Troels Dyhr Pedersen.indd - Solid Mechanics
Troels Dyhr Pedersen.indd - Solid Mechanics
Troels Dyhr Pedersen.indd - Solid Mechanics
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DESCRIPTION OF THE EXPERIMENT<br />
OBJECTIVE<br />
The goal of this study was to determine the<br />
influence of compression ratio (CR) and engine<br />
speed on HCCI combustion of DME at selected<br />
excess air ratios.<br />
MOTIVATION<br />
The primary motive for investigating HCCI<br />
combustion of DME is that of avoiding highpressure<br />
pumps and injectors. As DME has a very<br />
low lubricity, pumps and injectors are susceptible to<br />
rapid wear. If DME can be introduced with a low<br />
pressure nozzle instead, these problems are<br />
avoided.<br />
Prior experiments have shown that the combustion<br />
of pure DME in the HCCI process necessitates a<br />
careful choice of CR to achieve the best possible<br />
result, e.g. a high IMEP and indicated efficiency. It<br />
is also of interest to investigate the influence of<br />
engine speed on the combustion process. Higher<br />
engine speeds may improve the characteristics of<br />
the combustion, which may be of interest in smaller<br />
engines.<br />
EXPERIMENTAL OUTLINE<br />
Excess air ratios<br />
From earlier experiments it was found that the<br />
richest mixture that could be used without<br />
excessive knock would be an excess air ratio<br />
(lambda) of 2.5. It was also found that compression<br />
ignition of mixtures leaner than the excess air ratio<br />
of 4 required a high compression ratio of about 12-<br />
14, and that such lean mixtures cannot produce<br />
sufficient torque to keep an engine running except<br />
for idle conditions.<br />
Three different excess air ratios were chosen to<br />
represent the rich limit (lambda 2.5), the lean limit<br />
(lambda 4) and a value in between (lambda 3). As<br />
keeping an equivalence ratio constant can be a<br />
challenge when air flow changes, three constant<br />
values of fuel mass per cycle were used instead.<br />
The three values are however referred to as<br />
lambda 2.5, 3 or 4 in the text and figures.<br />
Variation of engine speed<br />
The HCCI combustion is a premixed and<br />
homogeneous combustion which is mainly<br />
governed by chemical kinetics. The reactions<br />
therefore occur very fast compared to DI CI<br />
engines and SI engines, but may still be affected by<br />
engine speed.<br />
It is well known that higher engine speeds lead to a<br />
more adiabatic compression of the mixture, but also<br />
increases the heat flux from the combustion<br />
chamber and therefore results in higher in-cylinder<br />
temperatures.<br />
To investigate the possible effects of engine speed<br />
on the combustion event and engine performance,<br />
an interval of engine speed comparable to that of a<br />
medium duty engine has been chosen. To avoid<br />
excessive amounts of data, the fixed engine<br />
speeds used were 1000, 2000 and 3000 RPM.<br />
Variation of compression ratio<br />
The CR has been varied from 8.8 to 12.8 in steps<br />
of 0.2. The purpose was to accurately determine<br />
the range of CR necessary to achieve satisfactory<br />
engine performance within the desired range of<br />
excess air ratios and engine speeds.<br />
Determining the usable interval of compression<br />
ratio at different engine speeds and equivalence<br />
ratios<br />
In this study, the lowest acceptable compression<br />
ratio is found at the point where the engine is<br />
capable of self-sustaining combustion. It was<br />
necessary to preheat the inlet air at the lowest<br />
compression ratios to initiate HCCI combustion, but<br />
if combustion did not proceed after preheating was<br />
removed, the operating point was not considered<br />
valid.<br />
With lambda 4 it was however difficult to determine<br />
whether HCCI combustion was completed while the<br />
CR was in the lower end. To determine if<br />
combustion was satisfactory, the amounts of CO2<br />
and CO were monitored to determine if the<br />
combustion efficiency was satisfactory. It turned out<br />
that the combustion resulted in higher amounts of<br />
CO than CO2 until the CR was raised enough to<br />
complete the final CO oxidation. A figure displaying<br />
emissions of CO and CO2 is found in the results<br />
section.<br />
At the higher engine speeds it was more difficult to<br />
initiate HCCI combustion of the leaner mixtures<br />
lambda 3 and 4. As preheating the air could not<br />
effectively solve this problem, preheating was done<br />
by running the engine with the rich mixture for a<br />
short time before shifting to the leaner mixture. If<br />
the compression ratio was adequate the<br />
combustion would continue and stabilize; otherwise<br />
it would only continue for a short while before<br />
entering a mode of partial combustion.<br />
The highest acceptable compression ratio is found<br />
at the point at which no further improvement in<br />
performance is achieved. While it is difficult to<br />
determine this limit during the experiment, it is clear<br />
from the results that IMEP as well as indicated<br />
efficiency peaks at the optimum compression ratio<br />
and then decreases as compression is further<br />
increased. This happens fast with lambda 2.5, while<br />
lambda 4 benefits from a higher compression ratio<br />
than the lowest acceptable.<br />
While the intensity of knock or pressure rise rate is<br />
sometimes used as a subjective limit of operation,<br />
this limit is not used in this study as it is desired to<br />
show the amplitude of engine knock when<br />
operating limits are exceeded.