The cell diagram is:
Zn(s) | Zn2+(aq), (a=1) || Cu2+(aq), (a=1) | Cu(s)
This is the Daniel cell.
Potential determining equilibria:
at RH Electrode: ½Cu2+(aq) + e- ⇌ ½ Cu(s); E0Cu|Cu2+ = +0.34V
at LH Electrode: ½Zn2+(aq) + e- ⇌ ½ Zn(s); E0Zn|Zn2+ = -0.76V
Formal Cell Reaction:
½Cu2+(aq) + ½Zn(s) ⇌ ½Zn2+(aq) + ½Cu(s)
E0cell = E0Cu|Cu2+ - E0Zn|Zn2+ - {RT/2F} ln(aZn2+ /aCu2+)
E0cell = 0.34 - (-0.76) = +1.10V
E0cell > 0 Zinc reduces a copper(II) solution to metallic copper.
The cell diagram is:
Pb(s) | Pb2+(aq), (a=1) || Ag+(aq), (a=1) | Ag(s)
The EMF if E0cell = +0.912 V.
Potential determining equilibria:
at RH Electrode: Ag+(aq) + e- ⇌ Ag(s); E0Ag|Ag+ = ?
at LH Electrode: ½Pb2+(aq) + e- ⇌ ½Pb(s); E0Pb|Pb2+ = -0.130V
Formal Cell Reaction:
Ag+(aq) + ½Pb(s) ⇌ ½Pb2+(aq) + Ag(s)
Nernst Equation:
Ecell = E0cell + {RT/F}ln{aAg+ aPb½/aAg aPb2+½}
Lead and silver are both pure solids at room temperature (298K), and therefore the activities of these species are unity.
Hence, 0.912 = E0cell + (8.313 x 298/ 96 490)ln{0.5/1½}
ie., E0cell = E0RHE - E0LHE = E0Ag|Ag+ + 0.130 = +0.930V
Therefore, E0Ag|Ag+ = +0.800V
This result is consistent with data given in Table 1.1 on page 29.
The cell diagram is:
Pt | Fe2+(aq), (a=1), Fe3+(aq), (a=1) || Ce3+(aq), (a=1), Ce4+(aq), (a= 1) | Pt
E0cell = +0.84V At 298K
Potential determining equilibria:
RHE Ce4+(aq) + e- ⇌ Ce3+(aq)
LHE Fe3+(aq) + e- ⇌ Fe2+(aq)
Formal cell reaction:
Ce4+(aq) + Fe2+(aq) ⇌ Ce3+(aq) + Fe3+(aq)
This is a 1 electron transfer.
ΔG0 = -FE0cell
ΔG0 = -RTln K
-FE0cell = -RTln K
ln K = FE0cell/RT
ln K = (96 490 x 0.84) / (8.313 x 298) = 32.72
K = exp(32.72) = 1.6 x 1014
Notice that in this case K is a dimensionless quantity.
The cell diagram is:
Pt | H2(g) (P = 1atm) | HBr (10-4M) | CuBr(s) | Cu(s)
E298K = +0.559V
Potential Determining Equilibria:
RHE: CuBr(s) + e- ⇌ Cu(s) + Br-(aq); E0Cu|CuBr = ?
LHE: H+(aq) + e- ⇌ ½H2(g); E0H+|H2 = 0.00V (by definition)
Therefore, E0cell = E0Cu|CuBr
Cell Reaction:
CuBr(s) + ½H2(g) ⇌ Cu(s) + Br-(aq) + H+(aq)
Hence, the Nernst Equation for this equilibrium is:
E = E0cell - {RT/F}ln{aBr- aH+ / PH2½} = 0.559V
Therefore, E0cell = ECu¦CuBr = +0.0861V
Now, consider the cell:
Cu(s) | Cu+(aq) || Br-(aq) | CuBr(s) | Cu(s)
The cell reaction is: CuBr(s) ⇌ Cu+(aq) + Br-(aq)
We notice that the equilibrium constant for this process is the solubility product (KSP) for CuBr.
