3.5
Calculating Equilibrium Constants from Gibbs free energy data
3.5a The relationship between
free energy and equilibrium constants
To calculate the
concentration equilibrium constant Kc or Kp
for a reaction
aA + bB ...
dD + eE ...
Kc
= ([A]a [B]b...)/([D]d [E]e...)
where [] are the concentration terms
Kp =(pAa
pBb...)/(pDd
pEe...)
where px are the partial pressures
The standard
Gibbs free energy change ∆Gθsys =
∆Hθsys – T∆Sθsys and
∆Gθsys
= –RT ln(Kc) = –RT ln{([A]a [B]b ..)/([D]d
[E]e...)}
or for a gaseous
equilibrium
∆Gθsys
= –RT ln(Kp) = –RT ln{(pAa pBb...)/(pDd
pEe...)}
Two examples of Kp
and a Kc equilibrium constant calculations are given below
and both start from fundamental thermodynamic data, but in an exam, you
might well start the calculation given a G value. A Kc
equilibrium constant calculation for a redox reaction is described in
section 3.5b.
Ex 3.5a1 Calculate the
equilibrium constant at 298K for the dissociation of dinitrogen
tetroxide
This colourless gas
readily dissociates into nitrogen(IV) oxide (nitrogen dioxide).
equilibrium equation |
N2O4(g) |
 |
2NO2(g) |
ΔHθf,298K/kJ
mol–1 |
+9.7 |
|
2 x +33.9 |
Sθ298K/J
mol–1K–1 |
304 |
|
2 x 240 |
ΔHθsys,298K
= ∑ΔHf,products
– ∑ΔHf,reactants
= (2 x +33.9) – (+9.7) = +58.1 kJ mol–1 |
ΔSθsys,298K
=
∑Sproducts
– ∑Sreactants
= (2 x 240) – (304) = 176 J mol–1K–1 |
ΔGθsys,298K
= ΔHθsys
– TΔSθsys = (+58.1) – (298 x
176/1000) = +5.652
kJ mol–1 |
∆Gθsys
= –RT ln(Kp) = –RT ln{(pNO22)/(pNO2)} |
substituting:
5.652 x 1000 = –8.314 x 298 ln(Kp)
ln(Kp)
= –5652/(8.314 x 298) = 2.281
Kp = pNO22/pNO2
= exp(–2.281) = e(–2.281) =
0.102 atm
One data book value quoted is
0.115 atm, so not too bad! |
Ex 3.5a2
Calculate the equilibrium constant for the formation of ammonia
equilibrium |
N2(g) |
+ 3H2(g) |
 |
2NH3(g) |
ΔHθf,298K/kJ
mol–1 |
0 |
0 |
|
2 x –46.2 |
Sθ298K/J
mol–1K–1 |
192 |
3 x 131 |
|
2 x 193 |
ΔHθsys,298K
= ∑ΔHf,products
– ∑ΔHf,reactants
= (0 + 0) – (2 x 46.2) = –92.4
kJ mol–1 |
ΔSθsys,298K
=
∑Sproducts
– ∑Sreactants
= (2 x 193) – (192 + 3x131) = –199
J mol–1K–1 |
ΔGθsys
= ΔHθsys
– TΔSθsys = (–92.4) – (298 x
–199/1000) =
–33.1 kJ mol–1 |
∆Gθsys
= –RT ln(Kp) = –RT ln{(pNH32)/(pN2
x pH23)} |
substituting: –33.1 x 1000 = –8.314
x 298 ln(Kp)
ln(Kp) =
33100/2477.6 = 13.35, so Kp = exp(13.36) = 6.33 x 105
atm–2
Kp = pNH32/pN2 pH23
= 6.28 x 105 atm–2
You can also calculate Kp
via Kp = exp(–ΔG/RT)
= exp{33100/(8.314 x 298} = exp(13.36) = 6.33 x 105
atm–2
One data book value quoted is
6.76 x 105 atm–2, so again, quite good
agreement. |
Ex 3.5a3
Calculating the equilibrium constant for an esterification
equation, all (l) |
CH3COOH |
+ CH3CH2OH |
 |
CH3COOCH2CH3 |
+ H2O |
ΔHθf,298K/kJ
mol–1 |
–487 |
–278 |
|
–481 |
–286 |
Sθ298K/J
mol–1K–1 |
160 |
161 |
|
259 |
70 |
ΔHθsys
= ∑ΔHf,products
– ∑ΔHf,reactants
= (–481 –286) – (–487 –278) = –2
kJ mol–1 |
ΔSθsys,273K
=
∑Sproducts
– ∑Sreactants
= (259 + 70) – (160 + 161) = +8J mol–1K–1 |
ΔGθsys
= ΔHθsys
– TΔSθsys = –2 – (298 x +8/1000)
= –4.38 kJ mol–1 |
∆Gθsys
= –RT ln(Kc) = –RT ln{[CH3COOCH2CH3][H2O]/[CH3COOH][CH3CH2OH]} |
substituting: –4.38 x 1000 = –8.314
x 298 ln(Kc)
ln(Kc) =
–4380/–2478 = 1.77, so Kc = exp(1.77) = e(1.77)
= 5.8
Kc = [CH3COOCH2CH3][H2O]/[CH3COOH][CH3CH2OH]
= 5.8
However a figure
of 4 is often quoted for this Kc esterification
equilibrium constant at 298K (25oC), but in an early
investigation in 1862 this value of 4 was quoted for 373 K (100oC).
