X-Ray Structural Analysis of NiII, PdII, and PtII Complexes with the Potentially Tridentate Ligand 1,3-Bis(diphenylphosphinomethyl)benzene, 1,3-C6H4(CH2PPh2)2

The ligand 1,3-bis(diphenylphosphinomethyl)benzene, 1,3-C₆H₄(CH₂PPh₂)₂ undergoes cyclometalation reactions, thus forming derivatives containing the tridentate moiety 2,6-bis(diphenylphosphinomethyl)phenyl,2,6-C₆H₃(CH₂PPh₂)₂. Complexes of the type trans-[MBr(C₆H₃CH₂PPh_{2 2})] with M = Ni^II, Pd^II, and Pt^II could be obtained and their crystal structures were here determined by X-ray diffraction (XRD) methods. The Ni complex belongs to the space group P2 ₁/c with a = 10.257(2), b = 16.234(5), c = 17.475(4) Å, = 109.34(2), and Z = 4. The Pd complex belongs to the space group P2 ₁/n with a = 10.325(3), b = 16.279(4), c = 17.303(4) Å = 105.34(3), and Z = 4. The Pt complex belongs to the space group P2 ₁/n with a = 10.127(2), b = 14.776(2), c = 19.023(3) Å, = 91.01(1), and Z = 4. Different distortions are induced by the rigid tridentate ligand on the square planar coordinations of the three metals. A significant difference between the two M-P bond distances is present in the Pt complex and can also be found in an analogous Pd complex.     

Structure électronique de l'o-benzoquinone (méthode L.C.A.O. améliorée)

Résumé La théorie L. C. A. O. améliorée est appliquée à l'étude de la structure électronique de l'o-benzoquinone. Les indices de liaison obtenus conduisent aux distances interatomiques suivantes: 1,23 Å pour les groupements carbonyles, 1,46 Å pour les liaisons «simples», 1,35 Å pour les liaisons «doubles». Les résultats obtenus pour l'énergie des transitions N V et N A et pour le moment dipolaire sont en bon accord avec l'expérience.

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The improved LCAO theory is applied to o-benzoquinone. The mobile bond orders give the following bond distances: 1,23 Å for the C=O bonds, 1,35 Å for the double bonds, 1,46 Å for the single bonds. The results we got for the N V and N A transition energies, and for the dipole moment are in good agreement with the experiment.

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Zusammenfassung Die elektronische Struktur der o-Benzochinon-Molekel wird mit Hilfe der verbesserten LCAO-Methode untersucht. Die berechneten Bindungsindices geben die folgenden interatomaren Abstände: 1,23 Å für die C=O-Bindungen, 1,46 Å für die Einfachbindungen, 1,35 Å für die Doppelbindungen. Die Werte für die N V- und N A-Übergänge und für das Dipolmoment stimmen gut mit der Erfahrung überein.

     

The electronic spectrum of acrylonitrile

The vapor absorption spectrum of acrylonitrile CH₂CHCN has been measured in the vacuum ultraviolet region. In addition, an all-valence-electron molecular orbital calculation has been used to calculate the electronic structure and spectrum of the molecule. On the basis of the MO calculation, as well as a vibrational analysis of the observed spectrum, several electronic transitions are assigned. The lowest energy absorption band (2107Å, = 150) is assigned as an n ^* transition. Absorption bands at 2030Å (=1600), 1725Å ( = 2100), and 1570Å ( = 1920) are assigned as 0–0 bands associated with transitions that are, respectively, ^*,^*, and ^* in character.

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Zusammenfassung Das UV-Absorptionsspektrum von dampfförmigen Acrylnitril wurde gemessen und eine CNDO/2-Rechnung für die Elektronenstruktur durchgeführt. Auf dieser Basis konnten unter Zuhilfenahme der Analyse der Schwingungsstruktur im beobachteten Spektrum mehrere Banden zugeordnet werden: die 2107-Å-Bande ( = 150) einem n^*-Übergang, die drei Banden bei 2030Å ( = 1600), 1725Å ( = 2100) und 1570 Å ( = 1920)0-0-Übergängen von ^*-, ^*- bzw. ^*-Banden.

