Open access peer-reviewed chapter - ONLINE FIRST

Effects of Electrolyte on Redox Potentials

Written By

John R. Miller and Matthew J. Bird

Submitted: December 14th, 2021 Reviewed: February 2nd, 2022 Published: April 8th, 2022

DOI: 10.5772/intechopen.103003

IntechOpen
Redox Chemistry - From Molecules to Energy Storage Edited by Olivier Fontaine

From the Edited Volume

Redox Chemistry - From Molecules to Energy Storage [Working Title]

Prof. Olivier Fontaine

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Abstract

Redox potentials, especially as measured by cyclic voltammetry and related electrochemical techniques, are the basis for understanding energetics of photochemical solar energy storage, organic photovoltaics, light-emitting diodes, and even photosynthesis. These very popular techniques are dominant although none of the energy systems just mentioned contain large concentrations, typically 100 mM, of supporting electrolyte needed for electrochemical techniques to work. At the same time, the added electrolytes often have large, but unknown effects on the energetics studied. Despite substantial efforts using microelectrodes, it has not been possible to utilize electrochemical techniques to measure redox potentials in the absence of electrolytes. This chapter will be an account of new techniques applying the method of pulse radiolysis to partly answer the question: what is the effect of electrolytes on redox potentials?

Keywords

  • redox potentials
  • electrolytes
  • electron transfer
  • microelectrodes

1. Introduction

Redox potentials are essential to our understanding of energetics of photosynthesis, organic photovoltaics, dye-sensitized solar cells, redox catalysis, organic light-emitting diodes (LEDs), lithium and flow batteries, and respiratory electron transport cycles. Electrochemical methods such as cyclic voltammetry, polarography, and differential pulse voltammetry are the main sources of redox potentials. But to operate, these techniques require the addition of electrolyte, usually at concentrations near 0.1 M. The presence of electrolyte should stabilize radical cations or radical anion altering redox potentials from their true values in systems mentioned above, many of which contain no electrolyte.

Measurement of the effects of electrolytes on redox potentials has not been easy, but the advent of micro- and ultramicro electrodes enabled several groups to observe electrochemical waves at strongly reduced or even zero electrolyte concentrations [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13]. Still these waves are difficult to interpret to obtain values of ΔE°, the difference between the redox potential with, E°[XY] = 0.1 and without, E°[XY] = 0 electrolyte,

ΔE°=E°XY=0E°XY=0.1E1

Here XY is an inert, supporting electrolyte. A popular electrolyte is tetrabutylammonium hexafluorophosphate, TBAPF6. In our reading of the literature, we have yet to find even one report of the difference ΔE° for 0.1 moles/l (M) or any other concentration of electrolyte by electrochemical methods.

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2. What is the effect of electrolytes on redox potentials?

While reports of the change in redox potential due to addition of electrolyte are rare, some results from our laboratory became available recently [14, 15]. To introduce the concept of shifts of redox potentials, Figure 1 displays potentials for four couples, t-stilbene0/−, F100/−, Cocp2+/0, and Fecp2+/0 (referred to herein as Fc) in THF over a wide range of concentrations of the electrolyte TBAPF6. F10 is a ten-unit oligomer of 9,9-dihexyl fluorene. Results for Stilbene and F10 used only experimental data. Those for Cocp2 and Fecp2+/0 used experiment and computations and may thus be slightly less reliable.

Figure 1.

The variation of redox potentials with the concentration of electrolyte, TBAPF6, from [TBAPF6] = 0 to 1.0 M. The position of E°(Fc) is marked.

Figure 1 displays the potentials of the four species vs. the reference of an electron in vacuum (left axis) or the aqueous saturated calomel electrode (right axis) SCE. These two external references remain constant as electrolyte is added. Table 1, below, on the other hand, uses the internal ferrocene (Fecp2) as reference, while keeping the reference constant by always using it in 0.1 M TBAPF6. Methods for establishing and comparing reference potentials are described in the section Reference couples and electrodes.

