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Design and Simulation of Two Stroke Engines

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<strong>Design</strong> <strong>and</strong> <strong>Simulation</strong> <strong>of</strong> <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

1.5.2 Scavenging efficiency <strong>and</strong> purity<br />

In Chapter 3 it will be shown that for a perfect scavenge process, the very best which<br />

could be hoped for is that the scavenging efficiency, SE, would be equal to the scavenge ratio,<br />

SR. The scavenging efficiency is defined as the mass <strong>of</strong> delivered air that has been trapped,<br />

mtas, by comparison with the total mass <strong>of</strong> charge, mtr, that is retained at exhaust closure. The<br />

trapped charge is composed only <strong>of</strong> fresh charge trapped, mtas, <strong>and</strong> exhaust gas, meX, <strong>and</strong> any<br />

air remaining unburned from the previous cycle, mar, where:<br />

m tr = m tas + m ex + m ar<br />

(L5,8)<br />

Hence, scavenging efficiency, SE, defines the effectiveness <strong>of</strong> the scavenging process, as<br />

can be seen from the following statement:<br />

SE = mtas = m tas (1.5.9)<br />

mtr<br />

mtas + mex + mar<br />

However, the ensuing combustion process will take place between all <strong>of</strong> the air in the<br />

cylinder with all <strong>of</strong> the fuel supplied to that cylinder, <strong>and</strong> it is important to define the purity <strong>of</strong><br />

the trapped charge in its entirety. The purity <strong>of</strong> the trapped charge, n, is defined as the ratio <strong>of</strong><br />

air trapped in the cylinder before combustion, mta, to the total mass <strong>of</strong> cylinder charge, where:<br />

m ta =m tas +m ar (1.5.10)<br />

n = - m ^- (1.5.H)<br />

mtr<br />

In many technical papers <strong>and</strong> textbooks on two-stroke engines, the words "scavenging<br />

efficiency" <strong>and</strong> "purity" are somewhat carelessly interchanged by the authors, assuming prior<br />

knowledge by the readers. They assume that the value <strong>of</strong> mar is zero, which is generally true<br />

for most spark-ignition engines <strong>and</strong> particularly when the combustion process is rich <strong>of</strong><br />

stoichiometric, but it would not be true for two-stroke diesel engines where the air is never<br />

totally consumed in the combustion process, <strong>and</strong> it would not be true for similar reasons for a<br />

stratified combustion process in a gasoline-fueled spark-ignition engine. More is written on<br />

this subject in Sees. 1.5.5 <strong>and</strong> 1.6.3 where stoichiometry <strong>and</strong> trapping efficiency measurements<br />

are debated, respectively.<br />

1.5.3 Trapping efficiency<br />

Definitions are also to be found in the literature [1.24] for trapping efficiency, TE. Trapping<br />

efficiency is the capture ratio <strong>of</strong> mass <strong>of</strong> delivered air that has been trapped, mtas, to that<br />

supplied, mas, or:<br />

TE = -^1 (1.5.12)<br />

28<br />

mQC

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