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Résumé Mesure du spectre d'absorption en phase vapeur de l'acrilonitrile CH₂CHCN dans la région de l'ultraviolet. Par ailleurs, la structure électronique et le spectre de la molécule ont été calculés à l'aide d'une méthode des orbitales moléculaires semi-empirique pour tous les électrons de valence. Sur cette base, ainsi que sur une analyse vibrationnelle du spectre expérimental, on procède à l'attribution de plusieurs transitions électroniques. La bande d'absorption de plus basse énergie (2107 Å, = 150) est attribuée à une transition n ^*. Les bandes d'absorption à 2030Å ( = 1600), 1275Å ( = 2100) et 1570Å ( = 1920) sont considérées comme des bandes 0 - 0 associées à des transitions ^*, ^* et ^* respectivement.

     

Thermal behaviour of transition metal complexes of dithiocarbazic esters. II

A thermal study (simultaneous TG and DTA measurements) was carried out on the dithiocarbazic ester complexes M[N³CH₂R₁N²C¹(S)SCH₃]₂, where M=Ni, Pt; R₁=C₆H₅. The following disproportionation reaction occurs in the solid state: II is formed through deprotonation of the CH₂ group bound to N³, whereas III is formed through protonation of N³.The influence of inductive and/or steric effects on the mechanism of this reaction is discussed, taking into account the electrochemical and X-ray data on the complexes Pt[NRNC(S)SR']₂ with differentR substituents: R=H, Ph, CH₂Ph, CH₂C₅H₁₁, CH(CH₃)₂, C(CH₃)₃; R=CH₃, CH₂Ph.These results accord with the behaviour of the same complexes in solution.

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Zusammenfassung Dithiokarbamidsäureesterkomplexe M[N³CH₂R₁N²C¹(S)SCH₃]₂ mit M=Ni, Pt und R₁=C₆H₅ wurden thermisch untersucht. Im festen Zustand spielt sich folgende Disproportionierungsreaktion ab: II wird durch Deprotonierung der an N³ gebundenen CH₂ Gruppe und III durch Protonierung des Atoms N² gebildet. Unter Zuhilfenahme der elektrochemischen und Röntgendaten der Komplexe Pt[NRNC(S)SR']₂ mit verschiedenen Substituenten R: R=H, Ph, CH₂Ph, CH₂C₅H₁₁, CH(CH₃)₂, C(CH₃)₃ und R=CH₃ bzw. CH₂Ph wurde der Einfluß von induktiven und/or sterischen Effekten auf den Reaktionsmechanismus diskutiert. Diese Ergebnisse stehen in Übereinstimmung mit dem Verhalten der Komplexe in Lösung.

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M[N³CH₂R₁N²C¹(S)SCH₃]₂, M= Ni, Pt,R ₁=C₆H₅. : II CH₂ , N³, III N². () , Pt[NRNC(S)SR]₂, R= , aR= . .

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We thank prof. A. La Ginestra for many helpful discussions on the various aspects of this work.     

The crystal structures of α, ω-diaminoalkanecadmium(II) tetracyanonickelate(II)-Aromatic molecule inclusion compounds. V. Toluidine clathrates of the hosts built of the diamines, 1,4-diaminobutane, 1.5-diaminonentane,and 1,8-diaminooctane

The crystal structures have been analyzed for the threeo-toluidine clathrates,catena-[catena--(1,4-diaminobutane)cadmium(II) tetra--cyanonickelate(II)]-o-toluidine(2/3),4-o,catena-[catena--(1,5-diaminopentane)cadmium(II) tetra--cyanonickelate(II)]-o-toluidine(3/4),5-o, andcatena-[catena--(1,8-diaminooctane)cadium(II) tetra--cyanonickelate(II)]-o-toluidine(1/1),8-o, for am-toluidine onecatena-[catena--(1,5-diaminopentane)cadmium(II) tetra--cyano-nickelate(II)]-m-toluidine(1/1),5-m, and for ap-toluidine onecatena-[catena--(1,8-diaminooctane)cadium(II) tetra--cyanonickelate(II)]-p-toluidine(1/1),8-p. 4-o crystallizes in the triclinic space groupP,a/Å = 9.806(3),b/Å = 14.388(3),c/Å = 7.725(2), /° = 89.71(2), /° = 89.96(2), /° = 98.12(2),V/ų = 1078.8(5),Z = 2, 3750 reflections,R = 0.056;5-o: tetragonalP4lmmm, (a = b)/Å = 7.485(7),c/Å = 10.06(3),V/ų = 563(2),Z = 1, 573 reflections,R = 0.19;8-o: monoclinicP2/m,a/Å = 11.513(4),b/Å = 7.626(1),c/Å = 7.101(1), /° = 109.63(3),V/ų = 587.2(2),Z = 1, 1682 reflections,R = 0.058;5-m: orthorhombicPbam,a/Å = 12.254(6),b/Å = 20.62(1),c/Å = 7.804(1),V/ų = 1972(1),Z = 4, 2240 reflections,R = 0.059; and8-p: triclinic,P,a/Å = 11.52(1),b/Å = 7.632(3),c/Å = 7.039(4), /° = 88.93(4), /° = 109.71(5), /° = 82.81(9),V/ų = 576.9(6),Z = 1, 2598 reflections,R = 0.042. Their structures are substantially similar to the already-known structure ofcatena-[catena--(1,6-diaminohexane)cadmium(II) tetra--cyanonickelate(II)]-o-toluidine(1/1): the guest toluidine molecules are accommodated in the cavities formed betweencatena-[cadmium(II) tetra--cyanonickelate(II)] layers bridged by the ambidentate ,-diaminoalkane ligands at the cadmium(II) atoms. The carbon chain length of the ,-diaminoalkane influences the number of cavities per formula unit and the deformation of the metal complex layers.     