ElectrolyteaKd (M)bE°vs. E°XY=0.1cE°XY=0cΔE mVRef
Stilbene0/−TBAPF63.1x10−6−2.72−2.85129[14]
F100/−TBAPF61.8x10−3−2.62−2.6417[14]
1-MePyreneTBAPF64.2x10−6−2.60−2.73128[14]
Cocp2+/0TBAPF61.4x10−6−1.33−1.48151b
Fecp2+/0TBAPF64.1x10−700.183183b
Per0/−TBAPF65.9 x 10−7−2.21−2.38174[15]
BzPh0/−TBAPF66.3 x 10−8−2.32−2.55232[15]
Per0/−NaBPh42.3 x 10−5−2.26−2.38124[15]
BzPh0/−NaBPh46.8 x 10−11−2.10−2.55451[15]
Per0/−{Na}BPh46.4 x 10−5−2.28−2.38100[16]
BzPh0/−{Na}BPh42.2 x 10−5−2.38−2.55173[16]

Table 1.

Dissociation constants, Kd, and redox potentials in THF. Redox potentials are vs. Fc (Fecp2+/0) with 100 mM TBAPF6.

Electrolytes are tetrabutylammonium hexafluorophosphate (TBAPF6, Kd = 2.7 x 10−6 M, [17]) sodium tetraphenylborate (NaBPh4, Kd = 8.8x10−5 M [18]) and sodium tetraphenylborate with the Na+ encapsulated in the 222-cryptand ({Na}BPh4, Kd = 9.3.x10−5 M [15]). MePy is 1-methylpyrene, Per is perylene, BzPh is benzophenone.


Kd for (Cocp2+, PF6) and (Fecp2+, PF6) were estimated from measured [14] Kd’s for Stilbene and MePyrene and the ratios of computed Kd’s for those to computed Kd’s for (Cocp2+, PF6) and (Fecp2+, PF6). cE°is the reduction potential in 0.1 M electrolyte vs. Fc in THF with 0.1 M TBAPF6. E°is the reduction potential without electrolyte, also vs. Fc in THF with 0.1 M TBAPF6. Potentials vs. Fc in THF with no electrolyte are more negative by 0.185 V.


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3. Redox potential shifts by ion pairing and activities

When electrolyte is added, two factors shift redox potentials: 1) ion pairing and 2) activity.

Both are pictured in Figure 2 and included in Eq. (2), below. In Figure 2, one positively charged ion of the electrolyte is close to the radical anion, forming an ion pair. Other ions of the electrolyte contribute to the ionic atmosphere. In highly polar media such as water or acetonitrile, there is little ion pairing and most electrolyte exists as free ions. Ionic atmospheres around radical anions or cations stabilize them, described as change of their activities, γ, calculated [14] here using extended Debye-Hückel theory. In these calculations in redox potential, the component attributed to activities is usually small. For 100 mM TBAPF6 estimates of the shift from activities are 18 mV in THF and 24 mV in acetonitrile using Kd’s for TBAPF6 from LeSuer, Buttolph, and Geiger [17].

Figure 2.

A radical ion (red oval) in solution surrounded by + and – ions of an electrolyte.

Shifts of redox potentials in Figure 1, calculated by Eq. (2), are much larger. The data in Figure 1 are in THF, where ion pairing can produce large changes in redox potentials.

E°XYE°XY=0=RTFln1γ±+γ±X+Kd°MX+E2
E°XYE°XY=0=RTFln1γ±+γ±YKd°M+YE3

Eq. (2), derived in Ref., [14] gives the change in redox potential with concentration of the electrolyte, XY, in terms of a dissociation constant, Kd, and an activity coefficient, γ±. The free electrolyte concentrations, [X+] or [Y], are found using the dissociation constants for the electrolyte in THF. It is derived by applying the Nernst equation in the presence of an ion-pairing equilibrium. Reference [14] also presents data used to obtain the parameters needed in Eq. (2). That data also examines and supports the model of Eq. (2). Eq. (2) is for reduction of molecule M to M˙ (e.g., Stilbene˙; (3) is for reduction of M˙+ (e.g. Cocp2˙+) to M. Qu and Persson [19] gave an equation similar to Eq. (2), although without effects of activity.

