Pyrolysis of iodobenzene by the toluene carrier technique and determination of D[C6H5—I]

1976 ◽  
Vol 54 (19) ◽  
pp. 2981-2984 ◽  
Author(s):  
R. John Kominar ◽  
Michael J. Krech ◽  
Stanley James W. Price

The pyrolysis of C6H5I has been studied by the toluene carrier technique over the temperature range 861–955 K using contact times of 0.54–3.28 s and total pressures of 2.5–4.13 kPa. Percent decomposition based on analysis for residual C6H5I ranged from 5.6–93.3%. Only trace quantities of I2 were observed and when HI was trapped out the only other gaseous products were small quantities of hydrogen and methane in about a 2:1 ratio. Within the limits of the experimental method the decomposition was found to be homogeneous and first order.[Formula: see text]The Arrhenius equation obtained for reaction 1 is[Formula: see text]Making an approximate correction of the activation energy to 298 K then gives[Formula: see text]

1978 ◽  
Vol 56 (11) ◽  
pp. 1589-1592 ◽  
Author(s):  
R. John Kominar ◽  
Michael J. Krech ◽  
Stanley James W. Price

The pyrolysis of C6H5Br bas been studied by the toluene carrier technique over the temperature range 1018 to 1126 K using contact times of 1.18 to 2.85 s and total pressures of 3.8 to 4.4 kPa. Percent decomposition based on analyses of residual C6H5Br ranged from 4 to 89%. When HBr was trapped out and quantitatively determined it accounted for more than 95% of the bromine expected. Within the limits of the experimental method the decomposition was found to be homogeneous and first order.[Formula: see text]The Arrhenius equation for reaction [1] is[Formula: see text]Making an approximate correction of the activation energy to 298 K then gives D(C6H5—Br) = 313 ± 5.4 kJ mol−1.


1931 ◽  
Vol 5 (6) ◽  
pp. 636-647 ◽  
Author(s):  
C. C. Coffin

The decomposition represented by the general equation[Formula: see text]has been found to take place according to the monomolecular law. In the case of the several homologous esters already investigated at pressures above 10 cm. of mercury the reaction is entirely homogeneous, is uninfluenced by the presence of inert gases and obeys the Arrhenius equation. This paper describes the experimental method and deals with the decomposition of ethylidene diacetate to acetaldehyde and acetic anhydride at temperatures of 220° to 268 °C. and at initial pressures of 11 to 46 cm. of mercury. The heat of activation is 32900 cal./mol and the velocity constants (sec−1) are given by the equation, ln [Formula: see text]. The theoretical significance of the data is discussed.


1967 ◽  
Vol 6 (48) ◽  
pp. 911-915 ◽  
Author(s):  
M. P. Hochstein ◽  
G. F. Risk

The activation energy ϵe1 of polar firn samples determined by D.C. resistivity measurements is a function of temperature and density. In the temperature range −2° C. to −10° C. ϵe1 decreases with decreasing temperature reaching a nearly constant value for temperatures colder than −10°C.; in the temperature range −10°C. to −21°C. ϵe1 was found to decrease with increasing density and to lie between 0.7 eV. and 0.4 eV.


1967 ◽  
Vol 6 (48) ◽  
pp. 911-915 ◽  
Author(s):  
M. P. Hochstein ◽  
G. F. Risk

The activation energyϵe1of polar firn samples determined by D.C. resistivity measurements is a function of temperature and density. In the temperature range −2° C. to −10° C.ϵe1decreases with decreasing temperature reaching a nearly constant value for temperatures colder than −10°C.; in the temperature range −10°C. to −21°C.ϵe1was found to decrease with increasing density and to lie between 0.7 eV. and 0.4 eV.


1970 ◽  
Vol 23 (4) ◽  
pp. 749 ◽  
Author(s):  
JJ Batten ◽  
DC Murdie

The activation energy has been determined in the temperature range 170-198�. If the sample was spread the activation energy was independent of the definition of the kinetic parameter substituted in the Arrhenius equation and was 63 kcal mole-1. In the case of the unspread samples the activation energies of the induction, acceleration, and maximum rates were 49, 43, and 62 kcal mole-1 respectively. The effect that sample geometry has on the activation energy is attributed to gaseous decomposition products influencing the reaction.


2013 ◽  
Vol 22 ◽  
pp. 255-260 ◽  
Author(s):  
R. V. BARDE ◽  
S. A. WAGHULEY

The binary glassy systems 60V2O5-(40-x)P2O5 –xB2O3 were prepared by melt quenching technique. The mole of B2O3 was varies from 5 to 20 mol % with constant mol % of V2O5 during preparation of glass samples. The dc electrical conductivity of samples was measured in temperature range 303-473 K and found to be higher for sample 60 V2O5-20P2O5 –20B2O3 . Using the Arrhenius equation of conductivity, the activation energy of conduction is estimated. The conduction in these glasses is takes place by phonon-assisted hopping between the localized states.