Röntgenuntersuchungen zur Kristallstruktur von Polybutylenterephthalat (PBT)

Zusammenfassung Polybutylenterephthalat (PBT) gewinnt als Spritzgußmaterial und als Faserrohstoff zunehmend an Bedeutung. Die thermischen und mechanischen Eigenschaften des PBT sind von denen des Polyäthylenterephthalates (PET) erheblich abweichend. Die vorliegende Arbeit soll einen Beitrag liefern, die abweichenden Ergebnisse deuten zu können.Deswegen wurden die Gitterzelle und die Kettenanordnung im Kristallverband des PBT untersucht. Aus Röntgenmessungen ergaben sich die folgenden Gitterzellenparameter:a=4,83 Å,b=6,05 Å,c=11,45 Å,=100,5°,=117°,=110,8°.Damit ergibt sich eine Kristalldichte von=1,433 g/cm³ im Vergleich zu=1,515 g/cm³ beim PET.Mit der Annahme einer abgewinkelten Kettenkonformation kann in befriedigender Weise die verkürzte Faseridentitätsperiode und die gegenüber dem PET verlängerte Zellenkante a des PBT erklärt werden.

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Summary Polybutylenterephthalate (PBT) is a new molding and fibre spinning material for industrial applications. The thermal and mechanical properties of PBT are quite different from those of polyethyleneterephthalate (PET).The unit cell of PBT was found by X-ray diffraction studies to be triclinic, similar to that of PET, but having the parameters:a=4.83 A,b=6.05 Å,c=11.45 Å,a=100.5°=117°,=110.8°. This gives a crystalline density of=1,433 g/cm³ compared with=1.515 g/cm³ for PET.Since a completely extended PBT chain would theoretical have a repeat length of 13.25 Å the above unit cell requires a kinked chain conformation. The increaseda axis dimension, in comparison to PET would be in agreement with this conclusion.

     

Antimony(III) Oxofluorides α-Sb3O2F5 and β-Sb3O2F5: Synthesis and Crystal Structures

The conditions for the synthesis of two polymorphous forms of antimony(III) oxofluoride Sb₃O₂F₅ from aqueous solutions are established. The crystal structure of a new polymorphous modification -Sb₃O₂F₅ is determined (monoclinic crystals with a = 6.9548(6) Å, b = 9.1043(7) Å, c = 20.336(2) Å, = 94.167(2)°, V = 1284.2(2) ų, Z = 8, (calcd) = 5.092 g/cm³, F(000) = 1712, space group P2₁/n) and the structure of -Sb₃O₂F₅ is refined. The geometric characteristics of crystal structures of antimony(III) oxofluorides SbOF (L- and -forms) are compared with those of Sb₃O₂F₅ (- and -forms).     

Reduction of NO by carbon monoxide on tin dioxide

The reduction of NO by carbon monoxide on SnO₂ has been studied in the temperature range from 90 to 450°C. The complicated temperature dependence of the reaction rate is due to the interaction of CO an CO₂ with the catalyst.

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NO SnO₂ 90–450°C. , CO CO₂ .