Ion pairing is strong in media of lower polarity. The shifts of redox potentials in Figure 1 and Table 1 (below) are in THF, a liquid of moderately low polarity with a dielectric constant ε = 7.6. With this low polarity, Eq. (2) predicts the ion-pairing contribution to shift redox potentials by amounts that are generally much larger than that due to activity (∼18 mV). A notable exception is the case of the highly delocalized anion of F10, to be discussed below. This is especially evident for the case of the largest shift, 451 mV for benzophenone radical anion paired with Na+. In that case, the small Na+ ion pairs strongly with the negative charge concentrated on the ketone of benzophenone. The shift is smaller by almost a factor of 2 for pairing with TBA+ and still smaller with Na+ encapsulated in the 2.2.2. cryptand.

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4. Methods to measure redox potentials with and without electrolyte

While we yet look forward to the possibility of measurements of redox potentials without electrolyte by electrochemistry at micro and ultramicro electrodes, two methods using pulse radiolysis have emerged from our laboratory. Both measure electron transfer equilibria without electrolyte and with electrolyte, studying electron transfer from a radical anion, D•− to an acceptor, A, under conditions where the equilibrium can be observed and the equilibrium constant, Keq, measured. Creating D•− by pulse radiolysis (Figure 3) enables determination of Keq.

Figure 3.

A spectrophotometric cell containing a solution. In our accelerator, LEAF, 9 MeV electrons enter one side of the cell creating ionizations in the solution. Each ionization is followed by secondary and tertiary ionizations.

In Figure 3, ionizations create electrons and holes, which add to solutes to create radical ions. In some liquids, such as THF, only radical anions are created. Radical cations can be created in other liquids. When an inert electrolyte is added, the electron transfer equilibrium is coupled to two ion-pairing equilibria as shown in Figure 4.

Figure 4.

An electron transfer equilibrium coupled to two ion-pairing equilibria with inert ion X+. Kdd and Kda are dissociation constants for the ion pairs of D•− and A•− with the counter-ion of the electrolyte.

4.1 Method 1

If the two ion-pairing equilibria have the same dissociation constants, Kdd = Kda, then the apparent “composite” equilibrium constant, KeqC, does not shift as electrolytes are added. If D•− and A•− have different Kd’s for pairing with counter ions of the electrolyte, then KeqC, shifts as electrolyte is added. KeqC is the equilibrium constant between all D- species and all A- species. The system of three coupled equilibria has a simple, analytic solution under appropriate conditions, enabling the measurements of as a function of electrolyte concentration to be fit to yield Keq, Kdd, and Kda. Eq. (2) then gives the shifts of redox potentials for both D0/− and A0/− [14]. The good fit to the equations describing this mechanism also serve to validate the mechanism.

This method is very general requiring only that Kdd and Kda are substantially different. A difference of a factor of 10 is sufficient. It also needs either D•− or A•− to have a readily measurable absorption spectrum. An aspect of the generality of this method is that it enables determination of dissociation constants of radical ions with anycounter ion, e.g., TBA+. Figure 5 presents an example of data using this method.

Figure 5.

Measurement of KeqC for electron transfer from MePy•− to F10 as a function of electrolyte concentration. Transient absorption at 1574 nm where only F10•− absorbs in THF a) without electrolyte and b) with 0.1 M TBAPF6. c) KeqC from the transient absorption data and d) the redox potentials for MePy and F10.

Previously, Szwarc determined Kd’s for pairs like (biphenyl•−, Na+) by conductivity, but the prior methods were applicable only to alkali metal ions. Reports in Table 1 of example like Kd(stilbene•−, TBA+) in Ref. [14] are new. The method can be readily generalized to equilibria of radical cations.

4.2 Method 2

A second method uses thermodynamic cycles like that in Figure 6. This cycle was constructed from measured equilibrium constants in THF for electron transfer from perylene to benzophenone,

Figure 6.

Free energy cycle for electron transfer from Per˙ to BzPh in THF without and with NaBPh4 electrolyte.

