berichte der bunsen-geseulschaft fur physikalische chemie
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Transcript of berichte der bunsen-geseulschaft fur physikalische chemie
BERICHTE DER BUNSEN-GESEULSCHAFT FUR PHYSIKALISCHE CHEMIE AN INTERNATIONAL JOURNAL OF PHYSICAL
Jahresregister von Band 91 (1987)
Herausgeber Deutsche Bunsen-Gesellschaft für Physikalische Chemie e.V. Carl-Bosch-Haus, Varrentrappstraße 40/42 D-6000 Frankfurt am Main 90
Telefon (069) 7917-201
Bchriftleiter Konrad Georg Weil Institut für Physikalische Chemie Technische Hochschule Darmstadt Petersenstraße 20 D-6100 Darmstadt
Telefon (06151) 162498
Alarich Weiss Institut für Physikalische Chemie Technische Hochschule Darmstadt Petersenstraße 20 D-6100 Darmstadt Telefon (06151) 162607
Redaktion Redaktion „Berichte der Bunsen-Gesellschaft" Institut für Physikalische Chemie Petersenstraße 20, D-6100 Darmstadt
Telefon (06151) 162498
Beratergremium Ernst Ulrich Franck, Karlsruhe Friedrich Kohler, Bochum Werner Kutzelnigg, Bochum Hermann Schmalzried, Hannover Heinz Georg Wagner, Göttingen Gerhard Wegner, Mainz Albert Weller, Gött ingen Herbert Zimmermann, Freiburg
Verlag
vor Verlagsgesellschaft
V C H Verlagsgesellschaft mbH Postfach 1260/1280 D-6940 Weinheim Federal Republic of Germany Telefon (06201) 602-0 Telex 465516 vchwh d Telefax (06201) 602328
Inhaltsverzeichnis von Band 91 (1987) (Autorenverzeichnis, Sachverzeichnis, Buchbesprechungen, Personalnachrichten)
A. Autorenverzeichnis
Abrantes, L. ML, R. Peat, L. M. Peter, A. Hamnett: Electroreflec-tance at the Semiconductor/Electrolyte Interface. A Comparison of Theory and Experiment for n-GaAs 369
Acs, Α., R. Schmidt, H.-D. Brauer: Generation and Deactivation of ' Ο ^ ' Δ ) by Helianthrene and He-lianthrene-Derivatives 1331
- siehe H.-D. Brauer 1337 Albers, P. W., G. H. Sicking, L. G.
Earwaker, J. B. A. England: Depth Profiling of Hydrogen Isotopes in Metals by Elastic Recoil Detection and Nuclear Reaction Techniques under In-Situ Conditions 573
Allongue, P., H. Cachet: Photoca-pacitance Study of n-GaAs/Elec-trolyte Interfaces 386
Alonso, M. C , siehe Μ. Costas . . . 184 Anderko, Α., siehe A. Ksiazczak . . . 1048 Andrecv, Β. Μ., G. Η. Sicking: Hy
drogen Equilibrium Separation Factors in Metal/Hydrogen Systems, a Synopsis on the Basis of the Localized Harmonic Oscillator Model 177
Andres, K., siehe Κ. Späth 909 Anic, S., Lj. Kolar-Anic: The Influ
ence of Potassium lodate on Hydrogen Peroxide Decomposition in the Bray-Liebhafsky Reaction 1010
Anik, S., M . G. Frohberg: Thermodynamics and Solubility of Oxygen in Liquid Bismuth-lead and Bismuth-antimony Alloys 790
Apelblat, Α., Ε. Manzurola: Thermodynamic Analysis of Partition Data in the CaCl 2 -H 2 0-n-Oc-tanol and CaCl 2 -H 2 0-n-Bu-tanol Systems.at 298.15 Κ 1387
Appel, I . , Κ. Kleinermanns: Fluorescence Excitation Spectra of Hydrogen-Bonded Cresol-Isomers in Supersonic Free Jets 140
Aracil, J., R. G. Rubio, J. A. R. Re-nuncio, M . Diaz Pena: Vapour-Liquid Equilibrium of n-Tetra-decane and of n-Hexadecane with Hexafluorobenzene and with Hexafluorobenzene -I- Benzene at 323.15 Κ 603
Arendt, P.: Diffusion of Excess Electrons in Decomposing Liquid Metal-Ammonia Solutions in the High-Conducting State, Injected into a Zero-Electric Field Space . 1363
Armitage, H., U . Blömer, I . Genge, A. Khuen, Ε. E. Wille, D. Ziessow: Fortschritte in der 2D-NMR-Spektroskopie mit Rauschanregung 1115
Auweraer, Μ. Van der 869
Badiali, J. P.: The Jellium Model in Electrochemistry 270
— siehe M . L. Rosinberg 276 Bässler, H., siehe F. Stolzenburg . . . 853 Bagdasarian, V. V., siehe Α. A. Sha-
hinian 670
Bahr, Ch., G. Heppke: Ferroelectric Liquid Crystals — Properties of the Smectic C Phase and the Smectic Α Phase of Compounds with High Spontaneous Polarization 925
Balducci, G., G. Gigli, M . Guido: Thermochemical Study of the Gaseous Molecules EuNb0 3 , EuNbO,, EuNb 2 0 6 and of the Niobium Oxides NbO and N b 0 2 635
Bartsch, Ε., Η. Bertagnolli: Test of a Symmetry Reduced Extended R1SM (XRISM) Equation Against Diffraction Experiments on Liquid Benzene and Hexafluorobenzene and Evaluation of Optimized Potentials 745
Bäuerle, P., M . S. Wrighton, Ο. M . R. Chyan, C W. Spangler: New Conducting Polymers of Some Bithiophene- and Bis-N-Methyl-pyrrole Polyenes, Their Properties and Their Application in M i -croelectrochemical Devices 889
Baumann, F., siehe S. Schneider . . . 1225 Beck, F., G. Heydecke: On the
Mechanism of the Cathodic Reduction of Anthraquinone to An-throne 37
- P. Braun, Μ. Oberst: Organic Electrochemistry in the Solid State-Overoxidation of Polypyr-role 967
Becker, A. C, U. Schurath: NBr (b1 Σ + , a1 Δ) in Solid Argon: Effect of the Rare Gas Matrix on Radiative and Radiationless Processes 1238
Becker, F., siehe Μ. Erol 731 Becker, Κ. D., F. Rau: High Tem
perature Ligand Field Spectra in Spinels: Cation Disorder and Cation Kinetics in N i A l 2 0 4 1279
Beden, B., siehe J.-M. Leger 336 Belkoura, L., siehe Μ. Jungk 507 - F. P. Harnisch, S. Kölchens, Th.
Müller-Kirschbaum, D. Woer-mann: Study of the System Nitro-benzene/Isooctane in the Vicinity of its Critical Point: Static and Dynamic Light Scattering and Reevaluation of Ultrasonic Absorption Data 1036
Bertagnolli, H., siehe Ε. Bartsch . . . 745 - Τ Engelhardt, Β. Lengeier: Local
Order in Liquid Bromobenzene — EXAFS Measurement and its Combination with X-Ray and Neutron Diffraction Results 1287
Bethune, D. S., siehe J. K. Sass 320 Beuthien, H., A. Torkler, W. Gunßer,
W. Niemann: X-ray Investigations of the Thulium-Iron Crystallization Process 1296
- siehe A. Torkler 1300 Bhat, S. N , siehe Ν. Van Nhu . . . . 525 Biasio, A. Di , siehe F. Bordi 737 Bignell, C. M. , siehe P. J. Dunlop . 156 - siehe P. J. Dunlop 817 Biswas, S. R , siehe Τ F. Sun 1013 Bitterling, Κ., siehe F. Willig 869
Blömer, U., siehe H. Armitage . . . . 1115 Blümich, B , C. Böflel, G. S. Harbi
son, Y. Yang, H. W. Spiess: Two-Dimensional MAS NMR: New Prospects for the Investigation of Partially Oriented Polymers 1100
- siehe C. Chmidt 1141 Blume, Α., siehe W. Hübner 1127 Bockhorn, Η., F. Fetting, A. Hedd-
rich, G. Wannemacher: Untersuchung der Bildung und des Wachstums von Rußteilchen in vorgemischten Kohlenwasserstoff — Sauerstoff Unterdruckflammen 819
Bodensteiner, T , siehe R. Winter . . 1327 Böflel, C, siehe B. Blümich 1100 Böhm, M. C, R. Ramirez, Α. Μ.
