jf chemistry 1101 2010 basic thermodynamics and kinetics · the standard entropy s 298 0 of a...
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Lecture 8
Entropy and Free Energy:Predicting the direction of spontaneous Predicting the direction of spontaneous
changeThe approach to Chemical equilibrium
Absolute entropy and the third law of thermodynamics
To define the entropy of a compound in absolute terms it is necessaryto define a reference value.We can define a zero of entropy at 0 K.According to the third law of thermodynamics the entropy of a perfectcrystal at T = 0 K is zero.yThe standard entropy S298
0 of a substance is defined as the molar entropyat T = 298 K and 1 bar pressure. Units are J mol-1 K-1. S0
298 values are termed absolute or third law entropies.
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05
04
03
02
01
0298 SSSSSS Δ+Δ+Δ+Δ+Δ=
The entropy of a substance increases on heating.There are sudden increases in entropy on melting at Tm and vaporization at Tb.
When CP,m/T is plotted against T the entropy changes due to heating the solid, liquid andgas are given by the shaded areas.
⎟⎠⎞
⎜⎝⎛+=
KKTCSS mPT 298
/ln,0298
0
Assume that substance remains insame phase between T = 298 K andT.
Standard entropy at temp. T.
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Entropy change in chemical reactions
( ) ( )∑ ∑−=Δ rxSprSS jjr0298
0298
0298 νν
Sum of standard enrropiesof reactants
Sum of standard entropiesof products
Stoichiometric coefficient(from balanced equation)
⎟⎠⎞
⎜⎝⎛Δ+Δ=Δ
KKTCSS mPrTr 298
/ln,0298
0
Reaction entropyAt temp. T
( ) ( )∑∑ −=Δ rxCprCC mPjmPjmP ,,, νν
See Chemistry3 worked example 15.5, p.718. Chemistry3 section 15.4, pp.716-722.
Gibbs Energy Change
We now discuss the way in which the spontaneityof a process may be determined.
Surroundings
Kotz, section 19.5, 19.6pp.871-879.Chemistry3, section 15.5,pp.722-730.
From 2nd law of thermodynamics
J.W. Gibbs, 1839-1903
System( ) ( ) ( )surrSsysStotS Δ+Δ=Δ
Assume process occurs at const.T and P.
( ) ( ) ( )Tsysq
TsurrqsurrS revrev −==Δ
Hence ( ) ( )sysHsysq Prev Δ=Multiplying across by -T( ) ( ) ( ) ( )sysGsysSTsysHtotST Δ=Δ−Δ=Δ−Hence ( ) ( )
( ) ( )TsysHsurrS
yyq Prev
Δ−=Δ
,
Now 2nd law thermodynamics implies that
( ) ( ) ( ) 0>Δ+Δ=Δ surrSsysStotS
( ) ( ) ( )TsysHsysStotS Δ
−Δ=Δ
( ) ( ) ( ) ( )sysGsysSTsysHtotST Δ=ΔΔ=Δwhere we define the Gibbs Energy as
STHG Δ−Δ=Δ
For a spontaneous process at const T,P ( )( ) 0
0<Δ>Δ
sysGtotS
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At low temp T theenthalpy change part Of ΔG has a greatermagnitude than TΔS.
STΔ−
STΔ−
gThe sign of ΔGdepends on the signof ΔH.
HΔHΔ
At high temp T the enthalpychange part of ΔG has asmaller magnitude thanTΔS. The sign of ΔGdepends on the sign of ΔS.
ΔG < 0 for a spontaneous process.ΔG 0 for a spontaneous process.ΔH < 0 (exothermic change) makes favourable contribution to spontaneity.ΔH > 0 (endothermic change) makes unfavourable contribution toSpontaneity.ΔS < 0, entropy decreases, makes unfavourable contribution toSpontaneity.ΔS > 0, entropy increases, makes favourable change to spontaneity.
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ΔG < 0 : reaction or process is spontaneousΔG > 0 : reaction or process is not spontaneousΔG = 0 : reaction or process is at equilibrium
Standard Gibbs energy change of formation ΔfG0298 is defined as the change in Gibbs
energy when 1 mol of a compound is formed at P = 1 bar and at T = 298 K from itsconstituent elements in their standard states.
Standard Gibbs energy of reaction ΔrG0298 is computed from Δf G0 for the
reactants and products using the following rule.
∑∑ Δ−Δ=Δ )()( 0298
0298
0298 rxGprGG fjfjr νν
See Chemistry3 worked example 15.8, pp.728-729.
