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Diesel Combustion and Emissions
Diesel
combustion is the process that occurs when a fuel blend, chosen for its
ability to auto-ignite, is injected into a volume of air that has been
compressed to a high temperature and pressure. When fuel is injected
into the turbulent compressed air inside the engine cylinder, it does
not ignite immediately. There is a time period called the ignition
delay, during which the fuel must heat up, vaporize, mix with air,
and undergo chemical precombustion reactions that produce the radicals
necessary for spontaneous ignition. The classical notion of ignition
delay calls the heating, vaporization and mixing processes the "physical
delay" and the pre-reactions the "chemical delay." This can be deceptive
in that all of the processes can be, and probably are, occurring
simultaneously.
After sufficient time has elapsed, ignition will occur spontaneously at
multiple nuclei in regions of fuel-air mixture that have fuel-air ratios
close to stoichiometric. Combustion proceeds very rapidly due to the
backlog of prepared or nearly prepared fuel-air mixture formed during
the ignition delay period. The rapidly rising temperatures and pressure
in the cylinder accelerate the combustion in an uncontrolled manner
until the backlog is depleted. This portion of the combustion process is
usually called premixed combustion. The remainder of the fuel in
the spray core is still too rich to burn, so combustion slows down and
is controlled by the rate at which the air is entrained and a
combustible mixture formed. This portion of the combustion process is
called mixing controlled or diffusion burning. Thus, while
chemical kinetics dominates the ignition delay, the high temperatures
and pressures of the post-ignition gases promote very fast reaction
rates which make fuel-air mixing the rate determining process.
Some fuels will autoignite more quickly after being
injected into the diesel engine than others. The laboratory test that
is used to measure this tendency is the Cetane Number Test (ASTM D
613). This test is described in detail in the section on
ignition indices. Fuels with a high cetane number will have short
ignition delays and a small amount of premixed combustion since little
time is available to prepare the fuel for combustion.
Diesel engines can be divided into two basic types, direct injection and
indirect injection. A direct injection diesel engine combustion system
is shown in the picture below.

Figure 1. Direct Injection Combustion System
In the direct injection diesel engine, the fuel is
sprayed into the combustion chamber directly above the piston. The
piston usually has a recess or bowl that is designed to confine the air
into a region that matches the fuel spray trajectory. This type of
system relies primarily on the momentum of the fuel spray to mix the
fuel and air. A drawback of this type of system is that there is a
chance that unburned fuel can contact the cylinder wall and find its way
down past the piston rings into the crankcase. When these engines are
operated on fuel with low volatility, some of the fuel that is slow to
vaporize may be deposited on the cylinder walls and end up diluting the
lubricating oil.
For more information on fuel dilution of the lubrication oil,
click here.
The second type of diesel engine is the indirect injection engine as
shown in Figure 2. In this type of engine, the fuel is injected into a
separate chamber that is connected to the main chamber above the piston
by a narrow passage-way. When the piston rises toward top-dead-center,
the air is forced through the connecting passage at high velocity into
the small chamber, called a swirl chamber. The high velocity air
rotates at high velocity in the chamber as fuel is injected. The
diagram also shows a glow plug being inserted into the chamber, which
helps with cold starting. This type of system relies on the high
velocity air swirl to mix the air so the fuel injection system can
operate at lower pressures and be less expensive. After the fuel
ignites, the combusting mixture pushes back out through the passage-way
where the rise in pressure does work on the piston.

Figure 2. Indirect Injection Combustion System.
The indirect injection (IDI) engine is less efficient than the direct
injection (DI) engine. This is because the high velocity air motion in
the combustion chamber causes high heat transfer rates resulting in
greater loss of fuel energy. The lower efficiency of the IDI engine has
resulted in it being out-of-favor and although there are a large number
of these engines currently being produced, virtually all new engine
designs use direct injection technology. An advantage of the IDI engine
was that it was generally found to be more fuel tolerant. Having the
liquid fuel injected into a separate chamber kept most of the fuel away
from the piston rings and lessened the likelihood of fuel contamination
of the lubricating oil and fouling of the piston rings. During the
1970s, many researchers experimented with using raw vegetable oils in
diesel engines, either as pure fuels or as blends. In those cases where
good results were achieved it was generally with IDI engines. DI
engines tended to degrade slowly due to incylinder deposits and seized
piston rings.
Diesel Emissions
Why do we worry about them?
The main reason we worry about the emissions
from diesel engines is because the EPA regulates them. Table 1 shows
the allowable values for each of the 4 pollutants that the EPA currently
regulates.
Table 1. EPA Heavy Duty Diesel Emissions Standards
|
Year |
CO, g/bhp-hr |
HC, g/bhp-hr |
NOx, g/bhp-hr |
PM, g/bhp-hr |
|
1988 |
15.5 |
1.3 |
10.7 |
0.6 |
|
1990 |
15.5 |
1.3 |
6.0 |
0.6 |
|
1991 |
15.5 |
1.3 |
5.0 |
0.25 |
|
1994 |
15.5 |
1.3 |
5.0 |
0.1 (0.07 for buses)* |
|
1998 |
15.5 |
1.3 |
4.0 |
0.1 |
|
2004 |
15.5 |
Option 1: NMHC+NOx = 2.4Option 2: NMHC+NOx =
2.5, NMHC=0.5 |
0.1 |
*PM
standard for buses dropped to 0.05 in 1996 with 0.07 in-use.
