15.02.2013 Views

Design and Simulation of Two Stroke Engines

Design and Simulation of Two Stroke Engines

Design and Simulation of Two Stroke Engines

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Chapter 4 - Combustion in <strong>Two</strong>-<strong>Stroke</strong> <strong>Engines</strong><br />

as declared earlier, the fuel for the spark-ignition engine is octane <strong>and</strong> dodecane for a diesel<br />

unit. The real situation is more complex than that, as Table 4.1 shows. The properties are the<br />

hydrogen to carbon molecular ratio, H/C (or n as seen in the chemical relationship CHn), the<br />

lower calorific value, Cfl, the specific gravity, <strong>and</strong> the latent heat <strong>of</strong> vaporization <strong>of</strong> the fuel,<br />

hvap-<br />

FUEL<br />

H/C ratio, n<br />

Cf|, MJ/kg<br />

Specific gravity<br />

hvap, kJ/kg<br />

Table 4.1 Properties <strong>of</strong> some fuels used in engines<br />

C 8 H 18<br />

2.25<br />

44.79<br />

0.70<br />

400<br />

C 12 H 26<br />

2.17<br />

43.5<br />

0.75<br />

425<br />

SU Gasoline<br />

1.65<br />

43.0<br />

0.76<br />

420<br />

Auto Diesel<br />

1.81<br />

43.3<br />

0.83<br />

450<br />

The tabular values show the typical properties <strong>of</strong> iso-octane, CsHis, <strong>and</strong> dodecane, Ci2H26-<br />

The values in the table for gasoline, labeled as SU or "super-unleaded" gasoline <strong>and</strong> for diesel<br />

fuel, labeled as "auto" diesel, are reasonably representative <strong>of</strong> the typical properties <strong>of</strong> fuels<br />

commercially available. The properties <strong>of</strong> such fuels are very dependent on the refining process<br />

which will vary from country to country, from refinery to refinery, <strong>and</strong> from the constituents<br />

<strong>and</strong> origins <strong>of</strong> the crude oil source for that particular fuel.<br />

4.3.2 Properties <strong>of</strong> exhaust gas <strong>and</strong> combustion products<br />

Sec. 2.1.6 shows the basic theory for the computation <strong>of</strong> the properties <strong>of</strong> a mixture <strong>of</strong><br />

gases. The example chosen is the stoichiometric combustion <strong>of</strong> octane. This continued in the<br />

introduction given in Sec. 1.5.5. In both these examples, stoichiometric, or chemically <strong>and</strong><br />

ideally exact, combustion was used <strong>and</strong> so all carbon burned to carbon dioxide <strong>and</strong> carbon<br />

monoxide was not formed. In all real combustion processes, dissociation takes place at elevated<br />

temperatures <strong>and</strong> pressures so that, even at stoichiometry, free carbon monoxide <strong>and</strong><br />

free hydrogen will be created. There are two principal dissociation reactions involved <strong>and</strong><br />

they are:<br />

C02 CO + -j-02<br />

H20 + CO H2 + C02<br />

(431)<br />

(4.3.2)<br />

The latter equation is <strong>of</strong>ten known as the "water-gas" reaction. The combustion equation<br />

that includes all <strong>of</strong> these effects, <strong>and</strong> for all air-fuel ratios with a generic hydrocarbon fuel<br />

CHn, is then completely stated as:<br />

CHn + *.m(02 + kN2)<br />

= XjCO + x2C02 + x3H20 + x402 + x5H2 + x6N2<br />

297<br />

(4.3.3)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!