     

“Blue silver”: transformation of clusters and metal coagulation

The formation and transformations of blue silver ( _max 700 nm) during -irradiation of a weakly alkaline (pH 9) aqueous solution containing AgClO₄, polyacrylic acid (PAA), and isopropanol were studied. We believe that blue silver is a linear silver cluster stabilized on a polymeric molecule. During radiation-chemical reduction the cluster is transformed into new clusters ( _max = 365 and 460 nm). When all of the Ag⁺ ions present in the solution have been reduced, clusters coalesce and a new phase,i.e., colloidal silver particles, forms. The mechanism of the radiation-chemical transformations is discussed.Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 1, pp. 35–37, January, 1995.     

V2O5/TiO2 oxidation catalysts, III. Oxidation of CO on pure and sodium-doped systems

The activity of vanadia/titania catalysts in CO oxidation has been tested and found to be of the same order as that observed for unsupported vanadia; the simultaneous presence of vanadium-sodium compounds cancels the activity, probably because of the elimination of labile V=0 species at surface defects.

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V₂O₅/TiO₂ CO, V₂O₅; - , , V=0 .

     

Spectra and structure of small ring compounds. Part L VIII: Structural parameters for chlorocyclobutane from combined microwave data and ab initio calculations

The structural parameters of chlorocyclobutane,c-C₄H₇Cl, have been obtained fromab initio Hartree-Fock calculations employing the 6–31G^* basis set for both the more stable equatorial and the high energy axial conformers. The determined carbonhydrogen distances were adjusted by 0.010 Å and held fixed while a weighted least-squares adjust was used to obtain all of the heavy atom parameters for the equatorial conformer by fitting the rotational constants of nine isotopic species. The determinedr ₀ parameters are:r(C - C) = 1.535(8) År(C - C) = 1.548(3) År(C - Cl) = 1.788(9) Å CCC, - CL = 132.0(2)°; CCC, = 89.7(6)°; CCC, = 87.1(2)°, and CCC, = 88.7(2)°. These results are compared to the calculated values as well as those obtained earlier from electron diffraction and microwave studies.For Part LVII, seeJ. Raman Spectrosc.,1990,21, 591.Taken in part from the thesis of M. J. Lee which will be submitted to the Department of Chemistry in partial fulfillment of the Ph.D. degree.     

Upper bounds to atomic electron densities in position and momentum spaces

Modified functions r ^–(r) and p ^–(p) of the spherically averaged electron densities (r) in position space and (p) in momentum space are found to be convex (i.e., the second derivatives are nonnegative everywhere) for all the 103 ground-state atoms from hydrogen (atomic number Z=1) to lawrencium (Z=103), if the parameters are chosen to be 0.6 and 1.4. The convex property of r ^–(r) and p ^–(p) is used to derive upper bounds to the density functions (r) and (p) in terms of their radial moments r ^s and p ^s or frequency moments ^t and ^t . In most cases, the present bounds are shown to be more general and more accurate than those reported in the literature.     

Kinetic parameters of the thermal decompositions of nitritonickelates(II)

Kinetic parameters of thermal decomposition of compounds of general formulaM ₂ ^I M ^II[Ni(NO₂)₆], whereM ^I= K⁺, Rb⁺ or Cs⁺ andM ^II= Ca²⁺, Sr²⁺ or Ba²⁺, were investigated on the basis of the respective thermal curves. Calculations of the reaction order and activation energy carried out by the Coats-Redfern method and by Doyle's method (modified by Zsakó) gave similar results, The reaction order is 2 for all the compounds investigated. In the group of potassium salts the activation energy increases fromM ^II=Ca²⁺ toM ^II=Ba²⁺. In the groups of rubidium and caesium salts, the lowest activation energy is observed whenM ^II=Sr²⁺. Such behaviour of the nitritonickelates is explained in terms of structures and the principle of maximum density.

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Zusammenfassung Die kinetischen Parameter der thermischen Zersetzung von Verbindungen der allgemeinen FormelM ₂ ^I M ^II [Ni(NO₂)₆] (M ^I= K⁺, Rb⁺ oder Cs⁺ und M^II = =Ca²⁺, Sr²⁺ oder Ba²⁺) wurden auf Grund der entsprechenden thermischen Kurven untersucht. Die an Hand der Coats-Redfern Methode und der durch Zsakó modifizierten Doyleschen Methode durchgeführten Berechnungen der Reaktionsordnung und der Aktivierungsenergie ergaben ähnliche Resultate. Die Reaktionsordnung ist 2 für sämtliche untersuchten Verbindungen. In der Gruppe der Kaliumsalze steigt die Aktivierungsenergie vonM ^II=Ca²⁺ in RichtungM ^II=Ba²⁺ an. In der Gruppe der Rubidium- und Caesiumsalze wird die niedrigste Aktivierungsenergie beiM ^II=Sr²⁺ beobachtet. Dieses Verhalten der Nitritonickelate wird durch die Strukturen und das Prinzip der maximalen Dichte erklärt.