Once the standard Gibbs energy of reaction ΔrG0298 is known at 298 K
then it is possible to compute the correspondingGibbs energy of reaction at any other temp T using the definition ofthe Gibbs energy function.
0 0 0r T r T r TG H T SΔ = Δ − Δ
( )
0 0298 ,
0
r T r P mH H C TΔ = Δ + Δ Δ
⎟⎠⎞
⎜⎝⎛Δ+Δ=Δ
KKTCSS mPrTr 298
/ln,0298
01
2
( )0298 , 298r P mH C T= Δ + Δ −
( ) ( )∑∑ −=Δ rxCprCC mPjmPjmP ,,, ννSee Chemistry3
Worked example 15.9,pp.729-730.
More of this type of calculation in SF Thermodynamics.
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Chemical equilibrium.
• What is chemical equilibrium ?•How much product will form under a given setof starting conditions ?• What is the composition of a reaction mixture
h h i l ti h tt i d ilib i ?when a chemical reaction has attained equilibrium?• What is the effect of temperature on the composition of a reaction mixture at equilibrium?
N2 (g) + 3 H2 (g) 2 NH3 (g)
Chemical Equilibrium.forward reaction
reverse reactionEquilibrium
Kinetics
• Reactant concentrations decrease with time ; product concentrations increase with time .
• After a long enough time reactant and product concentrations attain steady, time invariant values.
• A state of chemical equilibrium has been attained.
reverse reaction
Haber Process:• If a plot of reaction rate versus time is examined we
note that the rate of the forward reaction decreasesand the rate of the reverse reaction increaseswith increasing time, until, at long times they becomeequal. At this stage the reaction rates no longer changewith time and the reaction is said to be at equilibrium.
Haber Process:Ammonia synthesis
Kinetic definition ofEquilibrium.
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Kinetics applies to the speed of a reaction,
the concentration of product that appears
(or of reactant that disappears) per unit time.
Kinetics versus Equilibrium.
Equilibrium applies to the extent of a reaction, the concentration of product that has appeared after an unlimited time, or once no further change occurs.
A system at equilibrium is dynamic on the molecular level;
no further net change is observed no further net change is observed
because changes in one direction are balanced by changes in the other.
At equilibrium: rate forward step = rate reverse step
Reaching Equilibrium on the Macroscopic and Molecular Level
N2O4 (g) 2 NO2 (g)
colourless brown
NO2
N2O4
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Properties of an equilibrium Reaction
Equilibrium systems are dynamic (in constantchemical change) and reversible (chemical changecan be approached from either direction).
2622242
2242262
)(2)(2)()(
ClOHCoOHClOHCoOHClOHCoClOHCo
→++→
Pink Blue
Blue Pink
PLAY MOVIE
+
( ) ( )( )3 22 2 26 5
Fe H O SCN Fe SCN H O H O+ +−+ +
•• After a period of time, the concentrations of reactants and products After a period of time, the concentrations of reactants and products are constant. are constant.
•• The forward and reverse reactions continue after equilibrium is The forward and reverse reactions continue after equilibrium is attained.attained.
PLAY MOVIE PLAY MOVIE
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Examples of Chemical equilibria : Phase Change
( ) ( )2 2H O s H O
PLAY MOVIE
Chemical Equilibrium :a kinetic definition.
• Countless experiments with chemical systems have shown that in a state of equilibrium, the concentrations of
[ ] ↑ [ ]
Concentrations varywith time
Concentrations timeinvariant
qreactants and products no longer change with time.
• This apparent cessation of activity occurs because under such conditions, all reactions are microscopically reversible.
• We look at the dinitrogen tetraoxide/nitrogen oxide equilibrium whichoccurs in the gas phase.
[ ][ ] ↓
↑
t
t
ON
NO
42
2
Equilibriumstate
Kineticregime
NO2
entra
tion
N2O4 (g) 2 NO2 (g)
[ ][ ] eq
eq
ON
NO
42
2
∞→t
N2O4
time
conc
e2 4 (g) 2 (g)
colourless brown
Kinetic analysis.
[ ][ ]22
42
NOkR
ONkR
′=
=
Equilibrium:
[ ] [ ][ ][ ] K
kk
ONNO
NOkONk
RR
eq
eqeq
=′
=
′=
=
42
22
2242
Valid for any time t
∞→t
Equilibriumconstant
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rateforward = ratereverse
kforward[reactants]m = kreverse[products]n
k [products]n
forward
reverse
reactants n productsrate [reactants]
rate [products]
mforward
nreverse
mk
k
=
=
= = K the equilibrium constantkforward
kreverse
[products]n
[reactants]m
This is also known as the LAW OF MASS ACTION.
