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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.

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