Oles: The One-Dimensional Band Structure of (Tetrazapor-phyrinato)iron(Il) 717
- siehe S. Fleck 1167 Börsch-Pulm, Β., siehe G. Hohl-
neicher 929 Borchers, D., Al. Weiss: Structures
and Phase Transitions in Pipe-razinium Hcxachlorometallates, (C 4 HpN 2 ) [MCl 6 ] , Μ = Te, Pb, Pt, and (C 4 H 1 2 N 2 )[MC1 6 ] · 3 H 2 0 , Μ = Sn. A X-ray Diffraction and 3SC1 NQR Study 1182
Borczyskowski, C. von: Optically Detected NQR on Matrix-Isolated Organic Molecules . . . 1137
Bordi, F., C. Cametti, A. Di Biasio: Osmotic Pressure of Aqueous Rod-Like Polyelectrolyte Solutions with Mono- and Di-Valent Counterions 737
Borggreven, J. Μ. P. M., siehe Η. P. F. Scholberg 129
- siehe Η. P. F. Scholberg 135 Boudh'hir, Μ. Ε., siehe Μ. L. Rosin
berg 276 Bougeard, D., siehe S. Schroetter . . 1217 - N . Le Calve, B. Pasquier: Crystal
Dynamics and Phase Transitions of Malonitrile 1273
Boyadjiev, B.: Der Einfluß der Nah-ordnungsstruktur auf die chemischen Verschiebungen der Aro-matenprotonen in flüssigen M i schungen von Acetonitril mit 5 aromatischen Lösungsmitteln . . . 225
Bräuchle, Chr.: Optical Solid State Spectroscopy by Holographie Grating Techniques with Quantum Limited Sensitivity 1247
Brandner, G., F. L. Dickert, Ε. Lehmann: The Formation of Carben-ium Ions and Naked Anions by the Protonation of Phthalophen-one with a Super Acid 740
Brauer, H.-D., siehe A. Acs 1331 - A. Acs, R. Schmidt: The Role of
Geminate Reaction in the Self-Sensitized Photooxygenation of Helianthrene and Helianthrene-Derivatives/Encounter- and Re-encounter Probabilities 1337
Braun, D., siehe Η. Yersin 1228 Braun, P., siehe F. Beck 967
VI Inhaltsverzeichnis von Band 91 (1987) — Autoren Verzeichnis
Brei, Μ., H. Jander, H. Gg. Wagner: Integral Carbon Mass Balance in Premixed Sooting Flames 30
Brückner, W., K. Grande, Η. A. 0ye: Vapour Pressure of the AlCl r POCh System 561
Brummer, S., AI. Weiss: NQR Spectroscopy and Structure of Pho-tochromic 2,3,4,4-Tetrachloro-1 -oxo-l,4-dihydronaphthaline and 2 ,4 ,4 -Tr i ch lo ro - l ,4-dihydro-naphth[l ,8-cd]isothiazole-l , l -dioxide 873
Buchberger, Ε. Μ., B. Mollay, W.-D. Weixelbaumer, H. F. Kauffmann, W. Klöpffer: Time-Resolved Fluorescence of Bichromophoric Rotors — Conformational Dynamics of l,3-di(N-carbazolyl)pro-pane 1209
Buchmann, L.-M., E. Illenberger: The Interaction of CFCU and CF 2C1 2 with Solid Surfaces Studied by Thermal Desorption Mass Spectroscopy 654
Büttner, H., siehe U. Sum 957
Cachet, Η., siehe P. Allongue 386 Calve, Ν. Le, siehe D. Bougeard . . . 1273 Cametti, S., siehe F. Bordi 737 Cardon, F., siehe L. S. Yun 390 Carnie, S. L.: Recent Developments
in Double Layer Theory 262 Castro, C. A. Nieto de, siehe U. V.
Mardolcar 152 Chang, R. K.: Surface Enhanced Ra
man Scattering at Electrodes: A Status Report 296
Chyan, O. M . R., siehe P. Bäuerle . 889 Clausen, B. S., siehe W. Niemann . . 2192 Conrady, R., W. Müller-Warmuth,
B. Krebs, G. Schwetlik, M . Wien-. kenhöver: Nuclear Quadrupole Coupling and Electronic Structure of Boron Trihalide Adducts with Chalcogen Ligands 1322
Conway, Β. Ε., T. C. Liu: Behaviour of Surface Intermediate States in Anodic 0 2 Evolution Electroca-talysis at C o 3 0 4 on N i and Ti Substrates 461
— D. P. Wilkinson, D. F. Tessier: Catastrophe Situation for Potential-Assisted Electron Transfer in Relation to Temperature-Dependence of Tafel Slopes 484
Costas, Μ., M . C. Alonso, A. Heintz: Experimental and Theoretical Study of the Apparent Molar Volumes of 1-Alcohols in Linear Hydrocarbons 184
Dachwitz, Ε., Μ. Stockhausen: A Dielectric Relaxation Study of Self and Heteroassociation in Binary Liquid Mixtures of Three Pyrrolidinones with Alcoholes and Water 1347
DalFO, L., H . Heydtmann: Kinetic Study of Chemically Activated Fluorocyclopropane 24
Decker, F., J. R. Moro, J. L. S. Ferreira, Μ. Vanzi: Growth and Morphology of Electrodeposited Semiconducting Films 408
Degen, J.: Application of Photon Count Statistical Measurements to the Stationary Fluorescence of Fluoranthene 1215
Denninger, G., siehe Th. Schimmel . 901 Deul, R., siehe R. Diguet 551
Dick, B.: Fluorescence Studies of Excited State Intramolecular Proton Transfer (ESIPT) in Molecules Isolated in Solid Argon: 3-Hy-droxyfiavone and 2,5-Bis(2-ben-zoxazolyl)hydroquinone 1205
Dickert, F. L., siehe G. Brandner . . 740 Dieckmann, R., siehe P. Franke . . . 48 - Μ. R. Hilton, Τ. Ο. Mason: De
fects and Cation Diffusion in Magnetite (VIII): Migration Enthalpies for Iron and Impurity Cations 59
Diguet, R., R. Deul, E. U. Franck: Static Dielectric Constant and Density of Supercritical Meth-ane-Methanol-Mixtures to 200 MPa 551
Dong, S., R. Jiang: Research on Chemically Modified Electrodes: Electrocatalytic Reduction of Dioxygen by Iron Tetraphenyl-porphyrin Modified Glassy Carbon Electrode with Heat Treatment 479
Dormann, E., G. Sachs: The Low-Temperature Phase of the Organic Conductor (Fluoranthe-ne)2PF6 879
- siehe P. Strohriegel 918 Dorris, S., siehe Μ. Martin 779 Driessens, F. C. M., siehe Η. P. F.
Scholberg 129 - siehe Η. P. F. Scholberg 135 Dunlop, P. J., H. L. Robjohns, C. M.
Bignell: Diffusion Coefficients and Thermal Diffusion Factors for the Systems He — CF 4 and N e - C F 4 156
- C M . Bignell: Diffusion in Binary Mixtures of Ammonia with Noble Gases 817
Durfee, W. S., siehe F. Willig 869 Durham, W. Β., Η. Schmalzried:
Chemical Potential Measurements on Nonhydrostatically Stressed Solids 556
Earwaker, L. G., siehe P. W. Albers 573 Ehbrecht, J., W. Hack, P. Rouvei-
rolles, H. Gg. Wagner: Hydrogen Abstraction Reactions by NH2(X2B,)-Radicals from Hydrocarbons in the Gas Phase 700
Eichberger, R., siehe F. Willig 869 Elfenthal, L., Κ. Leitner, J. W.
Schultze, O. Meyer: Migration of High Energy Defects After Pd-Implantation in Oxide Films on Titanium 432
Elfmger, G , siehe S. Schneider 1222 Engelhardt, T , siehe H. Bertagnolli 1287 England, J. Β. Α., siehe P. W. Albers 573 Enkelmann, V., siehe P. Strohriegel 918 - K. Göckelmann: Structure and
Phase Transitions of Aromatic Radical Cation Salts — a New Class of Organic Metals 950
Ernst, R. R.: Advanced N M R Methods for Liquids and Solids: Two-Dimensional Spectroscopy 1087
Erol, Μ., M . Kocak, P. Richter, A. Steiger, F. Becker: The Influence of Dissolved Electrolytes on the Miscibility of Binary Liquid Systems with Closed Miscibility Gaps 731
Ewig, F., D. Rhäsa, R. Zellner: K i netics, Energetics, and OH Product Yield of the Reaction C H 3 0 + 0( 3 P) -> C H 3 0 2 -> Products 708
Ezquerra, Τ. Α., siehe J. Rühe 885
Fechter-Rink, Ε., siehe H.-G. Kuball 1266 Feiner, A. S., A. J. McEvoy, Ν.