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₁ ^{2 II}[Ni(NO₂)₆], ^I= ⁺, Rb⁺Cs⁺,a ^II= ²⁺,8r²⁺²⁺. , - ( ), . 2. ^{+ 2+}. ^II=S²⁺. .

     

Mixed suspensions of semiconductors forming microheterojunctions. A new type of highly efficient photocatalysts: Photocatalytic production of dihydrogen from a water solution of sulfide ions in the presence of platinized ZnyCd1-y/CuxS suspension

A new method is proposed for increasing the quantum efficiency of H₂ production for the photocatalysts based on semiconductor suspensions. The method consists of the formation of suspended particles with microheterojunctions between their components--semiconductor phase.

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H₂ .

     

The kinetic energy components of LCAO-molecular orbitals: A comment on the “Electron-in-a-Box”-“LCAO-MO-Model” analogy

In many textbooks attention is drawn to the close analogy that seems to exist between the Electron-in-a-Box-wave functions _n and their LCAO-MO counterparts _J (J = n) for the movement of an electron in a -system. It is often implied that the wave lengths of _n and of _J (J = n) which satisfy to a high degree the relation =, have the same physical meaning. It is shown that this is not the case. for a linear system (e.g. a one-dimensional Electron-in-a-Box-model) is directly connected with the momentum of the electron and therefore with its kinetic energy according to the deBroglie relation. However, there is no such simple relationship between A and the corresponding kinetic energy component in LCAO-MO's _J . (The necessary two-center kinetic energy integrals have been computed for 1s-type atomic orbitals.)

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Zusammenfassung In vielen elementaren Textbüchern wird die Aufmerksamkeit auf die scheinbar enge Verwandtschaft hingelenkt, die zwischen den Wellenfunktionen _n für ein Electron-in-a-Box-Modell und den entsprechenden LCAO-MOs _J (J=n) für die Bewegung eines Elektrons in einem -System besteht. Unter anderem wird oft implizit angenommen, daß die Wellenlängen der Funktion _n und von _J (J=n), die weitgehend der Bedingung = genügen, die gleiche physikalische Bedeutung haben. In dieser Arbeit wird gezeigt, daß dies nicht der Fall ist. Für ein lineares System (z. B. ein eindimensionales Electron-in-a-Box-Modell) ist über die deBroglie'sche Beziehung direkt mit dem Impuls und damit mit der kinetischen Energie des Elektrons verknüpft. Im Gegensatz dazu existiert keine einfache Beziehung zwischen und der entsprechenden Komponenten der kinetischen Energie in einem LCAO-MO _J . (Die notwendigen Zweizentrenintegrale der kinetischen Energie wurden für Atomorbitale vom 1s-Typus berechnet.)

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Résumé Dans les textes élémentaires de chimie théorique on attire souvent l'attention sur l'analogie qui semble exister entre les fonctions d'onde _n pour un modèle «Electron-in-a-Box» et les fonctions correspondantes LCAO-MO _J (J=n) décrivant le mouvement d'un électron dans un système . En particulier cette comparaison implique que les «longueurs d'onde» de _n et de _J (J=n), qui satisfont pratiquement la relation =, ont la même signification physique. Dans ce travail on montre, que ceci n'est pas le cas. Pour un système linéaire (c.à.d. un modèle linéaire du type «Electron-in-a-Box») est reliée directement à la quantité de mouvement et par là à l'énergie cinétique, par la relation de deBroglie. Par contre on ne trouve pas une dépendance analogue entre et la composante correspondante de l'énergie cinétique dans une orbitale moléculaire LCAO _J. (Les intégrales bicentriques pour les composantes d'énergie cinétique nécessaires à ce calcul ont été déterminées pour des orbitales atomiques du type 1s.)

     

Integral invariants in chemical kinetics

Integral invariants of classical mechanical systems are used for the mathematical treatment of equilibrium systems of chemical reaction kinetics. Some conserved quantities and Hamilton equations in chemistry are shown.

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. .