The values of m and n are those of the coefficients in the balanced chemical equation.
The rates of the forward and reverse reactions are equal, NOT the concentrations of reactants and products.
Initial and Equilibrium Concentrations for theN2O4-NO2 System at 100°C
Initial Equilibrium Ratio[N2O4] [N2O4] [N2O4][NO2] [NO2] [NO2]2
2 4 2 4 2 42 2 2
0.1000 0.0000 0.0491 0.1018 0.211
0.0000 0.1000 0.0185 0.0627 0.212
0.0500 0.0500 0.0332 0.0837 0.211
0.0750 0.0250 0.0411 0.0930 0.210Constant values
Equilibrium constant K
•The value of the ratio of initial concentrationsvaries widely but always gives the same valuefor the ratio of equilibrium concentrations.•The individual equilibrium concentrations aredifferent in each case but this ratio ofequilibrium concentrations is constant.
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The size of the equilibrium constant indicates whether the reactantsor the products are favoured .
Reactants favoured Products favouredReactants and productsReactants favouredwhen Kc is small
Products favouredwhen Kc is large
pare in almost equalabundance when Kc nearunity
The Reaction Quotient, QThe Reaction Quotient, QIn general, ALL reacting chemical In general, ALL reacting chemical
systems are characterized by their systems are characterized by their systems are characterized by their systems are characterized by their REACTION QUOTIENT, QREACTION QUOTIENT, Q..
a A + b B a A + b B FF p P + q Qp P + q Q
[ ] [ ]p qP Q
If Q = K, then system is at equilibrium.If Q = K, then system is at equilibrium.
[ ] [ ][ ] [ ]
t ta b
t t
P QQ
A B=
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THE EQUILIBRIUM CONSTANTTHE EQUILIBRIUM CONSTANTFor any type of chemical equilibrium of the typeFor any type of chemical equilibrium of the type
a A + b B a A + b B FF p P + q Qp P + q Qthe following is a CONSTANT (at a given T)the following is a CONSTANT (at a given T)
If K is known, then we can predict concentrations. of products or If K is known, then we can predict concentrations. of products or
[ ] [ ][ ] [ ]
p q
eq eqa b
eq eq
P QK
A B=
Equilibriumconstant
Product concentrations
Reactant concentrations
, p p, p preactants in the reaction mixture at equilibrium and hence the reactants in the reaction mixture at equilibrium and hence the yield of the reaction. yield of the reaction.
Relationship between Gibbs Energy and Equilibrium Constant.
We now derive an expression which relates the change in Gibbs energy for areaction as a function of the composition of the reaction mixture at any stagein the reaction.
qQpPbBaA +→+
We can define Gibbs energy in terms of aRTGG ln0 +=
Activity = generalised concentration
Hence after some algebra and simplification the change in Gibbs energy for reaction can be computed.
( ) ( )BAQPr bGaGqGpGG +−+=Δ
We can define Gibbs energy in terms ofthe activity ak of the species k. kkk aRTGG ln+=
( ) ( )( ) ( )
QQPPr
RTGbRTG
aRTGqaRTGpG
ll
lnln00
00 +++=Δ
If the reaction is allowed to proceedTo equilibrium then we replace Q byThe equilibrium constant K and setΔrG = 0 by definition.
( ) ( )BBAA aRTGbaRTGa lnln 00 +−+−
QRTGaaaa
RTGG rbB
aA
pP
rr ln..
ln 00 +Δ=⎪⎭
⎪⎬⎫
⎪⎩
⎪⎨⎧
+Δ=Δ
Reaction quotient Q( ) ( )00000BAQPr bGaGqGpGG +−+=Δ
KRTG
KRTG
r
r
ln
0ln0
0
−=Δ
=+Δ
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a A + b B c C + d D
[ ] [ ][ ] [ ]BA
DCRTGG ba
dc
ln0
⎭⎬⎫
⎩⎨⎧
+Δ=Δ
• Under non-equilibrium conditionsGibbs energy change is :
KQ < KQ >Gibbs energy change for reaction mixture
Expression showshow ΔG varieswith composition[ ] [ ]
QRTG
BA ba
ln0 +Δ=⎭⎬
⎩⎨
Q = reaction quotient [ ] [ ][ ] [ ]ba
dc
BADCQ =
• Q defines reactant and product concentration ratio (i.e. reaction composition) at any stage in
with compositionof reaction mixture.
chemical transformation.