Now, E0cell = E0Cu|CuBr - E0Cu+|Cu = 0.0861 - 0.522 = -0.4359V
DG0 = -RTlnKSP = -nFE0cell
where n is the number of electrons involved in the cell equilibrium (= 1 in this case).
Therefore,
KSP = exp{ FE0cell / RT}
KSP = 4.225 x 10-8 mol2 dm-6
The reader will find that the quoted solubility product at 298K in data books is 6.27 x 10-9 mol2 dm-6 - an order of magnitude lower than the above result, which in fact corresponds to the value as measured at 293K. The interested reader will find it constructive to calculate a value for the enthalpy of dissolution of CuBr, using the van't Hoff isochore (assuming, to a good approximation, that this value does not change with temperature).
The cell diagram is:
Pt | H2(g) (P = 1 atm) | HCl (a = 1) | AgCl(s) | Ag(s)
This is the Harned Cell. We first write down the potential determining equilibria
at the RHE: AgCl(s) + e- ⇌ Ag(s) + Cl-(aq)
at the LHE: H+(aq) + e- ⇌ ½H2(g)
Hence, the cell reaction is:
AgCl(s) + ½H2(g) ⇌ Ag(s) + H+(aq) + Cl-(aq)
For one electron transfer processes, ΔG0 = -FE0cell
Therefore, at 298K,
E0cell = 0.2366 - 4.856 x 10-4(T - 273) - 3.421 x 10-6(T - 273)2
= 0.2366 - 4.856 x 10-4(298-273) - 3.421 x 10-6(298 - 273)2
= +0.225V
Therefore, ΔG0 = -(96 490)(0.225) = -21.45kJ mol-1
The reader is advised to review pp. 33-36. We quote the result ΔS0 = F(∂E0/ ∂T)P
Differentiating the expression given in the question with respect to T (at constant P) using the chain rule (see Sivia, D, "Fundamentals of Mathematics for Chemists"; Oxford Chemistry Primer, OUP) gives,
(∂E0/∂T)P = -4.856 x 10-4 - 2 x 3.421 x 10-6 x (T - 273)
Therefore, at 298K, (∂E0/∂T)P = -6.5665 x 10-4 V K-1
Hence, ΔS0 = -63.38J mol-1 K-1
Since, ΔG0 = ΔH0 - TΔS0
ΔH0 = -40.33kJ mol-1
The cell diagram is:
Ag | AgCl | Cl2(g) | Pt
The cell is reversible in both solid and liquid phases.
RHE: ½Cl2(g) + e- ⇌ Cl-(s/l)
LHE: AgCl(s/l) + e- ⇌ Ag(s/l) + Cl-(s/l)
Formal Cell Reaction:
½Cl2(g) + Ag(s) ⇌ AgCl(s/l)
We know that G = H - TS and H = U +PV
So, G = U + PV - TS
Therefore, dG = dU + PdV + VdP - TdS - SdT
But, dU = dq + dw (where the bold derivatives remind us that these two quantities are non-state functions. [See Price, G, "Thermodynamics of Chemical Processes"; Oxford Chemistry Primer, OUP for a treatment of state functions.]
Under reversible conditions, dS = dqrev/T, and thus, considering only expansion work,
dU = TdS - PdV and so dG = VdP - SdT
Hence, (∂G/∂T)P = -S, or (∂ΔG/∂T)P = - ΔS
(where the ∂ refers to a partial derivative. See Sivia, ibid. for more about partial derivatives.)
Since ΔG = -FE for a one-electron process,
ΔS = F(∂E/∂T)P
Therefore, a graph of E against T will enable us to calculate ΔS.
We observe two lines, as the temperature range of the experiment spans the transition temperature for the AgCl(s)/ AgCl(l) phase change. The melting point of the compound will be the temperature of the intersection of these two lines. Tfus = 742.5K One line (viz. the one with steeper gradient) refers to the cell reaction:
½Cl2(g) + Ag(s) ⇌ AgCl(l).
The entropy of this reaction will therefore be related to the gradient of this line. From the graph, the gradient is 5.0286 x 10-4V K-1 Similarly, the other line refers to the cell reaction:
½Cl2(g) + Ag(s) ⇌ AgCl(s).
