first law analysis for reacting system consider a constant pressure process in which n f moles of...

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First Law Analysis for Reacting System er a constant pressure process in which n f moles of fuel react s of air to produce n p moles of product: P n A n F n p a f ng First Law with state 1 being the reactants at P 1 , T 1 and st products at P 2 , T 2 : Reactants Products Reactants Products Reaction State 1 State 2 Q W ) ( ) ( 1 2 1 2 2 1 V V P U U Q W U Q

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Page 1: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

First Law Analysis for Reacting System

Consider a constant pressure process in which nf moles of fuel react withna moles of air to produce np moles of product:

PnAnFn paf

Applying First Law with state 1 being the reactants at P1, T1 and state 2being products at P2, T2:

Reactants Products

ReactantsProducts

Reaction

State 1 State 2

Q

W

)()( 121221 VVPUUQ

WUQ

Page 2: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

RRii

PpiiRP ThnThnHH

HH

VPUVPU

)()(

)()(

12

111222

HP < HR Q < 0 exothermic reaction

HP > HR Q > 0 endothermic reaction

)()( 1212 VVPUUQ

First Law Analysis for Reacting System

Page 3: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

Enthalpy of Reaction

Consider the case where the final temperature of the products is the same as the initial temperature of the reactants (e.g., calorimeter is used to measure Q).

ReactionQ

W

P1=P2=Po

T1=T2=To

The heat released under this situation is referred to as the enthalpy of reaction, HR ,

fuel of kmolor kgper kJ :units )()(

)()(

Roii

Poii

RRii

PpiiR

ThnThn

ThnThnH

To

Page 4: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

The maximum amount of energy is released from a fuel when reacted with astoichiometric amount of air and all the hydrogen and carbon contained in thefuel is converted to CO2 and H2O

This maximum energy is referred to as the heat of combustion or the heating value and it is typically given per mass of fuel

Heat of Combustion

22222 476.3

2)76.3(

4NOHCONOHC

HR(298K)

Page 5: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

Heat of Combustion

There are two possible values for the heat of combustion that can be calculated depending on whether the water in the products is taken to be in a liquid or vapour state.

Tp

T

S

hghf

From steam tables: hfg = hg – hf > 0

HR = HP – HR < 0 (exothermic)

The term higher heat of combustion is used when the water in the products is taken to be in the liquid state

The term lower heat of combustion is used when the water in the productsis taken to be in the vapour state

Page 6: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

Heat of FormationConsider the following reactions taking place at atmospheric pressure andwith TP = TR = 298K

222

2222

/ 000,394 )()()(

/ 000,286 )()()(2/1

COkmolkJQgCOgOsC

OHkmolkJQlOHgHgO

In these reactions H2O and CO2 are formed from their elements in theirnatural state at standard temperature and pressure (STP) 1 atm and 298K.

Reactions of this type are called formation reactions and the corresponding measured heat release Q is referred to as the standard heat of formationand takes the symbol so:

ofh

kmolkJh

kmolkJh

C

O

/ 000,394

/ 000,286

oO f,

oH f,

2

2

Values for standard heat of formation for different species are tabulated

Page 7: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

Enthalpy Scale for a Reacting System

By international convention, the enthalpy of every element in its natural state(e.g., O2(g), N2(g), H2(g), C(s)) at STP has been set to zero

0)298,1( ohKatmh

We need to take into account that for a reacting system the working fluid changes molecularly from reactants to products while undergoing a process.

Consider the following identity:

)]298,1(),([)298,1(),( KatmhTPhKatmhTPh

(note the notation convention)

at STP

Page 8: First Law Analysis for Reacting System Consider a constant pressure process in which n f moles of fuel react with n a moles of air to produce n p moles

The enthalpy of all other substances at STP is simply the heat of formation of the substance, since it is formed from its elements, for example:

)]298,1(),([ ),( , KatmhTPhhTPh iio

ifi

sensible enthalpychemical enthalpy TK ip dTc298 ,

Therefore, the enthalpy of the i’th component in a mixture is:

Enthalpy Scale for a Reacting System

)(,)(

)(,)()()(

222

22

2222

2/1 @

)()()(2/1

lOHflOH

lOHfgHgOlOH

hh

hhhhQSTPrecall

lOHgHgO

The sensible enthalpy for different species is tabulated as a function of temperature (JANNAF Tables).