Vlachopoulos, Μ. Grätzel: Electrochemical Photooxidation of Carboxylates on CdS Electrodes 399
Fernandez, Α.: Theory of Scaling for Fluctuations in Thermal Explosion Conditions 159
— Renormalization Group from a Center Manifold Reduction in Dynamic Critical Phenomena . . 570
— Statistical Weights for Primary Structures of Inhomogeneous Polymer Chains 611
— Statistics of Disordered Polymers: An Effective Hamiltonian and its Associated Gibbs Measure 753
— Intrinsic Fluctuations in Ma-cromolecular Self-Replicating Systems 1002
Ferrer, I . J., P. Salvador: Photoetch-ing of Polycrystalline n-CdS Film Electrodes in a Photoelectro-chemical Cell: an Electrolyte Electro reflectance Study 374
Fetting, F., siehe Η. Bockhorn . . . . 819 Ferreira, J. L. S., siehe F. Decker . . 408 Fesser, K., siehe U. Sum 957 Fleck, S., siehe AI. Weiss 913 — M. C Böhm, N. Weiden, AI.
Weiss: Hydrogen Bonds in Ammonium Hydrogen-DL-Malate Monohydrate Studied by 2 H -NMR, IR, and LCAO - MO Calculations 1167
— siehe A. Kehrer 1176 Förstcrling, H. D., siehe H. Schreiber 798 Fojtik, Α., siehe L. Spanhel 88 — siehe A. Henglein 441 Fontaine, F., siehe J. Ledent 112 Frahm, J., siehe K.-D. Merboldt . . . 1124 Franck, E. U., siehe R. Diguet . . . . 551 — siehe T. Krader 627 Franke, P., R. Dieckmann: Defect
Structure and Transport Properties of Manganese Oxides: (III) Relaxation Kinetics of Manga-nosite ( M n ^ O ) in CO/C0 2 Gas Mixtures 49
Freeman, P. Α., siehe R. Hayes 231 Friedrich, J., siehe W. Köhler 858 Frohberg, Μ. G , siehe S. Anik . . . . 790 Furlong, D N., siehe R. Hayes . . . . 231 Furuya, N. , siehe S. Motoo 457
Gäl, D., siehe G. Moger 794 Gallhuber, E., siehe Η. Yersin 1228 Gamsjäger, Η., siehe Ε. Königsber
ger 785 Garnier, F., siehe D. Gningue 402 Gaube, J., siehe L. König 116 Genge, I . , siehe H. Armitage 1115 Gerhard, W., siehe L. König 116 Gerischer, H., D. Kolb 262 — M . Lübke: The Electrochemical
Behaviour of η-Type Silicon (lll)-Surfaces in Fluoride Containing Aqueous Electrolytes . . . 394
— siehe Τ. Solomun 412 — siehe R. Mclntyre 488 Gerads, H., siehe K. Hilpert 190 Gigli, G , siehe G. Balducci 635 Gläser, W., siehe R. Winter 1327 Gliemann, G., siehe R. Schwarz . . . 1233 Gningue, D., G. Horowitz, F. Gar
nier: Stabilization of CdS and CdSe Photoelectrodes Modified by a Catalyst-Containing Poly-thiophene Coating 402
Göckelmann, Κ., siehe V. Enkelmann 950
Goez, Μ.: Extremely Sensitive Op-
Inhaltsverzeichnis von Band 91 (1987) — Autorenverzeichnis V I I
tical Detection System for Stopped-flow Measurements of Reactions with Very High Rate Constants or Small Absorbance Changes 616
Gogu, E., siehe D. Schweitzer 890 — siehe W. Kremer 896 Gomes, W. P., siehe L. S. Yun . . . . 390 Gordon, J. G , siehe Κ. A. Bunding
Lee 305 Goto, Ν., siehe Τ. Ohtsuka 313 Gottesfeld, S.: The Time-Resolved
Response of Semiconductor-Electrolyte Interfaces to Short Pulses of Illumination 362
Grätzel, M., siehe A. S. Feiner . . . . 399 Grande, K., siehe W. Brockner 561 Greger, M., L. Riekert: Nonequili-
brium Phase Transitions in Solid Catalysts for Oxidation 1007
Grieser, F., siehe R. Hayes 231 Gross, F., siehe K. Späth 909 Gruner-Bauer, P., siehe P. Strohrie
gel 918 Grupp, Α., siehe M. Mehring 1132 Gütlich, P., siehe L. König 116 Guido, M., siehe G. Balducci 635 Gunßcr, W., siehe H. Beuthien 1296 — siehe A. Torkler 1300
Haak, R., siehe R. Tenne 597 Haarer, D., siehe H. Kaul 845 Hack, W.. siehe J. Ehbrecht 700 Hänickc, W., siehe K.-D. Merboldt. 1124 Hallcy, J. W., J. Hautman: Molecu
lar Dynamics Study of Raman Scattering and Infrared Absorption of Ferrous and Ferric Ions in Aqueous Solution 491
Hamnett, Α., A. R. Hillman: Ellip-sometric Study of the Growth of Thin Organic Polymer Films . . . 329
— siehe L. M . Abrantes 369 Hansen, G. J., W. N . Hansen: In
frared Spectroscopy of the Electrochemical Double Layer Via Electrode Emersion 317
Hansen, W. N., siehe G. J. Hansen . 317 Harbison, G. S., siehe Β. Blümich . 1100 Harnisch, F. P., D. Woermann: En
thalpy of Demixing of a Binary Liquid Mixture of Critical Composition: Study of the System Iso-butyric Acid/Water 811
— siehe L. Belkoura 1036 Hartmann, J., Al . Weiss: Nuclear
Quadrupole Resonance of Substituted Anilinium Halides. l 2 7 I and 7 9Br NQR Studies of Tolui-dinium and Paraphenylenediam-monium Halides 1195
Hautmann, J., siehe J. W. Halley . . 491 Hayes, R., P. A. Freeman, P. Mul-
vaney, F. Grieser, Τ. W. Healy, D. N . Furlong: The Effects of pH and Adsorbed Hydrolysed Metal Ions on the Photodissolution of Colloidal Cadmium Sulphide 231
Healy, T. W., siehe R. Hayes 231 Heddrich, Α., siehe Η. Bockhorn . . 819 Heidmann, C. P., siehe K. Späth . . 909 Heindl, D., siehe P. Strohriegel 918 Heinze, J., M . Störzbach, J. Morten-
sen: Experimental and Theoretical Studies on the Redox Properties of Conducting Polymers . . 960
Helberg, Η. W., siehe W. Kremer . . 896 — Electronic Excitations in (BEDT-
TTF)-Salts 899 Heimle, Μ., siehe F. Hentsch 911 Heintz, Α., siehe M . Costas 184 — An Efficient Calculation Proce
dure of Predicting Heat Conductivities of Complex Gaseous Mixtures 190
Heinze, J., siehe Κ. Hinkelmann . . . 243 Henderson, D., Ε. Leiva, W.