The gradient of this line relates to the entropy of this cell reaction. From the graph, the gradient is 3.36 x 10-4V K-1 The entropy corresponding to the phase transition:
AgCl(s) → AgCl(l) will be the difference of these two entropies.
Hence, since ΔGfus = 0 at Tfus (as melting [fusion] is an equilibrium process),
ΔHfus = Tfus ΔSfus
From graph, ΔSfus = F{5.0286 - 3.36} x 10-4
= +16.1Jmol-1K-1
This is positive as expected, as there is an increase in molecular randomness (ie. entropy) on going from the solid to liquid phase.
ΔHfus = Tfus ΔSfus = +11.95kJmol-1
Reference to a data book (eg. Lide, D R (ed.) "CRC Handbook of Chemistry and Physics", 76th edn., CRC Press, Boca Raton, Florida (1995)) shows that these results are accurate within the limits of experimental error, again illustrating the usefulness of electrode potentials in determining thermodynamic data.
The reader is recommended to read pp. 63-66 of the book, to see how to solve this particular problem. Readers looking for innovative and novel ways to solve it are invited to read on!
Harned Cell:
Pt | H2(g) (P= 1atm) | HCl(aq) | AgCl(s) | Ag(s)
Potential determining Equilibria
RHE: AgCl(s) + e- ⇌ Ag(s) + Cl-(aq)
LHE: H+(aq) + e- ⇌ ½H2(g)
Cell Reaction:
AgCl(s) + ½H2(g) ⇌ Ag(s) + H+(aq) + Cl-(aq)
Nernst Equation: Ecell = E0cell - {RT/F}ln{aH+ aCl- a Ag / aAgCl PH2 ½}
Notice that since hydrogen is a gas at the temperature of the experiment (298K), we use its partial pressure. ( Strictly, we should talk about the fugacity of hydrogen. This is similar to the concept of activity. However, we can consider hydrogen [to an excellent approximation] as being an ideal gas, with a fugacity coefficient equal to unity.)
Also, since silver and silver chloride are pure solids, their activities can be equated to unity.
Therefore, the Nernst Equation simplifies to:
Ecell = E0cell - {RT/F}ln{aH+ aCl-}
Now, aH+ = f+mH+ = f+mHCl, and aCl- = f-mCl- = f-mHCl
But in the electrolyte solution, the H+ ions and Cl- ions co-exist, and hence, the activity coefficients of the individual ions have no physical meaning. We therefore use the mean ionic activity coefficient f±, which is defined on p.63, for each ionic species.
Therefore, since we are dealing with a 1:1- electrolyte, f±= (f+ f-)½
Hence, substituting these results into the Nernst Equation, and changing from natural logarthims to decadic logarthims gives:
Ecell = E0cell - 2.303{RT/F}log mHCl2 - 2.303{RT/F}log {f±2}
E0cell = E0Ag|AgCl - E0H+|H2 = E0Ag|AgCl ; (by definition of E0H+|H2 = 0V)
Thus, Ecell = E0Ag|AgCl - 2.303{RT/F}log mHCl2 - 2.303{RT/F}log {f±2}
The Debye-Hückel Limiting Law (DHL) states that logf± = -A|z+||z-|I½, where z+, z- are the charges on the ions, A is a temperature and solvent dependent parameter (= 0.509 in water at 298K) and I is the ionic strength of the solution, as defined on p.45. In this case, I = m. [The committed reader will find a derivation of the DHL in chapter 2, Rieger, P H, "Electrochemistry"; Prentice-Hall, New Jersey (1987).]
Hence, we can calculate a value for log f± .
m / mol kg-1 I / mol kg-1 log f±
4 x 10-4 4 x 10-4 -0.01
9 x 10-4 9 x 10-4 -0.015
1.6 x 10-3 1.6 x 10-3 -0.02
2.5 x 10-3 2.5 x 10-3 -0.025
We can now determine a value for the Standard Electrode Potential for the silver/silver chloride couple.
