• Non ci sono risultati.

 Adiabatic flame temperature

N/A
N/A
Protected

Academic year: 2021

Condividi " Adiabatic flame temperature"

Copied!
4
0
0

Testo completo

(1)

Adiabatic flame temperature

1. Estimate the constant-pressure adiabatic flame temperature for the combustion of a stoichiometric C3H8–air mixture. The pressure is 1 bar and the initial reactant temperature is 298 K. Use the following assumptions:

 “Complete combustion”, i.e., the product mixture consists only of CO2, H2O, and N2.

 The enthalpy of the product mixture is estimated using constant specific heats evaluated at 1200 K  (Ti + Tad)/2, where Tad is guessed to be about 2100 K.

2. Under the same assumptions, but obviously considering excess O2 in the products, estimate the adiabatic flame temperature for a C3H8–air mixture with equivalence ratio = 0.8.

--- Answers

1.

The mixture composition follows from balancing the chemical equation for a stoichiometric mixture of propane and air:

3 8 2 2 2 2 2

C H 5 O 3.76N 3CO 4H O+18.58N where in the product mixture we find

2 2 2

CO 3, H O=4, N =18.58

N N N

Properties:

Species Enthalpy of formation at 298.15 K

0 ,

hf i (kJ/kmol)

Specific Heat at 1200 K

,

cp i (kJ/kmol-K)

C3H8 –103847 (Table B.1, Turns’ textbook)

CO2 –393546 (Table A.2) 56.21 (Table A.2)

H2O –241845 (Table A.6) 43.87 (Table A.6)

N2 0 33.71 (Table A.7)

O2 0

By applying the first law of thermodynamics:

react prod

react prod

= =

i i i i

H N h HN h

      

3 8

react

C H

1 103847 5 0 18.58 0 103847 kJ/mol

H

 

(2)

 

 

3 8

0

prod , ,

prod

C H

298.15 3 393546 56.21 298.15 4 241845 43.87 298.15

18.58 0 33.71 298.15 kJ/mol .

i f i p i ad

ad ad ad

H N h c T

T T T

Equating (first law) Hreactto Hprodand solving for Tad yields

Tad = 2404 K for  1 (stoichiometric conditions)

Another way is:

0

react ,

react react

(in our case)

i i i f i

H N h N h

0

prod , ,

prod prod

i f i ad 298 i p i

H N h T N c

If we define, on a one-mole-of-fuel basis, the enthalpy of reaction HR0 and the average heat capacity Cp of the product mixture, respectively as:

0 0 0

, ,

prod react

R i f i i f i

H N h N h

; ,

prod

p i p i

C N c then we have

0

298.15 R

ad

p

T H

C

 .

Thus,

  3 8

0

3 393546 4 241845 103847 2044171 kJ/molC H

HR

         

C H3 8

3 56.21 4 43.87 18.58 33.71 970.4 kJ/mol K

Cp    

then

2044171 K

298.15

9 . 2404

ad 70 4

T  

.

2.

In this case, the mixture composition follows from balancing the chemical equation for a mixture of propane and air, with excess air. Suppose that we provide 4.76a moles of air, with a>5 (5 is the value for a stoichiometric mixture). We can write the species balance as:

(3)

3 8 2 2 2 2 2 2

C H a O 3.76N 3CO 4H O 3.76 N a bO

where a and b must be computed from the knowledge of the equivalence ratio. From the definition of the equivalence ratio  we can compute the value of a:

stoic

stoic

A F F A

A F F A

 

where

4.76

1

air stoic air

stoic

fuel stoic fuel

m a MW

A F m MW

; 4.76

1

air air

fuel fuel

m a MW

A F m MW

hence

0.8 5 6.25

0.8 0.8

stoic stoic

a a

a a

From the balance of oxygen atoms (or by simply observing that b a a  stoic) we find 2 3 2 4 1 2

a      b that is

5 1.25 b a   . We can now rewrite the species balance for  0.8:

3 8 2 2 2 2 2 2

C H 6.25 O 3.76N 3CO 4H O 1.25O 23.5N

where in the products we find

2 2 2 2

CO 3, H O=4, N =23.5, O =1.25

N N N N

In addition to the property values used in a.1, we need the Specific Heat at 1200 K for O2 : Species Enthalpy of formation at 298.15 K

0 ,

hf i (kJ/kmol)

Specific Heat at 1200 K

,

cp i (kJ/kmol-K)

O2 0 35.593 (Table A.11)

By applying the first law: react prod

react prod

= =

i i i i

H N h HN h react   1 103847 6.25 0  23.5 0 

103847 kJ

H

 

(4)

 

 

0

prod , ,

prod

298.15

3 393546 56.21 298.15 4 241845 43.87 298.15 23.5 0 33.71 298.15 1.25 0 35.59 298.15

3 393546 4 241845

3 56.21 4 43.87 23.5 33.71 1.25 3

i f i p i ad

ad ad ad ad

H N h c T

T T T T

    

   

5.59 298.15 3 56.21 4 43.87 23.5 33.71 1.25 35.59 Tad

   

that is:

Equating Hreactto Hprodand solving for Tad yields

103847 kJ 3 393546 4 241845

3 56.21 4 43.87 23.5 33.71 1.25 35.59 298.15 3 56.21 4 43.87 23.5 33.71 1.25 35.59 Tad

    

   

   

103847 3 393546 4 241845 298.15

3 56.21 4 43.87 23.5 33.71 1.25 35.59 2044171

298.15 2029

1180.78 Tad

K

   

 

Tad = 2029 K for  0.8

Riferimenti

Documenti correlati

We need also the following two identities... and the proof of (1)

[r]

[r]

[r]

1.4 hxq RN Assumption 1.4 already appears in [2, condition 1.4 of the existence Theorem 1.1] for positive solutions of semilinear elliptic Dirichlet problems in bounded domains and

In this paper, we consider smooth hypersurfaces X ⊂ P n+1 of sufficiently large degree, and we are interested in the existence of irreducible curves C ⊂ X having low gonality

1. Estimate the constant-pressure adiabatic flame temperature for the combustion of a stoichiometric CH 4 –air mixture. Under the same assumptions, but obviously considering

Chi  l’avrebbe  mai  detto,  pare  ci  sia  un  concetto  heideggeriano