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Modern Engineering Thermodynamics

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15.8 Adiabatic Flame Temperature 615<br />

EXAMPLE 15.10<br />

For liquid octane, C 8 H 18 ðÞ, l determine the following adiabatic flame temperatures when the reactants are in the standard<br />

reference state (25°C and 0.100 MPa) and the combustion products are assumed to be ideal gases:<br />

a. The open system (constant pressure) adiabatic flame temperature burning with 100.% theoretical air.<br />

b. The open system (constant pressure) adiabatic flame temperature burning with 200.% theoretical air.<br />

c. The closed system (constant volume) adiabatic flame temperature burning with 100.% theoretical air.<br />

Solution<br />

a. The combustion equation for octane burning with 100.% theoretical air is<br />

C 8 H 18 + 12:5 O 2 + 3:76ðN 2 Þ ! 8CO ð 2 Þ+ 9H ð 2 OÞ+ 47ðN 2 Þ<br />

Since the products can be considered to be ideal gases, we can use Eq. (15.17) and the average specific heat values given<br />

in Table 15.5. From Table 15.1, we find,<br />

and<br />

h° f fuel = h° f = −249:952 MJ/kgmole<br />

C8H18ðlÞ<br />

h° f = −393:522 MJ/kgmole<br />

CO2<br />

h° f = −241:827 MJ/kgmole<br />

H2OðgÞ<br />

h f ° N 2 = 0 because it is an element<br />

The open system constant pressure adiabatic flame temperature is given by Eq. (15.17), where<br />

∑<br />

P<br />

ðn i /n fuel Þ h° f = 8 h° i f + 9 h° f CO2 H2O + 47 h° f N2<br />

= 8ð−393:522Þ+ 9ð−241:827Þ+ 47ð0Þ<br />

= −5325 MJ/kgmole of C 8 H 18<br />

and<br />

∑<br />

P<br />

<br />

ðn i /n fuel Þ c pi avg = 8 c p<br />

CO2<br />

avg + 9 <br />

c p<br />

H2O<br />

avg + 47 c p<br />

<br />

<br />

N2 avg<br />

= 80:05818 ð Þ+ 90:04250 ð Þ+ 47ð0:03118Þ<br />

= 2:313 MJ/ ðkgmole of C 8 H 18 Þ . K <br />

Then, Eq. (15.17) gives<br />

T A<br />

= 25:0°C + open<br />

system<br />

b. The reaction equation when 200.% theoretical air is used is<br />

−249:952 MJ/kgmole fuel − ð −5325 MJ/kgmole fuel Þ<br />

2:313 MJ/ðkgmole fuel .<br />

= 2170°C = 3940°F<br />

KÞ<br />

C 8 H 18 + 212:5 ð Þ O 2 + 3:76 N 2<br />

ð Þ ! 8CO ð 2<br />

Þ+ 9H ð 2 OÞ+ 12:5 O 2<br />

ð Þ+ 94ðN 2 Þ<br />

The numerator in Eq. (15.17) is the same here as it was in part a, since we only added more elements to the reaction<br />

side of the equation. The denominator represents the energy required to raise the temperature of all the product gases<br />

and is consequently different from part a. In this case,<br />

∑<br />

P<br />

Then, Eq. (15.17) gives<br />

<br />

ðn i /n fuel Þ c pi avg = 8 c p<br />

CO2<br />

avg + 9 <br />

c p<br />

T A<br />

= open<br />

system<br />

200% TA<br />

H2O<br />

avg + 12:5 c p<br />

<br />

O2<br />

avg + 94 c p<br />

<br />

<br />

N2 avg<br />

= 80:05818 ð Þ+ 90:04250 ð Þ+ 12:5ð0:03299Þ+ 94ð0:03118Þ<br />

= 4:19 MJ/ ðkgmole of C 8 H 18 Þ . K <br />

−249:952 − ð−5325Þ<br />

4:19<br />

+ 25:0 = 1240°C = 2260°F<br />

(Continued )

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