Ecell = E0Ag|AgCl - 2.303(2){RT/F}ln m - 2.303(2){RT/F}log {f±}
or, Ecell + 4.606{RT/F}log {f±} = E0Ag|AgCl - 4.606{RT/F}log m
We now plot a graph of Ecell + 4.606{RT/F}log {f±} against log m. This gives an intercept of EAg|AgCl.
E / V I / mol kg-1 Ecell + 4.606{RT/F}log {f±} log m
0.62565 4 x 10-4 0.62447 -3.398
0.58460 9 x 10-4 0.58283 -3.046
0.55565 1.6 x 10-3 0.55329 -2.796
0.53312 2.5 x 10-3 0.53020 -2.602
From the graph, E0Ag|AgCl = +0.222V
Both cells A and B are Harned Cells
Pt | H2(g) | HCl(aq) | AgCl(s) | Ag(s)
Potential determining Equilibria:
RHE: AgCl(s) + e- ⇌ Ag(s) + Cl-(aq)
LHE: H+(aq) + e- ⇌ ½H2(g)
Cell Reaction:
AgCl(s) + ½H2(g) ⇌ Ag(s) + H+(aq) + Cl-(aq)
Nernst Equation: Ecell = E0cell - {RT/F}ln{aH+ aCl-},
for PH2 = 1 bar which approximates to 1 atm., and where E0cell = E0Ag|AgCl (by definition of E0H+|H2 = 0V).
Consider Cell A
aH+ = Kw/ aOH-
Hence, Ecell = E0Ag|AgCl - {RT/F}ln{Kw aCl-/ aOH-}
Now, aX = fX[X], where fX is the activity coefficient of X (also given the lower case Greek symbol gamma) and, [Cl-] = [OH-] = c
Also, since c < 10-2M, the Debye-Hückel Limiting Law (DHL) applies.
Since lgfi = -Azi2I½, and I, zi2 and A are all the same for both Cl- and OH-, fCl- = fOH- and so,
Ecell = E0Ag|AgCl - {RT/F}lnKw (1)
From the data given, we notice that Ecell A is not a function of concentration (as equation (1) predicts), and therefore,
1.0493 = E0Ag|AgCl - {RT/F}lnKw (2)
We next need a value for E0Ag|AgCl which (if we are to find Kwmust therefore be obtained from cell B.
Now we consider Cell B:
Ecell = E0Ag|AgCl - {RT/F}ln{aH+ aCl-}
aH+ = f+c and aCl- = f-(2c)
Using the DHL, we see that f+ = f- = f , since zi2, A(= 0.509 in water at 298K) and I are the same for both H+ and Cl-, as they co-exist in a solution of ionic strength I.
I = ½(c + 2c) = 3c/2 mol dm-3
Therefore, E = E0Ag|AgCl - {RT/F}ln{f2 2c2}
E + {RT/F}ln{2c2} = E0Ag|AgCl - {4.606RT/F}lg(f)
E + {RT/F}ln{2c2} = E0Ag|AgCl - 4.606(0.509)RT(3/2)½ c½/ F
Hence, a plot of E + {RT/F}ln{2c2} (on the ordinate axis) against c½ (on the abscissa) will have an ordinate intercept equal to the Standard Electrode Potential for Ag|AgCl.
E/V c/mol dm-3 c½/ mol½ dm-3/2 E + {RT/F}ln{2c2}/V
0.578 0.001 0.0316 0.2411
04969 0.005 0.0707 0.2426
0.4624 0.010 0.1000 0.2437
From the graph, ordinate intercept = E0Ag|AgCl = +0.2395V
Thus, from (2), Kw = 2.00 x 10-14 mol2 dm-6.
Of the course the true answer for Kw is only one half as big; students 'refining' their results beware!
Cell diagram:
Pt | H2 (1 atm) | NH3 (c), NH4Cl (c) | AgCl | Ag
This is (again) a Harned Cell ie.
