The thermal decomposition of nitrous oxide I. Secondary catalytic and surface effects

In the region of pressure 0 to 500 mrn approximately to the equation the thermal decomposition of nitrous oxide conforms approximately to the equation k = an /1 + a'n + bn , where k is the form al first-order rate constant, — (1/n) d n /d t , n the initial concentration and a, a' and b are nearly constant. Above about 100 m m this expression approximates to k = A + bn , which holds up to several atmospheres. Fresh and more detailed experiments have once again disproved the suggestion that the first term in these expressions is due to a surface reaction. (In certain states of reaction vessels, made of a particular brand of silica, a surface reaction may appear but is immediately recognizable by special criteria, and can be eliminated.) Detailed study of the formation of nitric oxide in the course of the decomposition, and of the effect of inert gas upon this process, shows that side reactions involving oxygen atoms, chain reactions and catalysis by nitric oxide play only minor parts in determining the shape of the k-n curve. The form of this curve, which is an inherent character of the reaction N 2 O = N 2 + O, raises theoretical questions of considerable interest.

1985 ◽  
Vol 63 (11) ◽  
pp. 2945-2948 ◽  
Author(s):  
J.-R. Cao ◽  
R. A. Back

The thermal decomposition of cyclobutane-1,2-dione has been studied in the gas phase at temperatures from 120 to 250 °C and pressures from 0.2 to 1.5 Torr. Products were C2H4 + 2CO, apparently formed in a simple unimolecular process. The first-order rate constant was strongly pressure dependent, and values of k∞ were obtained by extrapolation of plots of 1/k vs. 1/p to1/p = 0. Experiments in a packed reaction vessel showed that the reaction was enhanced by surface at the lower temperatures. Arrhenius parameters for k∞, corrected for surface reaction, were log A (s−1) = 15.07(±0.3) and E = 39.3(±2) kcal/mol. This activation energy seems too low for a biradical mechanism, and it is suggested that the decomposition is probably a concerted process. The vapor pressure of solid cyclobutane-1,2-dione was measured at temperatures from 22 to 62 °C and a heat of sublimation of 13.1 kcal/mol was estimated.


1956 ◽  
Vol 25 (1) ◽  
pp. 106-115 ◽  
Author(s):  
Frederick Kaufman ◽  
Norman J. Gerri ◽  
Roger E. Bowman

The first-order rate constant for the thermal decomposition of di-tertiary butyl peroxide in the pressure range 0 to 600 mm follows an equation of the form k = A 1 n /(1+ A' 1 n + A 2 n , where n is the peroxide pressure. For a given value of n additions of sulphur hexafluoride (which appears from analysis to have no chemical effect) raise k to a limiting value, k n ,∞. This value is itself a function of the peroxide pressure approximately of the form k n , ∞ = An /(1+A' n )+B. In the light of previous work on nitrous oxide and on paraffins, these results are tentatively explained in terms of a scheme in which energized molecules go reversibly to special activated states from which decomposition follows either spontaneously or when induced by collisions.


The influence of foreign gas additions (argon, nitrogen, carbon dioxide, carbontetrafluoride and mixtures of them) on the thermal decomposition of nitrous oxide at a series of different initial pressures has been studied. The curves of k , the formal first-order constant, as a function of x , the foreign-gas pressure, show regions of rapidly falling slope analogous to those found in the curves of k against n , the initial pressure of nitrous oxide. The forms of the curves have been investigated in some detail, and suggest very strongly the existence of potentially rate-determining processes other than those normally assumed in unimolecular reactions (which are energization of molecules in collisions and chemical decomposition of these molecules). It is now postulated that spontaneous and collision-induced transfers of energized nitrous oxide molecules to trip let states constitute the processes in question, and on this basis the forms of the k , n and k , x curves are interpreted. This postulate links up with certain spectroscopic considerations previously advanced by Herzberg.


It was recently discovered that iodine exerts a pronounced catalytic influence on the thermal decomposition of nitrous oxide. Bromine and chlorine have now been found to have similar effects. The reactions are of the first order with respect to the nitrous oxide and there appears to be little doubt that decomposition into a nitrogen molecule and an oxygen atom occurs under the influence of the halogen. The balance of evidence is in favour of the hypothesis that the effective catalyst is the free halogen atom. Whether the oxygen atom from the nitrous oxide remains attached to the halogen for a finite time cannot be definitely stated.


In the thermal decomposition of diethyl ether the first-order rate constant ( k ) varies with the pressure ( p ) of the ether itself, or that of added hydrogen, or that of various chemically inert gases according to a more complex pattern than has hitherto been supposed. In general, k increases approximately linearly with p X over a certain range: the slope of the curve then decreases as though a limit were being approached. When X refers to ether, hydrogen or certain other gases no limit is in fact reached, but k continues to increase at a considerably reduced rate. With certain gases, however, the slope of the curve becomes very small or zero. Changes in k are not explicable by variations in the chemical composition of the products. The forms of the k-p curves are qualitatively similar for the uninhibited reaction (largely a chain process) and for the nitric oxide-inhibited reaction (hypothetical molecular reaction), but the effects are quantitatively quite different. The k-p relations for the molecular reaction conform to those recently established for the decomposition of paraffins and of nitrous oxide, and may possibly be interpreted by the extended theory of unimolecular reactions proposed for these examples. The relations for the chain reactions are more complicated but the interpretation probably includes considerations similar to the above, applied to the initial molecular process by which the chains start.


When the homogeneous thermal decomposition of nitrous oxide was first studied in connection with the theory of gaseous reactions, the principal problem was to decide whether the activation of the molecules occurred independently of collisions, as would have been required by the radiation theory of activation. The influence of pressure on the rate of reaction showed definitely that the activation depended on a collisional process, in which sense the reaction proved to be bimolecular. The characteristic of an ideal bimolecular reaction is that the time of half change should be inversely proportional to the initial pressure. It was in fact found that the reciprocal of the half change period when plotted against initial pressure gave a straight line, which, however, did not pass through the origin. This meant that at low pressures a reaction of the first order was occurring, as well as the bimolecular change. This first order reaction was not further investigated, as it seemed quite possible that it was a surface reaction, the intrusion of which became relatively more serious as the pressure fell. It was observed, furthermore, that the complete course of a decomposition at a given initial pressure was not represented very well by the usual bimolecular equation; this, however, was capable of explanation in terms of an autocatalytic effect of the by-products of the reaction, since small amounts of the higher oxides of nitrogen were known to be formed in addition to the oxygen and nitrogen constituting the main products. More recently two new observations have been made, rendering desirable a fuller investigation of some of the details about the reaction, which have hitherto been regarded as of less importance than its general interpretation in terms of the collisional mechanism.The first of these is the observation of Volmer and Kummerow that, at low partial pressures of nitrous oxide, inert gases exert an accelerating influence on the decomposition. This suggests that the low pressure unimolecular part of the decomposition is perhaps really homogeneous, and also of the “quas-unimolecular type” which is subject to the influence of foreign gases. The second of the observations referred to is that of Voliner and Nagasako, who state that, between 1 and 10 atmospheres, the whole decomposition becomes of the first order. Thus the second order reaction observed in the earlier experiments, which were not carried out at pressures greater than an atmosphere, would be the low pressure part of a quasi-unimolecular reaction, The difference in mechanism between a true bimolecular reaction and the quasi-unimolecular reaction would be simply that in the former the nitrous oxide reacts at the moment of collision, while in the latter it survives the activating collision for a definite period and then splits up spontaneously into N 2 and an oxygen atom, unless in the meantime it has been deactivated.


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