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Design and Simulation of Two Stroke Engines

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4 -i<br />

3 -<br />

LU<br />

CC<br />

D 2<br />

CO '<br />

CO<br />

LU<br />

CC<br />

-1<br />

0 -<br />

1.17<br />

PV =K<br />

EXPERIMENTAL DATA<br />

TDC<br />

_U<br />

Chapter 1 - Introduction to the <strong>Two</strong>-<strong>Stroke</strong> Engine<br />

EXPERIMENTAL DATA<br />

THEORETICAL CYCLE<br />

BDC<br />

3 4 5 6 7<br />

LOG(VOLUME)<br />

Fig. 1.15 Logarithmic plot <strong>of</strong> pressure <strong>and</strong> volume.<br />

the actual compression process clearly begins before the <strong>of</strong>ficial trapping point at exhaust<br />

port closure, <strong>and</strong> this in an engine with no tuned exhaust pipe. The theoretical assumption <strong>of</strong><br />

a constant volume process for the combustion <strong>and</strong> exhaust processes is clearly in error when<br />

the experimental pressure trace is examined. The peak cycle pressures <strong>of</strong> 54 bar calculated<br />

<strong>and</strong> 36 bar measured are demonstrably different. In Chapters 4 <strong>and</strong> 5 a more advanced theoretical<br />

analysis will be seen to approach the measurements more exactly.<br />

The work on the piston during the cycle is ultimately <strong>and</strong> ideally the work delivered to the<br />

crankshaft by the connecting rod. The word "ideal" in thermodynamic terms means that the<br />

friction or other losses, like leakage past the piston, are not taken into consideration in the<br />

statement made above. Therefore, the ideal work produced per cycle (see Eq. 1.5.24) is that<br />

work carried out on the piston by the force, F, created from the gas pressure, p. Work is always<br />

the product <strong>of</strong> force <strong>and</strong> distance, x, moved by that force, so, where A is the piston area:<br />

Work produced per cycle = J Fdx = J pAdx = J pdV<br />

(1.5.24)<br />

Therefore, the work produced for any given engine cycle, in the case <strong>of</strong> a two-stroke<br />

engine for one crankshaft revolution from tdc to tdc, is the cyclic integral <strong>of</strong> the pressurevolume<br />

diagram in the cylinder above the piston. By the same logic, the pumping work required<br />

in the crankcase is the cyclic integral <strong>of</strong> the pressure-volume diagram in the crankcase.<br />

In both cases, this work value is the enclosed area on the pressure-volume diagram, be it a<br />

theoretical cycle or the actual cycle as illustrated in Fig. 1.14. The above statements are<br />

illustrated in Fig. 1.16 for the actual data shown previously in Figs. 1.14 <strong>and</strong> 1.15.<br />

33

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