Pt | H2 | HCl | AgCl |Ag
Potential determining Equilibria:
RHE: AgCl(s) + e- ⇌ Ag(s) + Cl-(aq)
LHE: H+(aq) + e- ⇌ ½H2(g)
Cell Reaction:
AgCl(s) + ½H2(g) ⇌ Ag(s) + H+(aq) + Cl-(aq)
Nernst Equation: Ecell = E0cell - {RT/F}ln{aH+ aCl-},
for PH2 = 1 bar (which approximates to 1 atm., and where E0cell = E0Ag|AgCl (by definition of E0H+|H2 = 0V).
Consider the acid dissociation equilibrium for the ammonium ion:
NH4+(aq) ⇌ NH3(aq) + H+(aq)
The acid dissociation constant for this equilibrium is:
Ka = aNH3 aH+ / aNH4+
We notice from the cell diagram that [NH4+] = [NH3] = c.
Thus, Ka = aH+ fNH3 / fNH4+. We can assume that fNH3 = 1. This is very reasonable, because ammonia is an uncharged species. Therefore, Ka = aH+ / fNH4+, which implies that:
aH+ = fNH4+ Ka
Thus, E = 0.2223 - {RT/F}ln{c Ka fNH4+ fCl-}
Now, c < 10-2M, and so the DHL applies. (lg fi = -Azi2 I½) Since zi2 and I are the same for both NH4+ and Cl-,
fNH4+ = fCl- =f± (since HCl is a 1:1 electrolyte) = f
Hence, E + {RT/F}ln(c) - 0.2223 = +4.606RT A I½ / F - {RT/F}ln{Ka}
We now plot a graph of E + {RT/F}ln(c) - 0.2223 against I½ (= c½). This should be a straight line with ordinate-intercept -{RT/F}ln{Ka}.
c / M E / V c / mol dm-3/2 E + {RT/F}ln(c) - 0.2223 / V
0.00857 0.8965 0.09257 0.55198
0.01580 0.8824 0.12570 0.55359
0.02120 0.8757 0.14560 0.55464
0.03030 0.8661 0.18166 0.55620
From graph, ordinate-intercept = 5.5 x 10-1V mol-½ dm3/2
Therefore, Ka = 5.5 x 10-10 mol dm-3 (pKa = 9.26)
Kb refers to the forward reaction of the following equilibrium:
NH3 + H2O⇌ NH4+ + OH-
Now, Kw = 1.008 x 10-14 mol2 dm-6 = Ka Kb
Therefore, Kb = 1.008 x 10-14 / 5.5 x 10-10 = 1.7 x 10-5 mol dm-3
Hence, using ΔG0 = -RT ln Kb, ΔG0 = +27.2 kJ mol-1
Since ΔG0 = ΔH0 - TΔS0, ΔS0 = (4.53 - 27.2) x 10-3 / 298
ΔS0 = - 76.00 J mol-1 K-1
The protonation of ammonia by water is an entropically disfavoured reaction, a facet manifested in the negative sign of ΔS0. This is primarily due to the increased ordering of the solvent (water) around the ionic species formed. The unfavourable entropy of solvation combined with the positive (unfavourable) enthalpy of reaction, causes the Gibbs free energy for the (forward) reaction to be positive. Hence, ammonia is only a weak base in water at 298K.
The reader is advised to re-read pp. 91-92 before considering this solution.
Cell diagram:
Cd(amalgam, 4.6% Cd) | CdCl2(aq, cM) | AgCl(s) | Ag(s)
Potential determining equilibria:
RHE: AgCl(s) + e- ⇌ Ag(s) + Cl-(aq)
LHE: ½Cd2+ + e- ⇌ ½Cd(amal)
Cell Reaction:
AgCl(s) + ½Cd(amal) ⇌ Ag(s) + ½Cd2+(aq) + Cl-(aq)
The Nernst Equation for this cell reaction is: E = E0cell - {RT/F}ln {aCl- aCd2+½}
(where the activity of cadmium in the amalgam is taken to be unity).