     

Renormalized Rayleigh-Schrödinger perturbation theory

One method which has been used in the literature to determine the eigenvalues F _k ⁽⁰⁾ of a hamiltonian operator = + W ( = kinetic energy operator) is to apply an approximation scheme (e.g. variational method) to the operator _R () = + V + (W – V) with eigenvalues G _k (), where the eigenvalue problem associated with ^(o) = + V is solvable. Specifically, F _k ⁽⁰⁾ = G _k (1). We investigate the method from a perturbation theoretic viewpoint. There is a renormalization map R:, [0, 1], [0, ), which relates the G() to the eigenvalues E() of () = + V + W. This, in turn, implies a linear relationship between the Rayleigh-Schrödinger -series coefficients G ⁽ⁿ⁾ and the -series coefficients E ⁽ⁿ⁾ of the form G=CE, where C is an infinite lower-triangular matrix. The renormalized -series, 01, is useful in the accurate computation of F ⁽⁰⁾ as well as the eigenvalues E(), 0< . In standard cases, the -series is Borel summable to G(). Applications are made to anharmonic oscillators and hydrogen atoms in radial fields.Dedicated to Professor J. Koutecký on the occasion of his 65th birthday     

Copper(I) Acetylenide π-Complexes. Synthesis and Structure of Cluster Compound HAmp[Cu9Cl8(C≡CCH2OH)2] (HAmp is 4-Aminopyridinium Cation)

Crystals of the HAmp[Cu₉Cl₈(CCCH₂OH)₂] cluster compound (HAmp is the 4-aminopyridinium cation (NH₂–C₅H₄NH)⁺) were obtained through ac electrochemical synthesis and their structure was determined using X-ray diffraction analysis (DARCh autodiffractometer, /2 scan mode, 3435 independent reflections with F 4(F), R = 0.047). The crystals are triclinic: space group P , a = 12.547(5) Å, b = 12.502(4) Å, c = 8.201(2) Å, = 75.93(2)°, = 82.21(3)°, = 76.05(3)°, V = 1207(2) ų, Z = 2. Two crystallographically independent moieties ^–(CCCH₂OH) were detected in the complex structure. Each moiety acts as a double bridging ,-ligand and binds four or five Cu(I) atoms, thus forming the [Cu₄(CCCH₂OH)] and [Cu₈(CCCH₂OH)₂] clusters. The shortest Cu···Cu distance is equal to 2.337(4) Å.     

Differential scanning calorimetry studies on influence of microstructure on transformation of γ-Fe2O3 to α-Fe2O 3 +

The transition-Fe₂O₃-Fe₂O₃ has been investigated in oxygen and argon using DSC measurements in the temperature range 298 to 820 K. The results have been interpreted by taking into account the method of preparation, the specific microstructure of the samples and the nature of the gas used. It has been shown that the transformation temperature, and in general the absolute value of the negative enthalpy of the transformation as well, rises with increase of the specific surface area of the -Fe₂O₃. The observed fluctuations in this trend are attributed to differences in the microporosity, gas sensitivity and crystallinity of the samples.

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Zusammenfassung Der Übergang -Fe₂O₃-Fe₂O₃ in Sauerstoff- und Argonatmosphäre wurde mittels DSC im Temperaturbereich von 298–820 K untersucht. Die Ergebnisse werden unter Berücksichtigung der Präparationsmethode, der spezifischen Mikrostruktur der Proben und der Natur des benutzten Gases interpretiert. Die Phasenumwandlungstemperatur und im allgemeinen die Absolutwerte der negativen Enthalpie der Phasenumwandlung erhöhen bzw. vergrößern sich mit steigender spezifischer Oberfläche des -Fe₂O₃. Die in diesem Trend auftretenden Fluktuationen werden Unterschieden in der Mikroporosität, der Gasempfindlichkeit und der Kristallinität der Proben zugeschrieben.

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-Fe₂O₃ -Fe₂O₃ 298–820 . , . , , -Fe₂O₃. , .

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The authors are grateful to Mr. Christian Sarda for his help during the sample preparation and characterization, and to Mr. B. Maachi and Dr. M. Gougeon for their help in surface area measurements. A. C. Vajpei expresses his gratefulness for the award of a Postdoctoral Fellowship in Materials Science by the French Government, made through the Indo-French Scientists' Exchange Programme.

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Paper presented at the World Conference on Thermal Analysis, Madeira (Portugal), 1986.