The spontaneous ignition of mixtures of n -heptane and 1-heptene in oxygen

Studies of the ignition in oxygen of binary mixtures of n -heptane and 1-heptene at tempera­tures below 400°C show that under all conditions investigated both hydrocarbons are consumed during ignition. However, below ca . 300°C, where 1-heptene is considerably less reactive than n -heptane, the alkene is not involved in the process leading to ignition and the ignitability of mixtures is controlled effectively by the concentration of the alkane. In con­trast, above 300 °C, 1-heptene is at least as ignitable as n -heptane and the alkene appears to contribute to the process leading to ignition. This shows that, although at relatively high temperatures conjugate alkenes maybe among the principal intermediates involved in the ignition of alkanes, this is not the case at lower temperatures. Here, the reaction between heptyl radicals and oxygen is additive leading to the formation of the corresponding heptylperoxy radicals and ignition then results from further reactions of these latter radicals. Comparison of the results obtained in stainless steel and vitreous vessels shows that the nature of the surface has little effect on limiting ignition pressures but does affect the multiplicity of cool flames. It thus appears that the surface exerts a considerable influence on the course of the reaction following the passage of a cool flame but not on the processes leading to the first cool flame and to ignition.

Spontaneous ignition pressure-temperature relationships of ethylene oxide-oxygen and -air mixtures have been studied. A low-temperature ignition system exists and cool flames can be initiated in air at atmospheric pressure and below. The propagation of cool flames through cold mixtures imder this condition has not, however, been observed. Nevertheless, ethylene oxide itself propagates a decomposition flame and is inflammable at constant volume in admixture with air for all percentages above 3*6. The products of decomposition are almost entirely accounted for by the two overall reactions: C 2 H 4 0 = CH 4 + CO +17-2 kcal., 2C 2 H 4 0 = C 2 H 4 + 2CO + 2H 2 - 2 x 6-15 kcal. These reactions are also very significant in the non-luminous flames that have been found to be propagated through the richer mixtures of ethylene oxide with air. It is shown that the latter flames are initiated only at high temperatures, of the same order as for normal flames, and that they correspond with the non-luminous flames occurring near to the hightemperature spontaneous ignition limit of richer mixtures.


Alloy Digest ◽  
2006 ◽  
Vol 55 (5) ◽  

Abstract AK Steel 410S is a fully ferritic stainless steel with elements added to retard austenite formation at high temperatures. The resulting low hardening allows for use as oxidation-resistant parts. This datasheet provides information on composition, physical properties, hardness, elasticity, and tensile properties. It also includes information on corrosion resistance as well as forming, heat treating, and joining. Filing Code: SS-964. Producer or source: AK Steel.


A detailed mathematical model of the non-isothermal oxidation of acetaldehyde has been found to give a realistic simulation of (i) single and multiple cool flames, their limits, amplitudes and induction periods; (ii) two-stage ignition; and (iii) the negative temperature coefficient for the maximum rate of slow combustion. A simplified form of the model, valid over a limited range of conditions, has been subjected to mathematical analysis to provide interpretations of the effects simulated by the detailed model. It is concluded that cool flames are thermokinetic effects often, but not exclusively, of an oscillatory nature, and that a satisfactory account of cool-flame phenomena must necessarily take reactant consumption into account.


1999 ◽  
Vol 121 (2) ◽  
pp. 365-375 ◽  
Author(s):  
R. J. Benjamin ◽  
A. R. Balakrishnan

A model for nucleate pool boiling heat transfer of binary mixtures has been proposed based on an additive mechanism. The contributing modes of heat transfer are (i) the heat transferred by microlayer evaporation, (ii) the heat transferred by transient conduction during the reformation of the thermal boundary layer, and (iii) the heat transferred by turbulent natural convection. The model takes into account the microroughness of the heating surface which has been defined quantitatively. The model compares satisfactorily with data obtained in the present study and in the literature. These data were obtained on a variety of heating surfaces such as a vertical platinum wire, a horizontal stainless steel tube and flat horizontal aluminium, and stainless steel surfaces (with various surface finishes) thereby demonstrating the validity of the model.


From the beginning of the century, and more especially of late years, an almost uninterrupted series of papers have appeared on the above subject. Unfortunately few of the authors have reduced their measurements to absolute units, thus rendering comparison of the results obtained very difficult. The first part of this paper is to some degree an extension to higher temperatures and pressures of the work so ably done by Dr. Bottomley, whilst the names of Langley, Paschen, Weber, and many others will occur to anyone glancing through the second and third parts.


2019 ◽  
Vol 283 ◽  
pp. 07011
Author(s):  
Didier Flotté ◽  
David Macel ◽  
Abd Ennour Bouzenad ◽  
Frédéric Navacchia

Monitoring the operation of the latest-generation nuclear reactor requires ultrasonic transducers able to operate at very high temperatures (> 600°C). To achieve this, CEA has requested from “Institut de Soudure” to help developing a new technology for these transducers compared to the one previously developed. This began with the development of a reliable assembly technique between a lithium niobate piezoelectric disc whose Curie temperature exceeds 1100°C and stainless steel discs. The chosen solution was to braze the niobate disc between two stainless steel discs. Parallel to this development, it was also necessary to develop a NDE procedure to verify the quality of the brazing assemblies. This development began with a simulation of immersion ultrasonic testing of the assemblies. The constraints were to be able to control the two brazed interfaces from the same access face, with the possibility of detecting and dimensioning defects with an equivalent diameter of 0.25 mm. This phase is important to define the optimal transducer with the associated operating conditions. The first assemblies validated the preliminary choices. To exploit the cartographies obtained, a signal processing procedure was developed. This enabled an automatic characterization of the indications observed. However, the analysis of the signals observed proved to be more complex than the one predicted by the simulation. Once the origin of the various observed signals was identified it was then possible to define windows allowing the construction of the cartographies to analyze. In case of a good quality assembly, it was possible to qualify the generated beam and to image it in the focal plane but with an observed signal having a very low damping. These first encouraging results, however, show that there is still some validation and development work to increase the sensitivity of the developed translator and its damping.


1961 ◽  
Vol 83 (2) ◽  
pp. 133-138 ◽  
Author(s):  
D. J. Baldwin ◽  
G. W. Rowe

An experimental study of the friction of metals which have been coated with inorganic films by reaction with their surrounding atmosphere. The specimens are first cleaned at high temperature in vacuo and then heated in the selected reactive vapor. Many coatings will prevent seizure and give a fairly constant but high coefficient of friction up to high temperatures. Layer-lattice compounds such as MoS2, CrCl3, and TiI2 give much lower friction at all temperatures below those at which the film decomposes or evaporates (about 850 C for molybdenum disulphide). A film of boron nitride formed on boron shows a high intrinsic friction, but this can be reduced by certain vapors or by raising the temperature above about 800 C. Most of the experiments were performed with very light loads but the films are shown to be effective under kilogram loads. A simple indentation test capable of selecting lubricants under loads up to 12 tons is described. This shows that a film formed by heating stainless steel in CCl2F2 will lubricate at 400 C when the steel is deformed by over 50 per cent.


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