aCl- = f-(2c) and aCd2+ = f+(c). Since c < 10-2M, we can use the DHL. The ionic strength of the solution, I = ½[ 4c +2c] = 3c. Since this is the same for both Cd2+ and Cl-, and since the ratio
zCd2+2/zCl-2 = 4, we can deduce that lg f+/lg f- = 4. ie., f+ = f-4. We can use this result to determine E0cell. However, it is easier and more convenient to use the mean ionic activity coefficient, f±, which is defined on p.63.
f± 3 = f-2 f+ = f-6
Hence, f± = f-2
Hence, aCl- = f±(2c) = f±[Cl-] and aCd2+ = f±(c) = f±[Cd2+]
Therefore,
E = E0cell - {RT/F}ln{f±3/2 (2)(c)3/2}
or,
E + {RT/F}ln{2c3/2} = E0cell - {3 RT/ 2F}ln{f±} (*)
or, using DHL,
E + {RT/F}ln{2c3/2} = E0cell - {6.909 RT A 31/2 / 2F} c1/2
We plot a graph of E + {RT/F}ln{2c3/2} against c1/2, and extrapolate to find the ordinate intercept (ie. a value for E0cell). The cell emf when aCd2+ = aCl- = 1 corresponds to Ecell.
c / 10-3 mol dm-3 E / V c1/2 / mol1/2 dm-3/2 E + {RT/F}ln{2c3/2} / V
0.1087 0.9023 0.01041 0.56861
0.1269 0.8978 0.01126 0.57007
0.2144 0.8803 0.01464 0.57277
0.3659 0.8641 0.01913 0.57715
From graph, ordinate-intercept = E0cell = +0.559V
(a). E0cell = E0Ag|AgCl - E0Cd|Cd(amal)
Therefore, E0Cd|Cd(amal) = 0.2222 - 0.559 = -0.3369V
Now consider the cell:
Cd(amal, 4.6% Cd) | CdCl2(aq, 0.5M) | Cd
E = -0.0534V
For this cell,
E0cell = E0Cd|Cd2+ - E0Cd2+|Cd(amal)
Cell Reaction is:
Cd2+(aq) + Cd(amal) Cd(s) + Cd2+(aq)
Thus, the Nernst Equation becomes: E = E0cell + {RT/ 2F} ln {aCd2+/ aCd2+}
E = E0cell
Hence, E0Cd|Cd2+ = -0.0534 + (-0.3369) = -0. 39V
Therefore, the S.E.P. for the Cd|Cd2+ couple is -0.39V
This result is consistent with the data supplied in Table 1.1 on p. 29.
(b). The Gibbs free energy of the formation of the hydrated ion Cd2+(aq) refers to the process:
Cd(s) → Cd2+(aq) + 2e-
But this process corresponds to the inverse of the Cd|Cd2+ S.E.P.
Since ΔG0 = -nFE0, and this process corresponds to a two electron transfer (n = 2),
ΔG0 = -(2)(96 490)(0.3903)
ΔG0 = -75.32 kJ mol-1
(c). Using the equation labelled with an asterix (*), we can deduce that the mean ionic activity coefficient (f±) of 0.2144 x 10-3 M CdCl2 is 0.701.