Very confusing! though it should be noted that applying Le
Chatelier's rule, Kc will increase at a lower
temperature as the reaction is slightly exothermic which
corresponds in principle to the value calculated here. |
TOP OF PAGE
3.5b Free
energy changes in redox reactions and calculation of the equilibrium
constant Kc
The free energy
change for a reversible electrode reaction is ∆Gθsys =
–nEθF
n is the
number of electrons transferred in the theoretical cell reaction
F is the Faraday constant (96500 C mol–1, i.e. equivalent
to 1 mole of electrons)
and in general ∆Gθsys =
–RT ln(Kc)
therefore for a
redox equilibria –nEθF = –RT ln(Kc)
R = ideal gas
constant, T absolute temperature in K, Kc =
concentration equilibrium constant,
so nEθF
= RT ln(Kc) from which the equilibrium constant Kc can be
calculated for a redox reaction.
REMEMBER ...
∆Gθ
must be negative, and Eθ positive, for the
theoretical overall redox reaction to be feasible.
Ex 3.5b1 Calculating the
equilibrium constant for the redox equilibrium between silver and
iron(III) ions at 298K
Ag+(aq)
+ e–
Ag(s) Eθ298 = +0.799V
(silver(I) ion – silver half–cell reaction equilibrium)
Fe3+(aq)
+ e–
Fe2+(aq) Eθ298 = +0.771V
(iron(III) – iron(II) ion half–cell reaction equilibrium)
For the 'cell'
reaction: Ag+(aq) + Fe2+(aq)
Ag(s) + Fe3+(aq)
Kc
= [Fe3+(aq)]/[Ag+(aq)]
[Fe2+(aq)] mol–1 dm3
(remember
solid concentrations are considered to be constant and treated
as being unity)
As the cell
reaction is set out,
silver ions are reduced to silver (Eθred)
and iron(II) ions oxidised to iron(III) ions (Eθox),
therefore at 298K from
Eθcell
= Eθred–half–cell – Eθox–half–cell
Eθcell
= (+0.799) – (+0.771) = +0.028 V
This shows
the reaction is feasible, but with Eθreaction
close to zero, an equilibrium situation would be expected, i.e.
the reaction will not go anywhere near completely to the right.
∆Gθsys =
–nEθF
= –1 x 0.028 x 96500 = –2702 J mol–1
∆Gθsys =
–RT ln(Kc)
–2702 = –8.314 x
298 x ln(Kc)
ln(Kc)
= 2702/(8.314 x 298) = 1.091
Kc
= exp(1.091) = e(1.091) = 2.98 mol–1 dm3
Ex
3.6 Kinetic stability versus thermodynamic
feasibility
If the calculated free
energy change is negative i.e. the reaction is feasible and reactants
theoretically suffer from instability! BUT will the reaction occur spontaneously on
mixing the reactants?
See also
"KINETICS" section 6.
A mixture of hydrogen
and oxygen (e.g. in air at room temperature) is perfectly stable until a
means of ignition, e.g. a lit splint, match or spark etc., is applied. Thermodynamically
the mixture is highly unstable with a very negative free energy
ΔGθ
and shouldn't exist! However, the activation energy to break the strong H–H
or O=O bonds is so high, that they 'happily' co–exist without reacting,
because the particle collisions are not energetic enough to cause a
reaction. Therefore the
mixture is kinetically stable. A high temperature from a match or spark etc., gives
enough of the reactant molecules sufficient kinetic energy to overcome the
activation energy on collision*.