Schmickler: The Jellium/Hard Sphere Electrolyte Interface . . . . 280
Henglein, Α., siehe L. Spanhel 88 — A. Fojtik, H. Weiler: Reactions
On Colloidal Semiconductor Particles 441
— siehe L. Spanhel 1359 Henning, I . , siehe D. Schweitzer . . . 890 Hensel, F., siehe R. Winter 1327 Hensler, G., siehe Η. Yersin 1228 Hentsch, F., Μ. Heimle, D. Könge-
ter, Μ. Mehring: Knight Shift in the Organic Conductor (Fluoran-thenyl)2AsF6 911
Heppke, G , siehe Ch. Bahr 925 Hermann, W., A. Raith, H. Rau: Dif
fusion of Fluorine in Silica 56 — siehe Η. Rau 833 Heusch, R., F. Kopp: Structures in
Mixtures of p-tert-Octylphenol Polyoxyethylene and Water. 1. Triton X-114R 806
Heydecke, G , siehe F. Beck 37 Heydtmann, Η., siehe L. DalPO . . . 24 — siehe U. Schwanke 1043 Hillmann, A. R., siehe A. Hamnett . 329 Hilpert, Κ., H. Gerads, D. Kobertz,
M. Miller: Composition and Thermochemistry of the Equilibrium Vapour of the Systems Nal - Fel 2 and Nal - Pbl 2 200
— siehe Μ. Miller 642 — Κ. Ruthardt: Determination of
the Dissociation Energy of the Cr 2 Molecule 724
Hilton, M . R., siehe R. Dieckmann . 59 Hinkelmann, Κ., J. Heinze: Analysis
of "Two-electron" Transfer Processes by Cyclic Voltammetry . . . 243
Höfer, P., siehe Μ. Mehring 1132 Hoffmann, Η., J. Kalus, Β. Schwand-
ner: Small-angle Neutron Scattering-measurements on a Surfactant System Consisting of Cat-ionic and Anionic Surfactant Molecules 99
— J. Kalus: Small Angle Neutron Scattering Measurement on a M i -cellar Solution of Dodecylam-monium-Triiluoro-Acetate Molecules 546
Hohlneicher, G , B. Borsch-Pulm: Classification of Higher Excited States in (4N+ 2)-Annulenes and Related π-Electron Systems 929
Homann, Κ. H., siehe Μ, Schottler. 688 — siehe Ch. Kubitza 695 — J. Traube: Use of a Wien Filter
for Mass and Velocity Analysis of Charged Soot Particles in a Nozzle Beam 828
Horiuchi, K., R. Ikeda, D. Naka-mura: Phase Transition and Anionic Motion in Solid [(CH 3 ) 2 NH 2 ] 2 SnCl 6 as Studied by the Temperature Dependence of 3 5C1 NQR Frequencies and Chlorine Nuclear Relaxation Times Determined with a Pulsed NQR Spectrometer 1351
Horowitz, G., siehe D. Gningue . . . 402 Hoshi, T , J. Okubo, M . Yananoto,
S. Tanabe: Electronic Spectra and Structures of Cation Radicals Produced from p-Phenylenedi-amine and 2,7-Diaminonaphtha-lene 1069
Hsin-min, J., siehe U. Nickel 997 Hübner, W., A. Blume: 2 H-NMR-
Spectroscopic Investigations of Phospholipid Bilayers 1127
Hürth, Μ., D. Woermann: Deuterium Isotope Effects in Binary Critical Mixtures Study of the Systems Methanol/Isooctane and Acetonitril/Water 614
Hüsser, Ο. Ε., Η. von Känel: Optically Generated Space Charge Layer in Insulators: Electrolyte Electroreflectance at the B i l 3 / Electrolyte Interface 379
Huck, H.: Die Messung der Ultraschall-Diffusion an einer Elektrode und ihre praktische Anwendung 647
Huth, M. , siehe O. Schrems 1261
Ikeda, R., siehe S. Sato 122 — siehe K. Horiuchi 1351 Ikegami, K., siehe N . Yoshida 666 Illenberger, E., siehe L . -M. Buch
mann 654
Jaegermann, W., siehe M . Sander . 416 Jander, H., siehe M . Brei 30 Jöllenbeck, Κ. M. , J. U. Weidner:
Röntgen Strukturuntersuchung des flüssigen Silicium-, Germanium- und Zinntetrachlorids. Ein Beitrag zur Frage einer gemeinsamen Flüssigkeitsstruktur. I . Streuexperimente an den reinen Komponenten und ihren binären Mischungen 11
Röntgenstrukturuntersuchung des flüssigen Silicium-, Germanium- und Zinntetrachlorids. Ein Beitrag zur Frage einer gemeinsamen Flüssigkeitsstruktur. I I . Bestimmung der individuellen partiellen Paarkorrelationsfunktionen. Vorschlag eines einheitlichen Strukturmodells 17
Jungermann, G , G. Luft: Vergleich der Perturbed-Hard-Chain-Theorie mit der Freien-Völumen-Theorie und der Flory-Huggins-Theorie zur Berechnung von Phasengleichgewichten von Ethy-len/Polyethylen-Mischungen unter Hochdruck 541
Jungk, M . , L. Belkoura, D. Woermann, U . Würz: Study of a Binary Critical Mixture of 2,6-Dimethyl Pyridine/Water: Measurements of Static and Dynamic Light Scattering and Specific Heat Near the Lower Critical Point 507
Kaiser, W., A. Seilmeier: Schwingungsenergieumverteilung in Lösung 1201
Känel, Η. von, siehe Ο. Ε. Hüsser . 379 Kalus, J., siehe H. Hoffmann 99 — siehe H . Hoffmann 546 Kappus, M . , siehe H.-G. Kuball . . . 1266 Karaaslan, H., siehe E. Yurtsever . . 600 Kassner, K., siehe P. Reineker . . . . 864 Kauffmann, H. F., siehe Ε. M . Buch-
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Generation and Transport in Po-lyvinylcarbazole: A Model System for Polymerie Photoconduc-tors 845
Kehrer, Α., S. Fleck, AI. Weiss: 7 9 ' 8 , Br and 1 2 7 I NQR Studies of Hydro-bromides and Hydroiodides of Amino Acids and Dipeptides . . . 1176
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Keldenich, J., siehe G. Peschel 285 Keller, H. J., siehe D. Schweitzer . . 890 — siehe W. Kremer 896 Keller, J. U.: Thermodynamics of
Non-Isothermal Coadsorption Processes 528
Kersting, H.-J., siehe Η. Stegemeyer 3 Khuen, Α., siehe Η. Armitage 1115 Kishimoto, S., siehe N . Yoshida . . . 666 Kita, H., siehe K. Uosaki 447 Kiyan, Ν. Z., siehe Ο. A. El Seoud . 825 Klein, B., siehe U. Nickel 997 Kleinermanns, K., siehe I . Appel . . 140 Klöpffer, W., siehe Ε. M . Buchber-
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Highly Repeated Sequences in Eukaryotic DNAs by Scanning Microcalorimetry 206
Klutz, T , siehe D. Schweitzer 890 Knözinger, Ε., siehe W. Langel 1257 — siehe Ο. Schrems 1261 Kobertz, D., siehe Κ. Hilpert 200 Kogak, Μ., siehe Μ. Erol 731 Koch, Ε., Zs. Nagy-Ungvarai: New
Strategies for Studies on the K i netics and Energetics of the Be-lousov-Zhabotinskii Reaction . . 1375
Köhler, W., J. Friedrich: Configura-tional Dynamics of Doped Low Temperature Glasses and Polymers 858
Kölchens, S., siehe L. Belkoura 1036 Köngeter, D., siehe F. Hentsch 911 König, U., Μ. Μ. Lohrengel, J. W.
Schultze: Computer Supported Pulse Measurements of Current and Capacity during Fast Oxide Formation on Iron 426
Königsberger, Ε., Η. Gamsjäger: Solid-Solute Phase Equilibria in Aqueous Solution. 1. Solubility Constant and Free Enthalpy of Formation of Huntite 785
Kohler, F., siehe Ν. Van Nhu 525 Kolar-Anic, Lj. , siehe S. Anic 1010 Kolb, D., siehe Η. Genscher 262 Kolb, D. Μ., siehe Μ. S. Zei 349 Kollhoff, Η., siehe W. Langel 1257 — siehe O. Schrems 1261 Kolodziejski, W.: Paramagnetic
Probe for Molecular Interactions: I I . 7 L i N M R Study of Lithium Cation Solvation by a Nitroxide Radical 95
Kopp, F., siehe R. Heusch 806 Kortbeek, P. J., siehe Τ. F. Sun . . . 1013 Krader, Τ., Ε. U . Franck: The Ter
nary Systems H 2 0 - C H 4 - N a C l and H 2 0 - C H 4 - C a C l 2 to 800 Κ and 250 MPa 627
Krebs, Β., siehe R. Conrady 1322 Kremer, W., H. W. Helberg, Ε.
Gogu, D. Schweitzer, H . J. Keller: Microwave Conductivity in the Pure and Iodine-Doped Organic Conductor a-(BEDT-TTF)?I3 . . . 896
Kremnitz, W., siehe W. Nitsch 218 Kröhnke, C, siehe Η. Rühe 885 — Single Crystals from Optically
Active Diacetylenes and Polydi-acetylenes 982
Ksiazczak, Α., A. Anderko: Properties of Polar Gases and Their D i mer Structures 1048
Kuball, H.-G, A. Strauss, M . Kap-pus, E. Fechter-Rink, A. Schön-hofer: The Orientation Axis. Comparison of Order Parameters of Anthraquinone Dyes in a Liquid Crystal Phase 1266
Kubitza, Ch., M. Schottler, Κ. Η. Homann: Scavenging of Radicals from the Gas Phase by Freezing with Dimethyl Disulfide. 2. Radicals from Discharges and a Flame of Acetylene 695
Kuczynski, W., siehe Η. Stegemeyer 3 Kuhn, Η., siehe Η. Schreiber . . . . . . 798 Kunimatsu, Κ., siehe Τ. Ohtsuka . . 313
Lamy, C, siehe J.-M. Leger 336 Lang, E. W., F. X. Prielmeier, H.