The standard electrode potential for the Cd/Cd2+ couple implies the following electrochemical cell
Pt|H2(g) (P=1 atm) | H+(aq) (a=1) ||Cd2+(aq)(aCd2+) |Cd
The corresponding half-cell reactions are
Right-hand electrode: 1/2 Cd2+(aq) + e- ⇌ 1/2 Cd(s)
Left-hand electrode: H+ (eq) + e- ⇌ 1/2 H2(g)
Accordingly, the formal cell reaction is
1/2 Cd2+(aq) + 1/2 H2(g) ⇌ 1/2 Cd(s) + H+ (eq) (eqn 1)
For which
△Go = -FEo
△Go = -0.400 F
Similarly, for
1/2 Cd[NH3]42+(aq) + e- ⇌ 1/2 Cd(s) + 2NH3 (aq) Eo = -0.610V
The formal cell reaction is
1/2 Cd[NH3]42+(aq) + 1/2 H2(g) ⇌ 1/2 Cd(s) + 2NH3 (aq) + H+ (eq) (eqn 2)
△Go = -FEo
= -0.610
Subtracting eqn 1 and 2 gives
1/2 Cd2+(aq) + 2 NH3(aq) ⇌ 1/2 Cd[NH3]42+(aq)
The Gibbs energy of the above ligand exchange reaction is
△Go = -F(-0.400 – (-0.610)) = -20.2kJmol-1
△Go = -RTln(K)
K = exp (20.2x103 / 8.31x298) = (a Cd[NH3]42+)1/2 / (a Cd2+)1/2 (a NH3)2
K = 3500
(i) The half-cell reaction for the anthraquinone monosulphonate redox-couple is
1/2 A(aq) + e- + H+ ⇌ 1/2 AH2 (aq)
which implies the following electrochemical cell
Pt|H2(g) (P=1 atm) | H+(aq) (a=1) ||A(aq)(aA), H+(aq) (aH+), AH2 (aq) (aAH2) |Pt
The corresponding Nernst equation is as follows noting that the hydrogen electrode above is standard
E = E0A/AH2 + RT/F ln[(aA1/2 aH+)/( aAH21/2)]
Since anthraquinone and anthrahydroquinone are neutral molecules and uncharged their activities can, to a good degree of accuracy, by approximated by their concentrations. The Nernst equation is simplified to
E = E0A/AH2 + RT/F ln[ ([A]1/2 aH+)/( [AH2]1/2) ]
(ii) The Nernst equation from (i) can be written as
E = E0A/AH2 + RT/F ln[ ([A]1/2 aH+)/( [AH2]1/2) ] + RF/T ln(aH+)
Substituting log10N = lnN/ln(10) into the above gives
E = E0A/AH2 + RT/F ln[ ([AH2]1/2)/( [A]1/2) ] + ln(10)RF/T log10(aH+)
Noting that pH = -log10(aH+), the Nernst equation can be written in terms of pH
E = E0A/AH2 + RT/F ln[ ([AH2]1/2)/( [A]1/2) ] + ln(10)RF/T pH
Differentiating the above equation with respect to pH gives
dE/d(pH) = -ln(10)RT/F
At 25°C, T = 298K.
dE/d(pH) = -ln(10) x 298 x 8.31 / 96485.3 = -59mV per pH unit
(iii) The generalised redox process
B + ne- + mH+ ⇌ BHm
can be written as an one electron half-cell reaction
1/n B + e- + m/n H+ ⇌ 1/n BHm
The Nernst equation for the generalised redox process is therefore
E = E0B/BHm+ RT/F ln[ (aB1/n aH+m/n)/( aBHm1/n) ]
E = E0B/BHm+ RT/F ln[ (aB1/n)/( aBHm1/n) ] + RF/T ln(aH+m/n)
E = E0B/BHm+ RT/F ln[ (aB1/n)/( aBHm1/n) ] + mRF/nT ln(aH+)
E = E0B/BHm+ RT/F ln[ (aB1/n)/( aBHm1/n) ] + mRF/nT log10(aH+)
Substituting in pH = -log10(aH+) gives
E = E0B/BHm+ RT/F ln[ (aB1/n)/( aBHm1/n) ] + mRF/nT pH
Differentiating the above equation with respect to pH gives
dE/d(pH) = - mRT/nF ln(10)
(iv) Acid dissociation constant, KA, for the dissociation reaction HA⇌ H+ + A- is given by
KA = aH+ aA- / aHA
(v) For A/AH2 system (e.g. anthraquinone/anthrahydroquinone), m = 2, n = 2
slope = dE/d(pH) = 2RT/2nF ln(10) = -59mV per pH unit
pKa1 (AH-/AH2) = -log(2x10-8)=7.7; pKa2 (A2-/AH-) = -log(1.2x10-11)=10.9
Accordingly, the reduced species (anthrahydroquinone) exists predominantly as AH2 for pH less than 7.7, as AH- in the pH range 7.7 to 10.9 and as A2- for pH > 10.9. Applying the results derived above leads to the following E – pH behaviour using the value n = 2 throughout but m = 0, 1 or 2 as appropriate.
(vi, vii)