2H2(g) +
O2(g) ==> 2H2O(l), ΔGθ
= –237 kJmol–1 or ΔHθ
= –286 kJmol–1
Note: A
very negative ΔHθ
is usually, but not necessarily, indicative of a negative free energy
change, which is the case here.
*The
transition metal palladium can reduce the activation energy so much that
it catalyses the spontaneous combustion/combination of hydrogen and
oxygen at room temperature!
Like the methane–chlorine
reaction below, the combustion of hydrogen is free radical chain reaction
(a complex mechanism not dealt with at A level). The
initiating energy produces the first free radicals.
A mixture of hydrogen/methane
and chlorine is stable in the dark, but exposed to light (particularly
ultra–violet), the mixture explodes to form hydrogen chloride/chloromethane gas. The
strong H–H/C–H and Cl–Cl bonds ensure a high activation energy, but the
absorption by chlorine (with the weakest bond) of a photon of light energy,
to start the Cl–Cl bond breaking and so initiating the fast and
exothermic free radical chain reaction (explosive!).
H2(g) +
Cl2(g) ==> 2HCl(g), ΔGθ
= –191 kJmol–1 or ΔHθ
= –185 kJmol–1 (again the free energy change is very
negative)
mechanism:
initiation: Cl2 ==> 2Cl
propagation:
Cl + H2 ==> HCl + H and H + Cl2
==> HCl + Cl
termination:
2Cl ==> Cl2 or 2H ==> H2
or H + Cl ==> HCl
CH4(g) +
Cl2(g) ==> CH3Cl(g) + HCl(g),
ΔGθ
= –103 kJmol–1 or
ΔHθ
= –99 kJmol–1
[full
mechanistic details for methane]
Hydrogen peroxide is
thermally unstable, its aqueous solution is kept in a brown bottle to avoid
decomposition initiated by light. It has a decent shelf–life of a few weeks,
i.e., reasonably kinetically stable in the short term, until manganese(IV)
oxide powder is added and then the rapid exothermic reaction takes place!
2H2O2(aq)
==> 2H2O(l) + O2(g)
See also
"KINETICS" section 6.
Energetics-Thermochemistry-Thermodynamics Notes INDEX
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QUICK INDEX for
Energetics:
GCSE Notes on the basics of chemical energy changes
– important to study and know before tackling any of the three Advanced Level
Chemistry pages Parts 1–3 here
* Part 1a–b
ΔH Enthalpy Changes
1.1 Advanced Introduction to enthalpy changes
of reaction,
formation, combustion etc. : 1.2a & 1.2b(i)–(iii)
Thermochemistry – Hess's Law and Enthalpy
Calculations – reaction, combustion, formation etc. : 1.2b(iv)
Enthalpy of reaction from bond enthalpy
calculations : 1.3a–b
Experimental methods
for determining enthalpy changes and treatment of results and
calculations :
1.4
Some enthalpy data patterns : 1.4a
The combustion of linear alkanes and linear
aliphatic alcohols
:
1.4b Some patterns in Bond
Enthalpies and Bond Length : 1.4c
Enthalpies of
Neutralisation : 1.4d Enthalpies of
Hydrogenation of unsaturated hydrocarbons and evidence of aromatic
ring structure in benzene
:
Extra Q page
A set of practice enthalpy
calculations with worked out answers **
Part 2 ΔH Enthalpies of
ion hydration, solution, atomisation, lattice energy, electron affinity
and the Born–Haber cycle : 2.1a–c What happens when a
salt dissolves in water and why? :
2.1d–e Enthalpy
cycles involving a salt dissolving : 2.2a–c
The
Born–Haber Cycle *** Part 3
ΔS Entropy and ΔG Free Energy Changes
: 3.1a–g Introduction to Entropy
: 3.2
Examples of
entropy values and comments * 3.3a ΔS, Entropy
and change of state : 3.3b ΔS, Entropy changes and the
feasibility of a chemical change : 3.4a–d
More on ΔG,
free energy changes, feasibility and
applications : 3.5
Calculating Equilibrium
Constants from ΔG the free energy change : 3.6
Kinetic stability versus thermodynamic
feasibility - can a chemical reaction happen? and will it happen?
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