1979 ◽  
Vol 57 (18) ◽  
pp. 2482-2483 ◽  
Author(s):  
Marsha T. J. Glionna ◽  
Huw O. Pritchard

The thermal isomerisation of allyl isocyanide to allyl cyanide has been studied in the gas phase over the temperature range 130–200 °C. The reaction is homogeneous and first order, and at high pressure (20 Torr) has an activation energy of 40.8 ± 0.6 (2sdm) kcal mol−1; the corresponding range of frequency factor is 1014.77±0.30 s−1.


1959 ◽  
Vol 26 (2) ◽  
pp. 227-234
Author(s):  
Pericles S. Theocaris

Abstract An experimental method is developed for the calculation of stresses in plane elasticity problems. The method consists substantially in determining a function of the complex variable representing the field of isostatics. This function has a convenient form so that the boundary conditions can be expressed by simple relations. From the isostatics, which are traced experimentally, the differential parameter of first order h can be calculated all over the field. The components of stresses are expressed by relations depending on boundary conditions and the parameter h. The method is applied to two particular problems of plane elasticity and a comparison of the results obtained by this method and by analytic methods is provided.


1958 ◽  
Vol 11 (1) ◽  
pp. 34
Author(s):  
WD Johnson ◽  
NV Riggs

The reaction of phenyliodoso acetate and aceto-p-toluidide in acetic acid is first order in each reactant and measured rates fit the Arrhenius equation in the temperature range 15-45 �C. Addition of water to the solvent markedly accelerates the reaction, whereas addition of benzene lowers the rate and acetic anhydride has little effect. A polar transition state is indicated.


1956 ◽  
Vol 29 (1) ◽  
pp. 37-48 ◽  
Author(s):  
Walter Scheele ◽  
Otto Lorenz

Abstract If we disregard for the moment the phenomena which occur in the interaction of thiuram disulfide with geraniol under the influence of air and confine our consideration to the results which can be deduced from the study of this reaction in a stream of nitrogen, we are led to the conclusion that geraniol, which was used as a model compound, behaves with respect to its interaction with tetraethylthiuram disulfide, not only qualitatively but also quantitatively, exactly like rubber, and that it is not to be assumed that other tetraalkylthiuram disulfides as well as other compounds which are analogous to geraniol will behave differently. Thus the results can be evaluated as a proof that the vulcanization of natural rubber by thiuram disulfides depends on nothing other than a definite and always similar interaction with the allyl groups of the polyisoprene chain. The results of the investigation described in this paper can be regarded, moreover, as support for the correctness of our procedure in the clarification of the vulcanization mechanisms, and they stress the importance of analytical-chemical methods, which have certainly not been pursued in the past with the necessary intensity and insight. These investigations are being continued. It has already been found that the vulcanization of natural rubber with thiuram monosulfides and sulfur leads to the same results as vulcanization with thiuram disulfides. This has been conjectured, to be sure, by a number of workers. However, it was never really demonstrated experimentally. We shall report on this in the near future. The experimental results can now be summarized as follows : 1. The reaction between thiuram disulfide and geraniol (demonstrated by the example of tetraethylthiuram disulfide) takes place qualitatively and quantitatively like the interaction between thiuram disulfide and natural rubber. In the vulcanization of rubber by thiuram disulfides, therefore, there is involved a reaction of the thiuram disulfide with the allyl groups, leading to a definite conversion. 2. It was found that in the interaction of geraniol with thiuram disulfide under nitrogen and in the presence of zinc oxide, the limiting value of zinc dithiocarbamate amounts to 66 mole-per cent of the original thiuram disulfide, independent of the temperature. This was the result found in the study of the reaction of the thiuram disulfides with rubber. 3. We were able to show that the limiting value of the dithiocarbamate yield in the interaction of tetraethylthiuram disulfide with geraniol is independent of the thiuram disulfide concentration. This is likewise true for the reaction of the thiuram disulfides with natural rubber. From this it follows that the interaction of thiuram disulfides with allyl groupings, as they occur in the polyisoprene chain, is apparently a stoichiometric one. For this reason we can no longer retain the assumption that the limiting value of the yield of dithiocarbamate is the result of a sterically hindered reaction. 4. The change of concentration of zinc dithiocarbamate in the interaction of tetraethylthiuram disulfide with geraniol under nitrogen can be accounted for by postulating a reaction of the first order. The velocity constants were calculated and it was found that the resulting activation energy is somewhat greater than the one for the interaction with natural rubber. 5. Similarly the concentration of thiuram disulfide obeys a first-order reaction as it falls off to zero. The velocity constants were calculated. The activation energy obtained from the temperature dependence is in good agreement with that found for the interaction with rubber. 6. In the presence of oxygen, the reaction between thiuram disulfide and geraniol takes a quite different course. The rate of decrease of concentration of thiuram disulfide, which likewise follows a first-order reaction, is higher. The yield of zinc dithiocarbamate does not attain the constant value of 66 mole-per cent of the original thiuram disulfide. In the temperature range studied, the amount of dithiocarbamate found is smaller. The limiting value reached at the various temperatures is progressively smaller, the lower the temperature chosen. Whether by expanding the temperature range, one would eventually reach a minimum and a maximum limiting value has not been investigated.


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