• When ΔG = 0 at constant T and P wehave equilibrium . Hence Q = Kc.
[ ] [ ][ ] [ ]
KRTG
BADC
RTG beq
aeq
deq
ceq
ln0
ln0
0
0
+Δ=
⎪⎭
⎪⎬⎫
⎪⎩
⎪⎨⎧
+Δ= KRTG ln0 −=Δ ⎥⎦
⎤⎢⎣
⎡ Δ−=
RTGK
0
exp
These are very importantrelations!
ProductProduct-- or Reactant Favored or Reactant Favored ProcessesProcesses
K comes from thermodynamics.K comes from thermodynamics.∆G˚ < 0: reaction is ∆G˚ < 0: reaction is product favoredproduct favored∆G˚ > 0: reaction is ∆G˚ > 0: reaction is reactantreactant--favoredfavored
KRTG ln0 −=Δ
If K > 1, then ∆G˚ is negative.If K < 1, then ∆G˚ is positive.
KRTG ln−=Δ
ProductProduct--favoredfavoredK > 1K > 1
ReactantReactant--favoredfavoredK < 1K < 1
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Gibbs energy and chemical equilibrium.
GΔ
Equilibrium Q large Q>K
Reaction not spontaneousIn forward direction
Qln0GG Δ=Δ
0=ΔG
qQ=K
Q small, Q<K[P]<<[R]ΔG negative
Q large, Q>K[P]>>[R]ΔG positive
Standard stateStandard stateQ=1lnQ=0
QRTGG ln0 +Δ=ΔReaction spontaneousIn forward direction
Tr
GG ⎟⎟⎠
⎞⎜⎜⎝
⎛∂∂
=Δξ forward reactionTp,⎠⎝ ∂ξ
reverse reactionspontaneous
forward reactionspontaneous
Extent of reaction ξ
0=ξ 1=ξ
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Reaction Gibbs energyTp
rGG
,⎟⎟⎠
⎞⎜⎜⎝
⎛∂∂
=Δξ
extent of reaction = ξ
1<<K 1>>K1=K
0=Δ Gr0=Δ Gr0=Δ Gr
0=ξ 1=ξ
ΔrG is the slope of the G versus ξ graph at any degree of advancement ξ of the chemical reaction.
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Key stages in the Haber-Bosch synthesis of ammonia.
NH3 synthesis is exothermic (ΔH0 = - 91.8 kJmol-1).Hence K decreases as T increases.
Fritz HaberFritz Haber18681868--19341934Nobel Prize, 1918Nobel Prize, 1918
N2 (g) + 3 H2 (g) 2 NH3 (g)
Carl BoschCarl Bosch18741874--19401940Nobel Prize, 1931Nobel Prize, 1931
Operating conditions dictated by a balance between kineticsand thermodynamics.Yield of NH3 is high when pressure P is large and temperature Tis low. Rate of formation of NH3 is low when T is low.High pressure and continuous removal of NH3 used to increase yield.Temperature is raised and catalyst employed to enhance rate of NH3 formation.
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Effect of Temperature on Kcfor Ammonia Synthesis
T (K) Kc
200. 7.17 x 1015
300. 2.69 x 108
400. 3.94 x 104
500. 1.72 x 102
↑↓ TasKC
How can we explain this ?
• We need to be able topredict the way that K
600. 4.53 x 100
700. 2.96 x 10 -1
800. 3.96 x 10 -2
varies with temperatureT.
• This is given by the van’t Hoff equation.
Temperature dependence of equilibrium constant:van’t Hoff equation.
KRTG ln0 −=Δ
000 STHG Δ−Δ=ΔKRTSTH ln00 −=Δ−Δ R
SRTHK
00
ln Δ+
Δ−=
STHG Δ−Δ=Δ
• We assume that ΔH0 and ΔS0 areindependent of temperature T overthe temperature range of interest.
• Assume that K = K1 when T = T1 andK = K2 when T = T2. Note that T2 > T1.
RS
RTHK
0
1
0
1ln Δ+
Δ−=
RS
RTHK
0
2
0
2ln Δ+
Δ−=
⎫⎧Δ⎫⎧ 0 11HK
⎭⎬⎫
⎩⎨⎧
−Δ
=⎭⎬⎫
⎩⎨⎧
=−211
212
11lnlnlnTTR
HKKKK
This can be used to understandthe temperature dependence ofthe equilibrium constant.