Radkowitsch, H.-D. Lüdemann: High Pressure NMR Study of the Molecular Dynamics of Liquid Methylfluoride and Deutero-Methylfluoride 1017
High Pressure NMR Study of the Molecular Dynamics of Liquid Fluoroform and Deutero-Fluoroform 1025
Langel, W., H. Kollhoff, E. Knözinger, M . Prager: Neutron Scattering and Dynamics of Small Molecules in Cryogenic Matrices . . . 1257
Latanowicz, L.: Dynamics of Proton Transfer in Solution by NMR Relaxation 237
Leaist, D. G : Bidirectional Coupled Diffusion of Glycine Driven by pH Gradients 1059
Lee, Bunding, Κ. Α., G. McLennan, J. G. Gordon: Surface-Enhanced Raman Scattering from Ethyle-nediaminetetraacetic Acid 305
Leeuwen, H. P. van, J. Lyklema: In-terfacial Electrodynamics of Interacting Colloidal Particles. Geometrical Aspects 288
Leger, J.-M., B. Beden, C. Lamy: The Adsorption of Carbon Monoxide on Platinum Single Crystals in Alkaline Medium 336
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Rate Coefficients in IR-Photo-chemistry: Simple Estimates of the Rate Constant from Molecular Parameters 565
Lyklema, J., siehe Η. P. van Leeuwen 288 Lytle, F. W.: X-ray Absorption Spec
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Manzurola, E., siehe A. Apelblat . . 1387 Mardolcar, U. V., C. A. Nieto de
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Markworth, Α., Ν. Weiden, ΑΙ. Weiss: Microcomputer Controlled 47U-Zeeman Split NQR Spectroscopy of 35C1 in Single Crystal p-Chloroanilinium Trich-loroacetate. Crystal Structure and Activation Energy for the Bleaching Out Process 1158
Martin, M.: Impurity Diffusion in a Chemical Potential Gradient (I): Theoretical Results 772
— S. Dorris: Impurity Diffusion in a Chemical Potential Gradient (II): Iron Tracer Diffusion in Cobalt Oxide in an Oxygen Potential Gradient 779
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H. Genscher: Physical and Electrochemical Aspects of Charge Transfer Reaction Inverse Photoemission Spectroscopy (CTRIPS): Photon Energy Enhancement for High Injection Currents 488
McLennan, G , siehe K. A. Bunding Lee 305
Mehring, M., siehe F. Hentsch . . . . 911 — P. Höfer, A. Grupp: Pulsed Elec
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Meisel, W., siehe L. König 116 Melzig, M., siehe S. Schneider 1222 — siehe S. Schneider 1225 Memming, R.: Charge Transfer K i
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Menzel, R., P. Witte: Photophysical Hole Burning on Dye Solutions in the Liquid Phase with ns-La-serpulses 1249
Merboldt, K . - D , W. Hänicke, J. Frahm: NMR Imaging of Restricted Diffusion 1124
Meyer, O., siehe L. Elfenthal 432 Miller, M., siehe Κ. Hilpert 200 — Κ. Hilpert: Analysis and Ther
mochemistry of the Equilibrium Vapour of the Nal —Snl2 and S c l 3 - S n l 2 Systems 642
Mindl, Α., siehe S. Schneider 1222 Möller, W., E. Mozzhukhin, H. G.
Wagner: High Temperature Reactions of C H 3 . 2. H-Abstraction from Alkanes 660
Moger, G , J. Paäl-Lukäcs, D. Gal: Studies on the Interaction of Anthraquinone Triplet and a-Phen-ylethyl Hydroperoxide in Benzene and Chlorobenzene 794
Mollay, B., siehe Ε. Μ. Buchberger 1209 Moro, J. R., siehe F. Decker 408 Mortensen, J., siehe J. Heinze 960 Motoo, S., N . Furuya: Effect of Ter
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Mozzhukhin, E., siehe W. Möller . . 660 Müller-Kirschbaum, Th., siehe L.
Belkoura 1036 Müller-Warmuth, W., siehe R. Con
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Nagamura, Τ , K. Matano, Τ Ogawa: Molecular Orientation and Photoelectric Properties of Alloxazine Monolayer Assemblies 759
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IX
— siehe Κ. Horiuchi 1351 Nakato, Υ., H. Tsubomura: Remark
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Nhu, N. Van, S. N. Bhat, F. Kohler: Calculation of Isothermal Compressibilities of Mixtures. The Example Acetone + Chloroform . . 525
Nickel, U., B. Klein, J. Hsin-min: K i netics and Mechanism of the Oxidation of N,N-Diethyl-p-pheny-lenediamine by 12-Tungstocobal-tate(III) 997
Niemann, W., siehe Η. Beuthien . . . 1296 — Β. S. Clausen, Η. Topsoe: EXAFS
Studies of Ammonia Catalysts at Synthesis Conditions 1292
— siehe A. Torkler 1300 Nitsch, W., W. Kremnitz, G.
Schweyer: Kinetische Untersuchungen zur Reversibilität der Makromoleküladsorption an der Grenzfläche Wasser/Luft 218
Nakanishi, M., siehe N . Yoshida . . 666
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Kunimatsu: IR Reflection and Raman Spectroscopies of the Anodic Oxide Films on Tungsten . 313
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— Determination of the Effective Charge Numbers of Colloidal Spheres by Electrophoretic Mobility Measurements 1064
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of the Isotrop-Nematic Phase Transition in Liquid Crystals. I . Nucleation Theory of Phase Transition 211
0ye, H. Α., siehe W. Brockner 561
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Photocurrent Spectroscopy of n-GaAs 381
Peschel, G., J. Keldenich: Electrical Double Layer Forces in Thin In-terlayers between Macroscopic Bodies of Different Materials when being Immersed in Electrolyte Solutions 285
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Pettinger, Β.: Quantum-Mechanical Model for Surface (Un-)-Enhanced Resonance Raman Scattering of Adsorbates at Metals. Common Effects in SERRS and SURRS 308
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Rosinberg, Μ. L., V. Russier, J. P. Badiali, Μ. E. Boudh'hir: Model-ization of the Electrical Double Layer: Structure of an Ion-Dipole Mixture Near a Wall 276
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Schmidt, M. , D. Ziessow: Nichtlineare, quantitative NMR-Spek-tralanalyse in der Reaktionskinetik m o
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Schneider, S., A. Mindl, G. Elfmger, M . Melzig: Photochromism of Spirooxazines. I . Investigation of the Primary Processes in the Ring-opening Reaction by Picosecond Time-resolved Absorption and Emission Spectroscopy 1222
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Schöne, G., W. Wiesbeck, Μ. Stoll, W. J. Lorenz: The Kinetics of the Polycry stalline Ag/Ag +-Electrode Studied by High-Frequency Impedance Spectroscopy 469
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Schindler: Kinetics of the Reaction of Atomic Fluorine with H 2S and Elementary Reactions of the HS Radical 66
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Scholz, Μ.: Laser Induced Thermal Diffusion 1054
Schottler, Μ., Κ. Η. Homann: Scavenging of Radicals from the Gas Phase by Freezing with Dimethyl Disulfide. 1. Test of the Method for Light Radicals 688
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Tanabe, S., sitehe T. Hoshi 1069 Tenne, R., Rl. Haak, R. Triboulet:
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Wagner, H. Gg., siehe Μ. Brei 30 — siehe W. Möller 660 — siehe J. Einbrecht 700 Wagner, L, H . Strehlow: On the
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Walz, L., siehe D. Zhang 1283 - siehe S. Wügand 1189
Wannemacher, G., siehe H. Bockhorn 819
Weaver, Μ. J.: Some Nontraditional Approaches for Examining Strong- and Weak-Overlap Electron-Transfer Processes at Electrodes 450
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anism of Electroless Copper Deposition 619
Wigand, S.. L. Walz, Ν. Weiden, ΑΙ. Weiss: *5C1 NQR Spectra and Crystal Structures of 1,2,4,5-Te-trachloro-3,6-dinitrobenzene and of 1,3,5-Trichloro-2,4-dinitroben-zene 1189
Wilkinson, D. P., siehe Β. Ε. Conway 484 Willand, C. S., D. J. Williams: Non
linear Optical Properties of Polymeric Materials 1304
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Winter, R., F. Hensel, T. Bodensteiner, W. Gläser: The Static Structure Factor of Cesium over the Whole Liquid Range up to the Critical Point 1327
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tions in Water-Acetamide Mixtures from Volume Data 519
Inhaltsverzeichnis von Band 91 (1987) — Autorenverzeichnis XI
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R. Schneider et al.: Ionisation and Dissociation of Diarylmethyl Chlorides in BC1 3/CH 2CI 2 Solution etc. 1369
Ionisation and Dissociation of Diarylmethyl Chlorides in BC1 3/CH 2C1 2
Solution: Spectroscopic Evidence for Carbenium Ion Pairs Reinhard Schneider, Herbert Mayr
Institut für Chemie, Medizinische Universität zu Lübeck, Ratzeburger Allee 160, D-2400 Lübeck 1, Federal Republic of Germany
Peter Η. Plesch
Chemistry Department, The University, Keele, North Staffordshire ST5 5BG, United Kingdom
Carbocations / Electrochemistry / Ionisation / Spectroscopy, Visible / Thermodynamics The ionisation equilibria of diarylmethyl chlorides Ar 2 CHCl (Ar = p - C H 3 0 - C 6 H 4 , p -PhO-C 6 H 4 , p - C H 3 - C 6 H 4 ) reacting with BC13 in CH 2C1 2 to give ion-pairs Ar 2 CH + BCLr (K{), and the dissociation of these (ΚΌ) were studied by conductimetry and spectro-photometry. The molar conductivities are almost independent of the nature of the aryl group («3 .5 · 10~3 Sm2/mol at —70°C). The ionisation constants K\ increase strongly with increasing electron releasing ability of the p-substituents. The standard ionisation enthalpies and entropies for (p-CH 3 -C 6 H 4 ) 2 CHCl and (p-PhO-QH 4 )(Ph)CHCl, calculated from the K\ at different temperatures are negative. The dissociation constants KD [(1.9 — 2.9) · 10~4 mol/L at — 70°C] do not show a systematic dependence on the electron donating abilities of the substituents in the aryl groups. Small differences between the UV-vis absorption spectra of unpaired and paired ions were used to confirm the
conductimetrically determined values of KD.
