/mole is estimated by the intensity method.
The microwave spectrum of several symmetric and asymmetric top isotopic species of CH3CCl3 has been studied in the region from 8 to 40 GHz. A least squares analysis of the rotational con-stants gave the following structural parameters : dC-C =(1.541 ±0.001) A, dC-Cl = (1,7712 ± 0.0008) A, dC-H = (1.090 ± 0.002) A, ∢H—C—H= (110.04±0.25) ° , ∢Cl—C—Cl= (109.39 ±0.25) °. A dipole moment of μ = (1.755 ± 0.015) D has been derived from the investigation of the Stark effect of the transition J=4→5 of CH3CCl3335. From intensity measurements the barrier to internal rotation is estimated to be (1740 ± 300) cal/mol. An analysis of the spectrum of CH2DCCl2Cl37 shows conclusively that methylchloroform in its equilibrium configuration has the methyl group staggered with respect to the CCl3-group. It could be shown that there exist two torsional isomers gauche and anti with specific microwave spectra.
The microwave spectra of SiHBr3 and SiDBr3 have been investigated in the region from 28 to 40 GHz. From the rotational constants the following structural parameters were derived by a least square method: dSi-H = (1,494 ± 0,009) A, dSi-Br = (2,170 ± 0,001) Å, ∢Br-Si-Br = (111,36 ± 0,25)0. The results are compared with those obtained for other Si-halogen-compounds.
The results of spectroscopic and paramagnetic resonance investigations show that the previously prepared substance with the empirical composition [VIdip3] J · ½ py is most presumably a mixed crystal of two similar compounds of bivalent and zero-valent vanadium. The ion [VIdip3] + exists only in solution and gives no paramagnetic resonance signal, which is understood on account of a low-lying singlet ground state.
Mit Alkalimetallen reduzierte Lösungen von 2,2′-Dipyridyl liefern ein ESR-Signal, dessen Hyperfeinstruktur vom Reduktionsmittel abhängt. Bei Verwendung von Lithium beobachtet man das Spektrum des Ionenpaares (Li+, dip-), mit Kalium dagegen erhält man im wesentlichen das ESR-Spektrum des Anionradikals dip-. Seine Hyperfeinstruktur wird quantitativ interpretiert. Abweichungen zwischen den daraus entnommenen experimentellen Spindichten und theoretischen Spindichten, die mittels der HÜCKELschen Theorie erhalten wurden, deuten auf Grenzen in der Anwendbarkeit dieser Theorie.
Arbeiten zur experimentellen Erhärtung der Vorstellungen über die Biogenese von Terpenen aus den Hemiterpenalkoholen Dimethylvinylcarbinol oder Prenol führten zur Auffindung der Dichloressigsäure als eines aliphatischen Polymerisationsbeschleunigers sowohl dieser beiden Alkohole als auch des ihnen zugrunde liegenden Dienkohlenwasserstoffs, des Isoprens. Die Ergebnisse mit dieser einfachen Carbonsäure regen zur Prüfung natürlicher organischer Säuren als Fermentmodelle an.
This paper reports about the fine structure in the O—K-spectra of the oxides BeO, MgO, CaO, SrO, BaO, Sc2O5, Y2O3, La2O3, Sm2O3, Yb2O3, NiO and ZnO. The spectra show the satellite lines α3, α4, α5, α6 on the short wavelength side of the main line α1,2 and a shoulder β′ on its long wavelength side. The wavelengths of all lines depend on the nature of the oxide. For the positions of the lines Kα1.2 in the spectra no systematic relation to other data of the oxides is observed. On the other hand the distance of the a4-satellite from the α1,2-line decreases with increasing electronegativity of the metal atom in the oxide. This distance can be used as a measure for the ionic character of the metal-oxygen bond in these compounds.
The O-K-spectra of α- and γ-Al2O3, β-Ga2O3 and In2O3 were measured with a high-resolution grating spectrograph using the method of electron excitation. The spectra were corrected for the nonlinear response of the photographic emulsions. A shift of the O - K-emission band edge of γ-Al2O3 to lower energy with respect to that of α-Al2O3 and a fine structure within all O -K-bands were observed for the first time. The details of the spectra are discussed in relation to the energy level diagrams, crystal structure, and chemical bond of these oxides.
Investigations were made of energy-transfer in liquid scintillators under UV- and β-excitation. The influences of n-hexane and methanol as diluting solvents on the scintillation process in p- terphenyl-toluene were measured. Differences of energy transfer under β - and UV-irradiation are discussed. Radiationless energy-transfer occurs over distances from 15 to 32 Angström units. Quenching effects of phenol on p-terphenyl, 2,5-diphenyl-oxazole, and 2,4 (or 5) -diphenyl-imidazole were studied. Oxygen-quenching in liquid scintillators containing hydroxy-benzenes was investigated. The results are in correspondence with the KALLMANN-mechanism of radiationless energy-transfer. — Further investigations were made of the connection between the chemical structure of aryl-imidazoles and their scintillation properties. Scintillation properties depend on spectral data. The results aprove HELLERS postulates, concerning structural requirements for good scintillation properties of organic liquid scintillators.
Die grundlegenden Untersuchungen von KALLMANN führten in den letzten Jahren meist auf empirischem Wege zur Entdeckung zahlreicher organischer Flüssigkeits-Szintillatoren, die besonders in der Meßtechnik hochenergetischer Teilchen und solcher mit sehr geringer Strahlungsenergie, Eingang gefunden haben. Es soll in dieser Arbeit versucht werden, einen Zusammenhang zu geben zwischen der chemischen Konstitution und den Szintillator-Eigenschaften einiger organischer Verbindungen.
Das Hückelsche zweite Näherungsverfahren wird durch Mitberücksichtigung der höheren Atomzustände erweitert. Dabei ergibt sich die Erklärung für das Scheibesche Phänomen. Der Begriff „theoretische Sonderenergie (Resonanzenergie)“ wird richtiggestellt. Die bekannten Schwierigkeiten, die sich beim Vergleich spektroskopischer und kalorischer Energiewerte im Rahmen der Einelektronentheorie der π-Elektronensysteme bisher immer ergeben haben, verschwinden.