An aromatics and cC5H5-8 model with improved transport for flat flames, flow reactors and shock tubes.

Elena Nehrbass, Henry Tang, Robert G. Butler

Research output: Chapter in Book/Report/Conference proceedingConference contributionpeer-review

Abstract

Presenting improvements to a detailed, quantitative, 1-dimensional, kinetic, aromatics and cC5H5-8 submodel with thermodynamics and transport. The model, with ∼250 species and ∼2000 reactions, includes a full NOx chemistry sub-model. Transport parameters:e, s and a are all determined by empirical or experimental data. Most m values are given by experimental values for the parent compounds and empirically for their radicals. Zrot has been set to 1 or experimental values. Shock tube conditions are explored. Flow reactor and flat flame results are updated. Selected experiments on toluene, benzene, cyclopentene (CPE) and cyclopentadiene are examined. A new method is implemented to avoid arbitrarily time-shifting the modeling data to match the fuel concentration at 50% consumption. Instead, the method of least squares fits the experimental data to a 1st-3rd order polynomial. The least squares value is compared against the modeling calculations and a root-mean squared (RMS) goodness of fit (GoF) is calculated. The time shift is then determined numerically to the millisecond by minimizing the GoF. Similarly when tuning the model using the concentrations of 1,3-cyclopentadiene (CPD) Indene, Benzene or sums of C4 and C3 species a GoF is used to iteratively determine the best rate constants. With this latest version of the model it is no longer necessary to tune rate constants for naphthalene, 1,2-dihydronaphthalene or 1-phenyl-1,3-butadiene. The model is compared to the experimental oxidation of CPD in an atmospheric pressure flow reactor and a shock tube. Side products for two reactions have been changed from 2H to H2 to avoid early and unrealistic chain branching: 2 cC5H6 → 1,2 dihydronaphthalene + H2 and 2 cC5H6 → 1-phenyl-1,3-butadiene + H2. The main naphthalene formation route is now 2 cC5H5 → C10H8 + H2 with k=1011 × e-34000/(8.314×T) cm3mol-1s1. Other changes in derived rates are discussed.

Original languageEnglish
Title of host publication8th US National Combustion Meeting 2013
PublisherWestern States Section/Combustion Institute
Pages283-287
Number of pages5
ISBN (Electronic)9781627488426
StatePublished - 2013
Externally publishedYes
Event8th US National Combustion Meeting 2013 - Park City, United States
Duration: 19 May 201322 May 2013

Publication series

Name8th US National Combustion Meeting 2013
Volume1

Conference

Conference8th US National Combustion Meeting 2013
Country/TerritoryUnited States
CityPark City
Period19/05/1322/05/13

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