Introduction Diarylcarbenium ions have been studied extensively in
solvents of low nucleophilicity, mostly by N M R and U V spectroscopy [1] , and several species have been isolated as crystalline hexachloroantimonates from CC1 4 solution [2] . The ionisation equilibria of various diarylmethanols have been determined in sulfuric acid/water mixtures (Eq. (1)) [3] .
A r 2 C H + + H 2 0 A r 2 C H O H + H + . (1)
The KR+ values show a linear correlation with the rates of the solvolyses of the corresponding diarylmethyl chlorides [4] and the enthalpies of ionisation of diarylmethyl chlorides and alcohols in superacidic media [5] .
A r 2 C H + B C 1 4 - + H 2 C = C R R 7 ' ( 2 )
— A r 2 C H - C H 2 - C R ' R ' C l + BC1 3 .
In the context of kinetic studies on the addition of carbenium tetrachloroborates to alkenes (Eq. (2)) [6] , the Lübeck group required information on the ionisation and dissociation equilibria (3), the equilibrium constants of which are given by Eqs. (4) and (5).
1 - X . V 1*-X,V B C I " 1+-X .Y Covotent I o n - P a i r Free I o n s
l o n i s o t i o n D i s s o c i a t i o n
Ber. Bunsenges. Phys. Chem. 91, 1369-1374 (1987) - © VCH Verlagsgesellschaft mbH, D-6940 Weinheim, 1987. 0005-9021/87/1212-1369 $ 02.50/0
R. Schneider et al.: Ionisation and Dissociation of Diarylmethy) Chlorides in BCI3/CH2CI2 Solution etc.
[ A r 2 C H + B C l 4 ] 1 [ A r , C H C l ] [ B C l 3 ] 1 '
[ A r 2 C H + ] [ B O , - ] K d ~ [ A r 2 C H + B C l 4 - ] ' ( 5 )
The investigation involved conduetimetric and spectropho-tometric measurements, and the results were analysed by means of the theory of Binary Ionogenic Equilibria [7]. A new and unexpected finding is, that there are small but quite definite differences between the U V-vis spectra of paired and unpaired diarylmethyl cations, which can be used to confirm the conductimetrically derived value of ΚΌ.
Experimental
Dichloromethane was purified and dried as described by Heub-lein and Bauerfeind [8] . Boron trichloride (>99%) was commercially available and was used without further purification. Benzyl-triethylammonium chloride was dried for 24 h in high vacuum at 130C and stored under dry nitrogen. The diarylmethyl chlorides were prepared from diarylkctones, which were obtained by the Fric-del-Crafts reaction of suitably substituted benzoyl chlorides with benzene derivates according to a standard literature procedure [9] , The reduction of the ketones was carried out with Zn/KOH in ethanol, following the method of Davies [10a]. Subsequent treatment of the diarylmethanols with gaseous HCl in dichloromethane at 0 C in the presence of CaCl 2 yielded the diarylmethyl chlorides. After recrystallization or distillation colourless materials were obtained. 1-CH,.H: bp. 110-112 C77 Pa (160- 164 C/(8-9) · 102
Pa [10a]); 1-CH,,CH,: pentane, mp. 45 -46 C (45-46 C [10b]); l-OPh,H: ether, mp. 52 -53 .5°C; l - O C H 3 , H : pentane, mp. 6 1 - 6 2 ° C (62-63°C [10c]); l -OPh,CH 3 : ether, mp. 67-68 .5°C; l -OCH 3 ,CH 3 : pentane, mp. 4 3 - 4 4 ° C ; 1-OPh,OCH3: pentane, mp. 54 -56°C ; l -OCH 3 ,OCH 3 : ether, mp. 8 0 - 8 2 ° C ( 8 3 - 8 4 ° C [10d]).
The UV-vis-Spectra were taken with the K O N T R O N U V I K O N 860 spectrometer at ambient temperature. Photometric measurements were carried out with a fibre optic system (Schölly KGS III) . The light of a 30 W halogen lamp is conducted in a liquid fibre, which splits the light into a probe channel and a reference channel. The probe (Fig. 1) consists of two parallel quartz rods, inserted into twin quartz sleeves, which dip into the solution to be analysed. The light travels down one rod, is totally reflected at its lower end to pass through the solution 5 mm) and then returns by the second rod, whence a liquid fibre conducts it through an interference filter (Bandpass-Filter Corion) with a band width of 10 nm to the signal monitor.
rvv burette
Fig. 1 Diagram of the reaction vessel
Conduetimetric measurements were carried out with a Tacussel CD 810 conductimeter and Pt plate electrodes. The cell constants, determined with 0.01 Μ and 0.001 Μ KCl solutions, ranged from 53 to 85 m - 1 . Conductances below 10 μ8 were determined with
62.5 Hz AC, and for those between 10 and 50 μ5 an AC of 2:0 Hz was used.
All experiments were carried out in a dry nitrogen atmosphere. All the concentrations quoted are those at the actual openting temperatures, the adjustments having been calculated from thecoef-ficient of thermal expansion of dichloromethane, 0.00137 Κ 1 11].
Results and Discussion
Ionisation of Diarylmethyl Chlorides by BC13 in Dichloromethane
The reactions of diarylmethyl chlorides 1-X,Y with 3C13
yield ion-pairs 1 + - X , Y BCLf in equilibrium with the free ions 1 + - X , Y and B O T (Eqs. (3)-(5)). Consequently, the UV-vis absorbance and the conductivity will grow vhen BC1 3 is added progressively to solutions of 1-X,Y.
n l 0 4 K / s m _ 1
1 -0CH 3 , 0CH 3 1-CH 3 ,CH 3
1 5 10 15
Fig. 2 Conductance of 1.1 · 10 3 Μ diarylmethyl chloride solutions in the
presence of various amounts of BC13 (CH 2C1 2, — 70°C)
As shown in Fig. 2, the conductance increases rapidly, when l - O C H 3 , O C H 3 is titrated with BC1 3 and reaches a limiting value after the addition of 1 equivalent of B C l 3 . These findings indicate a large value of Κι and a dissociation equilibrium, which is independent of the concentration of BC1 3 , as required by theory (Eqs. (3) —(5)).
When l - O C H 3 , O P h , l - O C H 3 , C H 3 (not shown in Fig. 2) and l - O C H 3 , H are titrated, 1—3 equivalents of BC1 3 are sufficient to reach the plateau in the titration curves, i. e., Ky
is large for all of these systems. For l - O P h , H and 1 - C H 3 , C H 3 , 100-120 equivalents of BC1 3 are needed to achieve complete ionisation, and 1 - C H 3 , H is not completely ionised even with 200 equivalents of BC1 3 . Note that "200 equivalents of BC1 3" amounts to only » 2 vol% of BC1 3 , so that any effect on the macroscopic dielectric constant of the mixture is in fact negligible.