Table 2 shows emissions data for five different engines that are
typical of current in-use on-highway diesel engines. It can be seen
that these engines have no trouble meeting the regulation levels for CO
and HC. However, NOx and particulate are usually very close to the
regulated values. Furthermore, measures taken to reduce NOx tend to
increase particulate and measures to reduce particulate usually increase
NOx.
Table 2. Typical Emissions Levels of Current Engines
|
Year |
CO, g/bhp-hr |
HC, g/bhp-hr |
NOx, g/bhp-hr |
PM, g/bhp-hr |
|
1991 DDC 6V-92TA |
1.67 |
0.45 |
4.46 |
0.26 |
|
1991 DDC S-60 |
2.19 |
0.14 |
4.28 |
0.23 |
|
1998 Cummins N-14 |
0.75 |
0.23 |
4.57 |
0.106 |
|
1998 DDC S-50 |
1.49 |
0.06 |
4.50 |
0.102 |
|
1998 Cummins B5.9 |
2.05 |
0.31 |
4.70 |
0.128 |
The other reason why we worry about
diesel emissions is that these substances are toxic and can contribute
to health problems.
Carbon monoxide - Is colorless, tasteless, and
odorless. I+ Does not irritate the skin or mucous membranes. CO binds
to the hemoglobin in the blood with 210 times the strength of oxygen.
As contact with CO increases, more and more hemoglobin is bound to CO
and the oxygen carrying capacity of the blood decreases resulting in
headaches, dizziness, unconsciousness and ultimately death.
Unburned Hydrocarbons - Some constituents in the
unburned hydrocarbon material are strong irritants of mucous membranes
such as the eyes and throat. This is particularly true of aldehydes.
Unburned hydrocarbons participate (along with NOx and
sunlight) in smog-formation reactions that produce ozone and other
irritants.
Oxides of Nitrogen - The primary oxide of nitrogen
in engine exhaust is nitric oxide, NO. However, after being exhausted,
the NO reacts photochemically with sunlight to produce nitrogen dioxide,
NO2. In diesel exhaust, 10-30% of the NOx may be
emitted directly as NO2. NO is not a strong irritant, but it
binds to hemoglobin in the same manner as CO. NO2 is a
strong irritant of mucous membranes and it also binds to hemoglobin. NO
binds with 1000 times the strength of CO and NO2 binds with
about 1/3 the strength of NO.NO2 is major participant in smog
formation reactions.
Particulates - There is
considerable current controversy about the hazard associated with diesel
particulate. Traditionally, the hazard has been associated with the
hydrocarbon portion of the particulate. This fraction, commonly
referred to as the soluble organic fraction or volatile fraction,
contains high molecular weight polynuclear aromatic hydrocarbons that
are known carcinogens. The usual argument is that soot particles are
inhaled and deposit deep in the lungs where the carcinogens have access
to sensitive tissue. More recent data suggests that
non-hydrocarbon-containing inert particles in the same size range as
diesel particulate may cause similar health problems.
Typical particulate data for diesel fuel, biodiesel, and B20 are shown
in Table 3. While the total particulate matter is the quantity
regulated by the EPA, the data presented here show the various
components that make up the particulate, the volatile organic fraction,
the sulfate and bound water, and the soot.
Table 3. Particulate Matter Composition
|
Test Engine |
Test Fuel |
Particulate Composition - g/hp-hr |
|
VOF |
Sulfate + H2O |
Soot |
Total PM |
|
CumminsN-14 |
B100 |
0.050 |
0.001 |
0.025 |
0.076 |
|
CumminsN-14 |
B20 |
0.046 |
0.005 |
0.051 |
0.102 |
|
CumminsN-14 |
2-D |
0.035 |
0.007 |
0.064 |
0.106 |
|
DDC Series 50 |
B100 |
0.032 |
0.001 |
0.018 |
0.052 |
|
DDC Series 50 |
B20 |
0.033 |
0.007 |
0.048 |
0.088 |
|
DDC Series 50 |
2-D |
0.029 |
0.010 |
0.063 |
0.102 |
|
Cummins B5.9 |
B100 |
0.055 |
0.000 |
0.026 |
0.081 |
|
Cummins B5.9 |
B20 |
0.044 |
0.009 |
0.056 |
0.109 |
|
Cummins B5.9 |
2-D |
0.048 |
0.010 |
0.070 |
0.128 |
The volatile
organic fraction is the portion of the particulate matter that
originates from unburned and partially burned fuel and lubricating oil.
It is determined by placing a particulate sample in a vacuum oven and
baking until all the volatile material has been removed. A similar
quantity is the soluble organic fraction (SOF), which is
determined using a chemical solvent to remove the hydrocarbon fraction.
The sulfate fraction consists of sulfuric acid and related sulfates that
originate from the sulfur in the fuel. These compounds are usually
hygroscopic so they contain an amount of bound water that may be greater
than the weight of sulfate itself. With low sulfur diesel fuels (<
0.05%) the sulfate fraction is usually low. The final fraction is the
soot. The soot consists mainly of carbon with small amounts of
hydrogen.
Table 3 shows that biodiesel causes substantial
reductions in the soot fraction of the particulate. The reduction
varied between 61 and 71%. However, this is offset by an increase in
the VOF that varied between 4.5 and 43%. The soot reduction is still
not completely understood but is most likely due to the presence of the
oxygen in the fuel decreasing the formation of soot in the
high-temperature, fuel-rich portions of the fuel spray. The mechanism
for the increase in VOF is also not understood but is probably
associated with the low volatility of the biodiesel allowing some of the
fuel to survive the combustion process as small droplets.
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