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Now T2>T1 so the term 1/T1-1/T2 is positivesince 1/T2 < 1/T1. Also the term ln{K2/K1} depends on the sign of ΔH0.
• Endothermic reaction: ΔH0 is positive, h i l i l i i d the exponential term is also positive, and
so K2/K1 >1 and K2 > K1.•The equilibrium constant for an endothermic process increases with temperature. Increase in T favoursproducts.• Exothermic reaction: ΔH0 is negative, and K2 < K1. •The equilibrium constant for an •The equilibrium constant for an exothermic process decreaseswith an increase in temperature. Increase in T favours reactants.
Percent Yield of Ammonia vs. Temperature (°C)
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70
Best NH3 yield at low T and high P.
340atm/P140600C/T400 0
≤≤≤≤
Optimizing Ammonia Synthesis
10
20
30
40
50
60
350
NH
3 yi
eld
/ mol
%
Low T : slow reactionkinetics
0350
400450
500550
600650
200250
300350
400450
500550 Temperature /
0 C
Pressure / atmHigh P : expensive plant N2 (g) + 3 H2 (g) 2 NH3 (g)
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Thermodynamic criteria ofspontaneity.
If the reaction is exothermic (ΔrH0 < 0)and ΔrS0 > 0 then ΔrG0 < 0 and K > 1 atall temperatures.
KRTGr ln0 −=Δ
000 STHG rrr Δ−Δ=Δ
reaction If the reaction is exothermic (ΔrH0 < 0)and ΔrS0 < 0 then ΔrG0 < 0 and K > 1provided that T < ΔrH0/ΔrS0 .
If the reaction is endothermic (ΔrH0 > 0)and ΔrS0 > 0 then ΔrG0 < 0 and K > 1provided that T > ΔrH0/ΔrS0 .
f h d h ( H0 0)
products dominantat equilibrium 01 0 <Δ>> GifK r
thermodynamicallyfeasible
0If the reaction is endothermic (ΔrH0 > 0)and ΔrS0 < 0 then ΔrG0 < 0 and K > 1 atno temperature.
reactants dominantat equilibrium
01 0 >Δ<< GifK r
reaction notthermodynamicallyfeasible
Chemical Equilibrium Problems.Suppose that 0.150 mol PCl5 is placed in a reaction vessel of volume 500 cm3 andallowed to reach equilibrium with its decomposition products phosphorous trichlorideand chlorine at 2500C. If the equilibrium constant Kc is 1.80, determine the composition of the reaction mixture at equilibrium.
PCl5(g) PCl3(g) + Cl2(g)[ ][ ][ ]
23
PClClPClKc =5(g) PCl3(g) Cl2(g) [ ]5PCl
Initial concentration of PCl5 = 0.150 mol / 0.500 L = 0.3 M. Let an amount x of PCl5 be used up in reaction to form products.
Species PCl5 PCl3 Cl2
Initial concentration
0.3 0 0
Change in
-x +x +x
[ ][ ][ ]
054.08.1
8.13.0
2
2
5
23
=−+
=−
==
xx
xx
PClClPClKc
Phosphorous(V) chloride Phosphorous(III) chloride
concentration
Equilibrium concentration
0.3 - x x x
( )2.06-and262.0
2)54.0.(1.48.18.1 2
=−−±−
=x
We choose the positive root of the quadraticequation and so x = 0.262. [ ]
[ ][ ] MxCl
MxPClMxPCl
262.0262.0
038.0262.03.03.0
2
3
5
====
=−=−=
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The formation of NO from N2 and O2 contributes to air pollution whenevera fuel is burnt in air at a high temperature as in a gasoline engine.At 1500 K the equilibrium constant K = 1 x 10-5. Suppose a sample of airhas [N2]= 0.80 mol/L and [O2]=0.20 mol/L before any reaction occurs.Calculate the equilibrium concentrations of reactants and products after the mixture has been heated to 1500 K.