When the titrations were monitored photometrically, curves closely similar to those in Fig. 2 were obtained. Photometric studies over a range of temperatures showed, that l - O C H 3 , O C H 3 , l - O C H 3 , O P h and l - O C H 3 , C H 3 in the presence of excess BC1 3 remain fully ionised from —70 up to — 20°C, whereas for the less stabilised cations 1 + -O C H 3 , H , l + - O P h , H , and 1 + - C H 3 , C H 3 the formation of
R. Schneider et al.: Ionisation and Dissociation of Diarylmethyl Chlorides in BC1 3/CH 2C1 2 Solution etc. 1371
the molecules 1-X, Y becomes noticeable at the higher temperatures (Fig. 3).
As discussed below, 10 5 Μ solutions of diarylcarbenium tetrachloroborates contain less than 10% of ion-pairs, and therefore the absorbances shown in Fig. 3 are almost entirely due to unpaired ions. If deviations from Lambert-Beer's law, which are caused by the use of non-monochromatic light [12], are neglected, K' = Kx · KD for the dilute solutions of 1 - C H 3 , C H 3 , and l - O P h , H can be derived from Fig. 3. From a plot of In AT' vs. 1 /r the thermodynamic parameters AH0
and A S 0 for the equilibrium (6) were calculated (Table 1).
Κι — [ A r 2 C H + ] 2
[ B C l 3 ] ( c 0 - [ A r 2 C H + ])/(! + tf, [BC1 3])* (9)
As discussed by Grattan and Plesch [7 a] , the ionic conductivity A\ can be considered to be independent of the concentration in dilute solutions, so that A\ = AQ = κ/ [ A r 2 C H + ] . With this substitution, Eq. (9) can be rewritten to give:
Cp 1-f l / g , [ B C l 3 ] 1 ' K + A KDAr
(10)
A r 2 C H C l + BC1 3 ^ CH 2C1 2
A r 2 C H + + BC1 4~. (6)
Table 1 Standard-enthalpies and entropies for the ionogenic equilibrium (6) from pho
tometric studies at different temperatures
1-X, Y AH°/k) m o r 1 AS°/)K~* mol-'
1-OPh, Η -47.5 -260 1-CH3. C H 3 -46.4 -260
This equation is equivalent to E q . (C.2.14) of Ref. [7a], if [BC1 3 ] * [ B C 1 3 ] 0 .
For fully ionised systems, in which / ^ [ Β 0 3 ] > 1, Eq. (10) is reduced to (11).
κ 1
KDA? κ +
_1_
A' (ID
Eqs. (10) and (11) can be used to derive the equilibrium constants and the molar conductivities as described [7].
1.00
0.50
0.10-
AIT) A(-70°C)
1 + - 0CH 3 ,H
[ 1 + - C H , , C H , ] » 1.1 · 1 0 " * mol/L / [ B C I , ] - 9 . 0 - 1 0 " 2 mol/L
[ 1 + - O P h f H ] - 1 . 1 · 1 ( Γ 5 mol/L / [ B C I , ] - 9 . 0 - 1 0 - 2 mol/L
[ 1 + - O C H , , H ] - 2 .2-10-" mol/L / [ B C I , ] = 2 . 2 - Κ Γ 2 mol/L
T/°C — ι ι 1 1 1 — - 8 0 - 7 0 - 6 0 - 5 0 -AO
—ι— - 3 0 - 2 0 - 1 0
Fig. 3 Temperature dependence of the UV-vis-absorbance of diarylcar
benium tetrachloroborate solutions in dichloromethane (A = 490 nm)
Quantitative Analysis of the Conductivity Results [7] If the system is described by E q . (3), the total concentra
tion (c0) of diarylmethyl species is
c 0 = [ A r 2 C H C l ] + [ A r 2 C H + B C L r ] + [ A r 2 C H + ] .
Substitute [ A r 2 C H + B C l 4 ~ ] from (4) into (7):
c 0 - [ A r 2 C H + ] [ A r 2 C H C l ] = •
l + j ^ C B c y
(7)
(8)
The product ΚχΚΌ is formed from Eqs. (4) and (5), [ A r 2 C H C l ] substituted from (8), and [ B C l f ] set equal to [ A r 2 C H + ] (electroneutrality); we thus obtain E q . (9):
^2./root S-W 2
•300
c=1.0 ·10' 4 mol/L I
c= 5.0-10"5 mol/L \
c = 5.0-10 mol/L
•200
5.0.· 10"U 10;10'*
Fig. 4 Evaluation of Ax and KD for l + - O C H 3 , O C H 3 in dichloromethane
at - 3 0 ° C
In a first series of experiments, diarylmethyl chlorides 1-X, Y were added gradually to solutions of BC1 3 in C H 2 C 1 2
while the conductance was determined. The concentration of BC1 3 and the temperature were selected so that ionisation was complete. A plot according to Eq . (11) (Fig. 4) was linear for c 0 < 5 10~ 4 mol /L, and its intercept yields 1/Ar With this value, the dissociation constant ΚΌ can be derived from the slope.
The dissociation constants thus obtained are of the same order as the ΚΌ values of other types of carbenium salts in C H 2 C 1 2 previously reported (Table 2). As expected, variations of the substituents have little effect on the molar conductivities. The temperature dependence of ΚΌ indicates negative dissociation enthalpies and entropies. The positive A G 0 value of the ion-pair dissociation is thus due to the unfavourable dissociation entropy. The paucity of data obtained at different temperatures inhibits a detailed discussion. It seems, however, that for the less stabilised carbenium
1372 R. Schneider et al.: Ionisation and Dissociation of Diarylmethyl Chlorides in BCI3/CH2G2 Solution etc.
Table 2 Molar conductivities, ion-pair dissociation constants and thermodynamic parameters for the dissociation of carbenium ion salts in dichloromethate
Saltb> T/"C No of Expts.
At • 10V S m 2 m o l ~ , a )
104 Kol mol L " 1 a >
AH0/ kJ mol 1
AS0/ J K " 1 mor ' Lit.
Ρ - O C H 3 , O C H 3 B C l 4 - 7 0 6 3.50 ± 0 . 1 4 2.2 ± 0.2 -2.3 -81 - 6 0 1 4.23 2.1 - 5 0 2 5.33 ± 0.03 1.9 ± 0.3 - 4 0 2 6.17 ± 0.08 1.8 ± 0.0 - 3 0 6 7.15 ± 0.09 1.8 ± 0.2 - 2 0 1 8.42 1.6
l + - O C H 3 , O P h B C l 4 - - 70 2 3.15 ± 0.06 2.1 ± 0.4
l + - O C H 3 , C H 3 B C l 4 - 7 0 9 3.49 ± 0 . 1 4 2.4 ± 0.3 -3.8 -88 c
- 6 0 1 4.34 2.3 -50 2 5.21 ± 0.20 2.0 ± 0.1 - 3 0 2 7.18 ± 0.08 1.7 ± 0.1
l + - O P h , C H 3 B C L T - 7 0 3 2.99 ± 0 . 1 7 2.9 ± 0.5 CI
l + - O C H 3 , H B C L r - 8 0 5 2.45 ± 0.05 2.7 ± 0.2 -7.0 -105 ci
-70 15 3.37 ± 0.12 1.9 ± 0.2 - 6 5 2 3.95 ± 0.05 1.8 ± 0.1 - 6 0 3 4.29 ± 0 . 1 3 1.7 ± 0.1 - 5 0 4 5.28 ± 0 . 1 7 1.4 ± 0.2 - 4 0 3 6.09 ± 0.09 1.3 ± 0.1 - 3 0 4 7.03 ± 0.06 1.0 ± 0.1
l " - O P h , H B C l 4 - - 7 0 7 3.16 ± 0.14 2.0 ± 0.3 0
r - C H 3 , C H 3 B C 1 4 -70 3 3.31 ± 0.25 1.9 ± 0.1
T r ' SbCl 6 - 4 5 6.17 0.73 -10.5 -126 [13a] P y r SbCV -45 5.95 0.88 -13.0 -138 [13a] Et 4 N + SbCl6- - 4 5 5.53 1.2 -6.3 -100 [13a] P h 3 C + S b C l 6 - - 4 5 4.13 2.9 -3.3 -71 [13b]
- 4 5 4.43 5.3 -8.4 -96 [13a] 0 8.21 3.1
25 10.8 1.9
P h 3 C + S b F 6 " 0 9.71 2.4 -9.2 -105 [13c] P h 3 C + A s F r 0 9.69 1.9 -9.2 -105 [13c] Ph 3 C + C l - 0 - - « 0 -152 [8]
With standard deviations. Tr = Tropylium; Pyr = 2,4,6-Trimethylpyrylium; Et = Ethyl; Ph = Phenyl. This work, derived from Eq. [11].
