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Modern Engineering Thermodynamics

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ðn i /n fuel Þðc pi Þ E system<br />

Summary 643<br />

The often complex formulae of chemical thermodynamics provide an excellent topic for personal computer software<br />

development. In this chapter, simple Excel spreadsheet programs are developed for calculating heats of<br />

combustion and dissociation equilibrium conditions. The reader is encouraged to utilize and modify this material,<br />

to take full advantage of the computer’s ability to remove the tedium of calculation and expand the scope<br />

of the analysis.<br />

Some of the more important equations introduced in this chapter follow. Do not attempt to use them blindly<br />

without understanding their limitations. Please refer to the text material where they were introduced to gain an<br />

understanding of their use and limitations.<br />

1. Air/fuel ratio. For a chemical reaction combustion equation of the form<br />

αðFuelÞ + βðO 2 + 3:76 N 2 Þ!Products<br />

the molar and mass air/fuel ratios are<br />

αð1 + 3:76Þ<br />

ðA/FÞ molar<br />

= = αð4:76Þ<br />

β<br />

β<br />

ðA/FÞ mass = αð4:76ÞðM airÞ<br />

= αð4:76Þð28:97Þ = αð137:9Þ<br />

βðM fuel Þ βðM fuel Þ βðM fuel Þ<br />

where α and β are the stoichiometric coefficients in the reaction equation, and M fuel is the molecular mass of<br />

the fuel.<br />

2. Stoichiometric reaction equation for the combustion of a hydrocarbon of the form C n H m in 100%<br />

theoretical air:<br />

<br />

C n H m + n + m <br />

<br />

½O 2 + 3:76ðN 2 ÞŠ6nðCO 2 Þ + m <br />

<br />

ðH 2 OÞ + 3:76 n + m <br />

ðN 2 Þ<br />

4<br />

2<br />

4<br />

3. The temperature at which water condenses out of the products of combustion:<br />

T condense = T sat ðp H2 OÞ<br />

where p H 2O = (χ H 2O/χ total )p total is the partial pressure of the water vapor in the products.<br />

4. The standard reference state (SRS):<br />

Temperature: T SRS = T° =25:0°C = 298 K = 77:0°F = 537 R<br />

Pressure: p SRS = p° =0:100 MPa = 14:5 psia ≈ 1 atmosphere<br />

5. Molar specific heat of formation of a hydrocarbon C n H m in MJ/kgmole:<br />

ðq f °Þ CnH m<br />

= − ½nð393:5Þ + ðm/2Þð285:5Þ + HHV Cn H m<br />

Š<br />

6. Molar specific enthalpy of formation of a compound at the standard reference state is the same as its molar<br />

specific heat of formation:<br />

ðh f<br />

°Þ compound = ðq f °Þ compound<br />

7. Molar heat of reaction:<br />

q r = ∑ðn i /n fuel Þh i −∑ðn i /n fuel Þh i<br />

P<br />

R<br />

8. Higher and lower heating values of a fuel:<br />

HHV = q r ðSRS and H 2 O in the liquid stateÞ<br />

LHV = q r ðSRS and H 2 O in the vapor stateÞ<br />

9. Open and closed system adiabatic flame temperature:<br />

ðT A Þ open<br />

= T°+<br />

ðh f<br />

°Þ fuel<br />

−∑ðn i /n fuel Þðh f<br />

°Þ i<br />

P<br />

∑<br />

P

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