[ ] ( )2 2 25 2 4NO x x
2 2( ) ( ) 2 ( )N g O g NO g+
N2/M O2/M NO /M
Initial 0 80 0 20 0
ICE Table
[ ] ( )( )( )
5
2 2
2 6
4
41.0 10[ ].[ ] 0.8 0.2 0.8 0.2
4 1.6 106.3 10
NO x xKN O x x
xx
−
−
−
= × = =− − ×
×
×
We assume that x << 1, i.e. lessthan 10% of initial reactant concentration [R]0 then ([R]0-x)≈[R]0Approximation valid when equilibriumInitial 0.80 0.20 0
Change -x -x +2x
Equilibrium 0.80-x 0.20-x 2x
42
42
3
[ ] 0.80 0.8 6.3 10 0.8
[ ] 0.20 0.20 6.3 10 0.8
[ ] 2 1.3 10
N x M
O x M
NO x M
−
−
−
= − − ×
− − ×
×
Approximation valid when equilibriumConstant K is small and << 1.
x = amount reacted
Under certain conditions nitrogen and oxygen react to form dinitrogen oxide N2O.Suppose that a mixture of 0.482 mol N2 and 0.933 mol O2 is placed in a reaction vessel of volume 10 dm3 and allowed to form N2O at a temperature for which Kc= 2 x 10-13.Determine the composition of the reaction mixture at equilibrium.
2 N2(g) + O2(g) 2 N2O(g) [ ][ ] [ ]2
22
22
ONONKc =[ ] smallvery102 13 ONK −×=
[ ]
9330
0482.010482.0N
ionsconcentratInitial
32 ==
l
Mdm
mol
[ ] [ ]22 ON[ ] smallvery102 2ONKc ×=[ ]
[ ] 0
0933.010933.0
2
32
=
==
ON
Mdm
molO
Species [N2] [O2] [N2O]
Initialconcentration
0.0482 0.0933 0
Change in 2x x +2x
[ ][ ] [ ]
( )( ) ( )xx
xON
ONKc −−==
0933.020482.02
2
2
22
2
22
When rearranged this expression yieldsa cubic equation in x.Since Kc is small we can assume that x isalso very small and assume :
Change inconcentration
-2x -x +2x
Equilibriumconcentration
0.04-2x 0.0933-x 2x0933.00933.0
0482.020482.0≅−≅−
xx( )
( ) ( )( )
9
2
2
2
103.34
0933.00482.0
0933.00482.02
−×=
××≅
≅
C
C
Kx
xK
Hence our approximationis OK
Hence at equilibrium:
[ ][ ][ ] MxON
MxOMxN
92
2
2
106.62
0933.00933.00482.020482.0
−×≅=
≅−=≅−=
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Le Chatelier’s PrincipleTemperature, catalysts, and changes in concentration Temperature, catalysts, and changes in concentration affect equilibria.affect equilibria.The outcome is governed by The outcome is governed by LE CHATELIER’S LE CHATELIER’S PRINCIPLEPRINCIPLE“...if a system at equilibrium is disturbed, the system “...if a system at equilibrium is disturbed, the system tends to shift its equilibrium position to counter the tends to shift its equilibrium position to counter the tends to shift its equilibrium position to counter the tends to shift its equilibrium position to counter the effect of the disturbance.”effect of the disturbance.”
When a reactant is added to a reaction mixture at equilibrium, the reaction tends to form products. When a reactant is removed, more reactant tends to form.When a product is added, the reaction tends to form reactants. When a product is removed, moreproduct is formed.
KQKQ
Henri Le Chatelier1850-1936
KQ >KQ <
[ ][ ][ ][ ]eq
eq
RP
K
RPQ
=
=
Note : only Q responds to additionof R or P ; K remains the same.
Le Chatelier’s PrincipleLe Chatelier’s Principle
• Change T– change in K change in K – therefore change in P or concentrations at
equilibrium• Use of catalyst: reaction comes more
quickly to equilibrium. K not changed.• Add or take away reactant or product:y p
– K does not change– Reaction adjusts to new equilibrium
“position”
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Effect of Various Disturbanceson an Equilibrium System
Disturbance Net Direction of Reaction Effect on Value of KConcentration
Increase [reactant] Toward formation of product NoneDecrease [reactant] Toward formation of reactant None[ ]
Pressure (volume)Increase P Toward formation of lower
amount (mol) of gas NoneDecrease P Toward formation of higher
amount (mol) of gas NoneTemperature
Increase T Toward absorption of heat Increases if ΔH0rxn> 0
D if ΔH0 0Decreases if ΔH0rxn< 0
Decrease T Toward release of heat Increases if ΔH0rxn< 0
Decreases if ΔH0rxn> 0
Catalyst added None; rates of forward and reverse reactions increaseequally . None