Table 3 Molar conductivities and ionisation constants for solutions of diarylmethyl chlorides and BC13 in CH 2 C1 2 at — 70°C derived from conductivity measure
ments on partially ionised systems
1-X, Y No of Expts.
A, · ΙΟ3/ S m 2 mol"1 a ) L mol- 1 a )
AG?(70°C) kJ mol-'
1-OPh, Η 2 2.97 ± 0.08 145 ± 7 -8.4 1-CH 3, C H 3 3 3.64 ± 0.99 64 ± 10 -7.0
I - C H 3 , H b ) 3 1.94 ± 0.43 0.49 ± 0.05 + 1.2 (0.17) ( + 3.0)
a ) With standard deviations. b ) Calculated for KD = 2.0· 10~4 mol/L; values in parentheses calculated for
Ai = 3.20· Ι Ο - 3 Sm2/mol (see text).
ions both AH° and AS0 are more negative, which indicates that in these systems the solvation of the free ions is more important.
In a second series of experiments, diarylmethyl chlorides 1-X,Y were added gradually to solutions of BC1 3 under conditions of incomplete ionisation. Large concentrations of
B C I 3 were again used, and the changes of [BC1 3 ] during the titrations were negligible. Again, linear plots of CQ/K V S . Κ were obtained (Eq. (10)), but the intercepts (ί/Λ{) observed in different experiments varied considerably, which diminished the accuracy of the A{ values. However, the A{ values of l + - O P h , H and 1 + - C H 3 , C H 3 (Table 3) agree well with those in Table 2. Since Table 2 showed Ax to be almost independent of the nature of the para-substituents, we consider the low Ax value found for 1 + - C H 3 , H to be an artefact of unexplained origin.
The K\ values can be calculated from the slopes of the plots, [BC1 3 ] , A-, and ΚΌ (Eq. (10)). These values together with the KD in Table 2 give K' = ΚνΚΌ for l - O P h , H + BC1 3 (0.029) and 1 - C H 3 , C H 3 + BC1 3 (0.0122), corresponding to A G 0 ( - 7 0 ° C ) of 6.0 and 7.4 kJ mol" 1 , respectively. These numbers are closely similar to those derived from the temperature dependence of absorbance (5.3 and 6.4 kJ m o l - 1 , Table 1).
Furthermore, the difference between the AG? values of the lower two compounds of Table 3 (8 —10 kJ/mol) agrees
R. Schneider et al.: Ionisation and Dissociation of Diarylmethyl Chlorides in BCI3/CH7CI2 Solution etc. 1373
well with the corresponding value (7-11 kJ/mol) derived from the pKR, values of 1 - C H 3 , C H 3 (pKR+ = -10.4 [3b]) and 1 -CH 3 ,H ( p £ R , = -12.3 [3c]; -11.6 [3d]) at 25°C.
Spectroscopic Evidence for Ion-Pair ±? Free Ions Equilibria
It has long been known that the UV-vis absorption spectra of carbocations are influenced only slightly by the solvent and the state of the ions [14]. Consequently, many analyses of ionogenic equilibria have been based on the identity of the absorption spectra of unpaired and paired ions [15]. The differences in the absorption spectra shown in Fig. 5 enable us to progress beyond these conventional approximations and to extract information on ion-pair dissociation from absorbance measurements.
The absorption spectrum A (Fig. 5) can be attributed to unpaired 1 + - O C H 3 , O C H 3 ions, since at a concentration of 10~ 5 M, the degree of dissociation exceeds 90% (from ΚΌ
in Table 2). The same solution, but containing also 10~ 2 Μ benzyltriethylammonium tetrachloroborate gave spectrum B, which showed a 2 nm blue shift of A m a x and a decrease of f-max (Fig. 5). Similar changes have been observed for the absorption spectrum of l + - O C H 3 , C H 3 .
This effect may be attributed a priori either to the formation of ion-pairs or to a more general solvatochromic
550 λ/nm
Fig. 5 Absorption spectrum of 1 + - O C H 3 , O C H 3 (1.0* 10~5 M) in CH 2C1 2
at 20°C (curve A) in presence of benzyltriethylammonium tetrachloroborate (1.0· 10" 2 M) (curve B)
1.00
0.50-
0.10
curve II
curve I
1.00 5.00 10.00
Quantity of BClf/mmol
Fig. 6 Titration of 1 + -OCH 3 ,OCH 3 BClf (2.0· 10" 5 mmol) and BC13 (10 mmol) in 92 mL of CH 2C1 2 with benzyltriethylammonium chloride at — 70°C. Upper curve: 485 — 495 nm, lower curve: 515 — 525 nm
effect caused by the change of the medium. Since all spectra were taken in the presence of a large excess of BC1 3 , the differences are unlikely to arise from nucleophilic impurities.
In order to assign these spectral effects, solutions of 1 + -X , Y BC14~ with excess of BC1 3 were titrated with benzyltriethylammonium chloride. When the ammonium chloride is added, the BC1 3 accepts C l ~ ions so that [ B C L f ] increases at the expense of [B C 1 3 ] . According to Eqs. (4) and (5), these concentration changes reduce the degree of ionisation of 1-X,Y and the degree of dissociation of the 1 + - X , Y B C L f ion pairs.
0.50-
0.10-
100 5.00 10.00 Quantity of BCl^/mmol
Fig. 7 Titration of 1 +-OCH 3 ,CH 3 BC14" (2.0· 10~5 mmol, Xm&x = 488 nm in CH2C12) and BC13 (10 mmol) in 92 mL of CH 2C1 2 with benzyltriethylammonium chloride at — 70°C. Upper curve: 465 — 475 nm;
lower curve: 505 — 515 nm
Fig. 6 shows the change of the absorbance during the titration of 1 + - O C H 3 , O C H 3 / B C l 3 with C I " in two different spectral regions. If the titration is monitored in the 515 — 525 nm range (Fig. 5, area I) one observes an initial 8% decrease in absorbance, then a wide range in which the absorbance remains constant, and finally an abrupt decrease (Fig. 6, curve I). A similar behaviour was observed when the absorbance was measured at 485 — 495 nm (Fig. 5, area II ) ; the only difference is that now an increase in absorbance was observed during the first phase of the titration (Fig. 6, curve II) . Similar titration curves were obtained with 1 + -O C H 3 , C H 3 (Fig. 7).
With all systems, an abrupt decrease of the absorbance occurs when the BC1 3 is used up and the chloride ions are then trapped by the 1 + - X , Y . This finding supports the previous conclusion that the diarylmethyl chlorides with X = O C H 3 and Y = O C H 3 or C H 3 are completely ionised by one equivalent of BC1 3 , i.e. Κλ is relatively great.
It remains to find the reason for the changes of absorbance in the initial phase of the titration. If they were due to a change of the medium, i.e. a general solvatochromic effect, one would not expect the absorbance to remain constant while 90 — 95% of the ammonium chloride is added. However, the noticeable change in the absorbance at the beginning and the long plateau while most of the C l ~ is added,
1374 R. Schneider et al.: Ionisation and Dissociation of Diarylmethyl Chlorides in BCI 3/CH 2C1 2 Solution etc.
are readily compatible with our explanation in terms of ion-pairs.
A Ao
1.05
1.00< ο experimental
<3 calculated
0.10 0.50 1.00 Quantity of BCI 4 /mmol
Fig. 8 Upper part: Spread out section of Fig. 6 and calculated changes of
absorbance (see text). Lower part: percentage of free ions
Fig. 8 shows an enlargement of the left part of Fig. 6 and the percentage of unpaired ions calculated by means of KD
[16]. It is obvious that the changes of absorption take place in the same range in which the percentage of unpaired ions decreases from » 9 0 % to less than 13%. From the absorbance observed before C l ~ was added (92% free ions and 8% ion-pairs) and the absorbance at the plateau (5% free ions and 95% ion-pairs), we can calculate the absorbance at different stages of the titration and, as Fig. 8 shows, the experimental and the calculated curves superimpose. The participation of 1:1 ion-pairs in binary ionogenic equilibria has thus been supported by an independent method.
We thank Ute Grabis for experimental assistance, the Deutsche Forschungsgemeinschaft for financial support, and the British Council for supporting the cooperation between Lübeck and Keele.
References
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[16] For the calculation of the percentage of free ions we assumed KD of 1 + BC14~ and R 4 N + B C L r to be equal (see Table 2 and corresponding discussion).
(Eingegangen am 4. Mai 1987, Ε 6485 endgültige Fassung am 21. Juli 1987)