dc.contributor.author |
Tanui, Josephat Kipyegon |
|
dc.date.accessioned |
2016-03-01T06:52:42Z |
|
dc.date.available |
2016-03-01T06:52:42Z |
|
dc.date.issued |
2016-03-01 |
|
dc.identifier.uri |
http://hdl.handle.net/123456789/1981 |
|
dc.description |
A thesis submitted in partial fulfillment for the degree of Master of Science in
Mechanical Engineering in the Jomo Kenyatta University of Agriculture and
Technology
2013 |
en_US |
dc.description.abstract |
The increasing demand for energy and the need for reduction of greenhouse gases has necessitated
the development of renewable sources such as biodiesel fuel. Methyl ester fuel
burns more efficiently and has lower emissions of particulate matter, unburned hydrocarbon
and carbon monoxide than fossil fuels. However, combustion of a methyl ester fuel
results in increased nitrogen oxides (NOx) emissions relative to fossil fuels. This study is
concerned with the formation of NOx in combustion of methyl formate, the simplest methyl
ester molecule, under different flame conditions. Homogeneous ignition, freely propagating
and diffusion flames of methane, methanol and methyl formate have been numerically
simulated. To this end, recently developed chemical kinetic mechanism for methyl formate
(Dooley 2009) has been identified and further developed to capture the production processes
of pollutants. This is particularly important given that kinetics of combustion of
methyl esters have not received much attention in existing literature. NOx concentration
profiles for methyl formate in all configurations studied have been compared to those of
methane/air and methanol/air flames which are well understood.
It has been established that, the thermal NO in the three fuels are produced in nearly
the same amount (within the same order of magnitude), while the prompt NO production
in methane is observed to have a significant difference (one order of magnitude higher)
compared to those of methanol and methyl formate flames. For thermal NO, the ratelimiting
step: N2 + O −! NO + N, which has a high activation energy is the decisive
reaction. N2 and O are readily available in all the three fuels, hence the thermal NO
production is nearly the same. In prompt NO, reaction: CH + N2 −! HCN + N is
the determining step. A small amount of CH and subsequently N atoms in CH3OH and
CH3OCHO explain the low values of NO concentration as compared to that for methane.
In addition, NO concentration showed a high sensitivity to reaction: NNH + O −! NH
xviii
+ NO in oxygenated fuels (CH3OH and CH3OCHO) as opposed to high sensitivity of
reaction: CH + N2 −! HCN + N seen in CH4 flames. The low concentration of N atoms
in oxygenated fuels makes the contribution through the reaction path that results in NNH
being significant.
The NO formation in freely propagating and diffusion flames is mostly through prompt
NO since the maximum flame temperatures attained are relatively low (approximately
2000 K). While the NO formation in a homogeneous system is mostly through thermal
NO mechanism (Zel’dovich mechanism) since they attained high flame temperatures (approximately
between 2800 and 3200 K) due to high initial temperatures. It is observed
that, NO concentration in a homogeneous system is significantly higher (by three orders
of magnitude) than those in freely propagating and diffusion flames. |
en_US |
dc.description.sponsorship |
Prof. P. N. Kioni
DeKUT, Kenya
Mr. A. Gitahi
JKUAT, Kenya |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Mechanical Engineering,JKUAT |
en_US |
dc.relation.ispartofseries |
Msc. Mechanical Engineering;2013 |
|
dc.subject |
Mechanical Engineering |
en_US |
dc.title |
Impact of Fuel Oxygenation on NOx Formation in Biodiesel Flames |
en_US |
dc.type |
Thesis |
en_US |