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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 />

BORE,mm= 60<br />

STR0KE,mm= 60<br />

C0N-R0D,mm= 110<br />

EXHAUST 0PENS,eatdc= 100<br />

TRANSFER 0PENS,2atdc= 120<br />

INLET 0PENS,2btdc= 65<br />

TRAP COMPRESSION RATI0= 7<br />

SQUISH CLEARANCE,mm= 1.5<br />

WRIST PIN-CROWN,mm= 25<br />

WRIST PIN-SKIRT,mm= 25<br />

DEFLECTOR HEIGHT,mm= 18<br />

SWEPT V0LUME,cm3= 169.6<br />

TRAP 5WEPT V0LUHE,Cm3=l 1 1<br />

CLEARANCE V0LUME,cm3= 18.5 165.0<br />

Fig. 1.13 Example <strong>of</strong> a calculation from Prog. 1.3, QUB CROSS ENGINE DRAW.<br />

143.7<br />

pression <strong>and</strong> expansion strokes, reducing both power output <strong>and</strong> fuel economy. Therefore, the<br />

QUB-type engine has enhanced engine reliability <strong>and</strong> efficiency in this regard over the life<br />

span <strong>of</strong> the power unit.<br />

The data values used for the basic engine geometry in Figs. 1.10-1.13 are common for all<br />

three program examples, so it is useful to compare the actual data output values for similarities<br />

<strong>and</strong> differences. For example, it can be seen that the QUB cross-scavenged engine is<br />

taller to the top <strong>of</strong> the deflector, yet is the same height to the top <strong>of</strong> the combustion chamber<br />

as the loop-scavenged power unit. In a later chapter, Fig. 4.13 shows a series <strong>of</strong> engines which<br />

are drawn to scale <strong>and</strong> the view expressed above can be seen to be accurate from that comparative<br />

sketch. Indeed, it could be argued that a QUB deflector engine can be designed to be<br />

a shorter engine overall than an equivalent loop-scavenged unit with the same bore, stroke<br />

<strong>and</strong> rod lengths.<br />

1.5 Definitions <strong>of</strong> thermodynamic terms used in connection with engine design <strong>and</strong><br />

testing<br />

1.5.1 Scavenge ratio <strong>and</strong> delivery ratio<br />

In Fig. 1.1(c), the cylinder has just experienced a scavenge process in which a mass <strong>of</strong><br />

fresh charge, mas, has been supplied through the crankcase from the atmosphere. By measuring<br />

the atmospheric, i.e., the ambient pressure <strong>and</strong> temperature, pat <strong>and</strong> Tat, the air density<br />

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