Estimating the activation energy of exothermic reactions in substances that undergo self heating processes with the Heat Release method: Use of sub critical data

Fuel ◽  
2014 ◽  
Vol 125 ◽  
pp. 152-154 ◽  
Author(s):  
Giovanni Cocchi
Author(s):  
Harvinder S Sidhu ◽  
Mark I Nelson ◽  
Thiansiri Luangwilai ◽  
Xiao Dong Chen

We model the increase in temperature in compost piles or landfill sites due to micro-organisms undergoing exothermic reactions. The model incorporates the heat release due to biological activity within the pile and the heat release due to the oxidation of cellulosic materials. The heat release rate due to biological activity is modelled by a function which is a monotonic increasing function of temperature over a particular range and followed by a monotone decreasing function of temperature. This functionality represents the fact that micro-organisms die or become dormant at high temperatures. The heat release due to the oxidation reaction is modelled by the usual manner using Arrhenius kinetics. The bifurcation behaviour is investigated for two-dimensional slab geometries to determine the critical sizes of the compost piles.


2016 ◽  
Vol 94 (5) ◽  
pp. 494-500 ◽  
Author(s):  
Xuyao Qi ◽  
Haibo Xue ◽  
Haihui Xin ◽  
Cunxiang Wei

Hydroxyl groups are one of the key factors for the development of coal self-heating, although their detailed reaction pathways are still unclear. This study investigated the reaction pathways in coal self-heating by the method of quantum chemistry calculation. The Ar–CH2–CH(CH3)–OH was selected as a typical structure unit for the calculation. The results indicate that the hydrogen atoms in hydroxyl groups and R3–CH are the active sites. For the hydrogen atoms in hydroxyl groups, they are directly abstracted by oxygen. For hydrogen atoms in R3–CH, they are abstracted by oxygen at first and generate peroxy-hydroxyl free radicals, which abstract the hydrogen atoms in hydroxyl groups later. The reaction of R3–CH contains three elementary reactions, i.e., the hydrogen abstraction of R3–CH by oxygen, the conjugation reaction between the R3C■ and oxygen atom, and the hydrogen abstraction of –OH by hydroxyl free radicals. Then, the microstructure parameters, IRC pathways, and reaction dynamic parameters were respectively analyzed for the four reactions. For the hydrogen abstraction of –OH by oxygen, the enthalpy change and activation energy are 137.63 and 334.44 kJ/mol, respectively, which will occur at medium temperatures and the corresponding heat effect is great. For the reaction of R3–CH, the enthalpy change and the activation energy are −3.45 and 55.79 kJ/mol, respectively, which will occur at low temperatures while the corresponding heat influence is weak. They both affect heat accumulation and provide new active centers for enhancing the coal self-heating process. The results would be helpful for further understanding of the coal self-heating mechanism.


1992 ◽  
Vol 260 ◽  
Author(s):  
Q. Z. Hong ◽  
K. Barmak ◽  
L. A. Clevenger

ABSTRACTThe composition dependence of crystallization of amorphous Co-Si alloys has been investigated. Crystallization temperature decreased slowly from 400°C for a Co0.42Si0.58 alloy to 300°C for a CO0.2Si0.8 alloy. However, abrupt decrease in the crystallization temperature was observed for alloys with the monosilicide and disilicide compositions. The crystallization of alloys compositionally close to the disilicide was a one-step process with an activation energy of about 1.3 eV. The heat release and the volume contraction during crystallization of the stoichiometric Co0.33Si0.67 alloy were measured to be 0.118 eV/atom and 0.6%, respectively. In the case of the CO0.2Si0.8 alloy, complete crystallization was achieved in two steps with an activation energy of 2.1 eV for the primary crystallization.


1996 ◽  
Vol 329 ◽  
pp. 389-411 ◽  
Author(s):  
F. J. Higuera ◽  
A. Liñán

The flow field of a diffusion flame attached to a thick-rim injector between two coflowing streams of fuel and oxidiser is analysed in the Burke–Schumann limit of infinitely fast reaction rate. The length of the recirculation region immediately behind the injector and the velocity of the recirculating fluid are proportional to the shear stresses of the reactant streams on the wall of the injector for a range of rim thicknesses, and the structure of the flow in the wake depends then on three main non-dimensional parameters, measuring the gas thermal expansion due to the chemical heat release, the air-to-fuel stoichiometric ratio of the reaction, and the air-to-fuel ratio of wall shear stresses. The recirculation region shortens with increasing heat release, and the position of the flame in this region depends on the other two parameters. An asymptotic analysis is carried out for very exothermic reactions, showing that the region of high temperature around the flame is confined by neatly defined boundaries and the hot fluid moves like a high-velocity jet under a favourable self-induced pressure gradient. The immediate wake is surrounded by a triple-deck region where the interacting flow leads to an adverse pressure gradient and a reduced shear stress upstream of the injector rim for sufficiently exothermic reactions. Separation of the boundary layers on the wall of the injector, however, seems to be postponed to very large values of the gas thermal expansion.


2010 ◽  
Author(s):  
Mehrzad Kaiadi ◽  
Per Tunestal ◽  
Bengt Johansson

Fuel ◽  
1998 ◽  
Vol 77 (1-2) ◽  
pp. 19-22 ◽  
Author(s):  
J.C. Jones ◽  
K.P. Henderson ◽  
J. Littlefair ◽  
S. Rennie

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