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Design and Simulation of Two Stroke Engines

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INFLOW<br />

mass dm|<br />

enthalpy dH|<br />

airdlli<br />

Chapter 2 - Gas Flow through <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

CYLINDER<br />

mass mc<br />

energy Uc<br />

purity nc<br />

pressure Pc<br />

temperature Tc<br />

volume VQ<br />

dVC<br />

mass dm£<br />

enthalpy dHg<br />

airdllE<br />

Fig. 2.25 The thermodynamics <strong>of</strong> open cycle flow through a cylinder.<br />

toward the cylinder. All ports <strong>and</strong> valves experience backflow at some point during the open<br />

cycle. The words "inflow" <strong>and</strong> "outflow" are, in the case <strong>of</strong> an engine cylinder, a convenient<br />

method <strong>of</strong> denoting ports <strong>and</strong> valves whose nominal job is to supply air into the cylinder <strong>of</strong> an<br />

engine. When dealing with an intake plenum, or an exhaust silencer box, "inflow" <strong>and</strong> "outflow"<br />

become a directionality denoted at the whim <strong>of</strong> the modeler; but having made a decision<br />

on the matter, the ensuing sign convention must be adhered to rigidly. The sign convention,<br />

common in engineering thermodynamics, is that inflow is "positive" <strong>and</strong> that outflow is<br />

also "positive"; this sign convention is employed not only in the theory below, but throughout<br />

this text. Backflow, by definition, is opposite to that which is decreed as positive <strong>and</strong> is then<br />

a negative quantity. The mesh computation must then reorient in sign terms the numerical<br />

values for the right- <strong>and</strong> left-h<strong>and</strong> ends <strong>of</strong> pipes during inflow <strong>and</strong> outflow boundary calculations<br />

as appropriate to those junctions defined as "inflow" or "outflow" at the cylinders or<br />

plenums. While the computer s<strong>of</strong>tware logic for this is trivial, care must be taken not to<br />

confuse the thermodynamic needs <strong>of</strong> the mesh spaces defined in Sec. 2.18.9 with those <strong>of</strong> the<br />

cylinder or plenum being examined here.<br />

Heat transfer is defined as positive for heat added to a system <strong>and</strong> work out is also a<br />

positive action. Employing this convention, the First Law <strong>of</strong> Thermodynamics reads as:<br />

heat transfer + energy in = change <strong>of</strong> system state + energy out + work done<br />

The entire computation at this stage makes the assumption that the previous application<br />

<strong>of</strong> the boundary conditions, using the theory <strong>of</strong> Sees. 2.16 <strong>and</strong> 2.17, has produced the correct<br />

values <strong>of</strong> the terms dmi, dHi, dPi, diriE, dHg <strong>and</strong> dP£. To reinforce an important point which<br />

has been made before, during the application <strong>of</strong> the boundary conditions in the case <strong>of</strong> a<br />

163

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