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Tutorials Manual

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Chapter 2: Combustion in Gas-phase Processes<br />

<strong>Tutorials</strong> <strong>Manual</strong><br />

valve close (IVC) time of our test engine is 142 degrees (crank angle) before TDC<br />

(BTDC). Accordingly, we should set our simulation starting crank angle to<br />

-142 degrees. We let the simulation run for 0.043 sec or for 257 degrees crank angle<br />

to 115 degrees after TDC. The gas mixture pressure and temperature at IVC are<br />

107911 Pa (or 1.065 atm) and 447 K, respectively. The composition of the initial gas<br />

mixture is a combination of natural gas, air, and EGR gas and is given in Table 2-8.<br />

Table 2-8<br />

Species<br />

Composition of Initial Gas Mixture<br />

Mole Fraction<br />

CH4 0.0350<br />

C2H6 0.0018<br />

C3H8 0.0012<br />

O2 0.1824<br />

CO2 0.0326<br />

H2O 0.0609<br />

N2 0.6861<br />

The project file for this HCCI engine simulation problem is called<br />

ic_engine__hcci_heat_loss_methane.ckprj and is located in the samples41<br />

directory. This project file actually contains two “sub-projects”: the<br />

ic_engine__hcci_adiabatic project assumes the cylinder is adiabatic and the other<br />

project, ic_engine__hcci_heat_loss_woschni, considers heat loss through the<br />

cylinder wall. By default CHEMKIN will append the new project to an existing project file<br />

if the name of the new project is different from the ones already saved in the file.<br />

Therefore, we can group similar projects into the same project file by saving those<br />

projects one by one to the same project filename.<br />

Heat transfer between the gas mixture inside the cylinder and the cylinder wall can be<br />

specified on the Reactor Physical Properties panel. For the adiabatic case, no heat<br />

transfer occurs between the gas and the wall. We can simply leave the text box<br />

corresponding to the heat loss entry blank because the heat loss value is set to zero<br />

by default. For non-adiabatic cases, we have several ways to describe the heat loss<br />

to the wall: a constant heat transfer rate (positive for heat loss to environment), a<br />

piecewise heat transfer rate profile, a user subroutine, or a heat transfer correlation.<br />

Here we choose the heat-transfer correlation for our HCCI problem. We also apply<br />

the Woschni correction 14 to get better estimates of gas velocity inside the cylinder.<br />

14. J. B. Heywood, Internal Combustion Engines Fundamentals, McGraw-Hill Science/Engineering/Math,<br />

New York, 1988.<br />

RD0411-C20-000-001 51 © 2007 Reaction Design

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