Per+BzPhPer+BzPhE4

In Figure 6, the top segment is the measured free energy change for reaction [4] without electrolyte; the bottom is the free energy change with NaBPh4 added. Strong ion pairing in (BzPh˙, Na+) changes the reaction from endoergic (ΔG = +171 meV) to exoergic (ΔG = -155 meV) in the presence of sodium. Kd(Per˙, Na+) measured by Slates, and Szwarc [20] specifies the left segment, while the cycle yields the right segment, giving Kd(BzPh˙, Na+) = 6.8 x 10−11 M.

The measurement of this the very small Kd(BzPh˙, Na+) illustrates the power of Method 2 for select cases, although this method can work only when external data supplies one segment of the cycle, in this case Kd(Per˙, Na+) measured by conductivity [20], which gives the left leg of the cycle.

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5. Reference couples and electrodes

IUPAC recommended reporting of redox potentials relative to the internal ferrocenium/ferrocene reference (Fc) [21]. Our measurements to obtain redox potentials in THF at small or zero electrolyte concentrations [14, 15] used the determinations of Shalev and Evans [22] to reference our measurements to Fc in THF with 100 mM TBAPF6. Potentials in Table 1 use this reference, which we will call Fc(THF, TBAPF6). Common reference electrodes are SCE, the standard hydrogen electrode, silver ion (Ag), Ag/AgCl, and internal references. In Figure 1, we referred potentials to the electron in vacuum and aqueous SCE because these do not shift with electrolyte concentration. Here we applied Connelly and Geiger’s finding that Fc(THF, TBAPF6) is 0.56 V vs. SCE [23] and references for vs. e- in vacuum [24, 25].

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6. Redox and reference shifts

Figures 5 and 7 graph redox potentials with two difference references.

Figure 7.

Shifts of redox potentials for reduction in THF for benzophenone (BzPh), t-stilbene and F10 vs. the fixed reference of Fc(100 mM TBAPF6).

In Figure 7, we see that the redox potential of BzPh0/− increases more rapidly with TBAPF6 concentration than either that Stilbene or F10. In the presence of Na+ ions, the redox potential increases still more rapidly and the increase begins even before the 10−9 M limit in the graph.

In Figure 7, the redox potential of F100/− changes little due to the remarkably large Kd(F10•−, TBA+) = 1.8x10−3 M. The weak association in this pair is due to weak electrostatic attraction of the positively charged TBA+ ion to the highly delocalized charge distribution of F10•− in the (F10•−, TBA+) pair. Figure 8 shows the computed ion pair using density functional theory (b3lyp/6–31 + g*) in Gaussian 16 [27] with the SMD solvation model for [28] THF.

Figure 8.

Pairing of the TBA+ ion with the very delocalized charge in the anion of F10 rendered by Gaussview [26].

The redox potential of F100/− changes more in Figure 9 where the reference is Fc at each electrolyte concentration. Most of this change is notdue to changes in the potential of F100/−, but to changes in the Fc reference potential with increasing TBAPF6 concentration. Vullev and coworkers emphasized the effect of electrolyte on the potential of ferrocene [29].

Figure 9.

Shifts of redox potentials for reduction in THF of t-stilbene and F10 vs. the variable reference of fc[TBAPF6]; at each concentration [TBAPF6] the reference is Fc at that concentration. The position of E°(Stilbene) is marked.

In Figure 10, the redox potentials of benzophenone (BzPh) and Perylene (Per) depend differently on the NaBPh4 electrolyte concentration due to very different Kd’s (Table 1), but the two curves are almost parallel at large [NaBPh4]; the difference between the two changes by only 11 mV from [NaBPh4] = 10−4 M to 0.1 M. This constancy occurs because changes in redox potential due to ion pairing are constant at 59 mV per decade of counter ion concentration once the onset of the effect occurs.

Figure 10.

Redox potentials of BzPh and per vs. NaBPh4 concentration.

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7. Conclusions and prospects

The effect of electrolytes on redox potentials is now becoming known. Those effects are expected to be small in polar media where ion pairing is not strong and very large in nonpolar media where ion pairing is expected to be very strong. This chapter describes effects of electrolytes in a liquid of medium polarity, THF (ε = 7.6), in which the measurements are moderately challenging, but possible using new methods based on pulse radiolysis.

A principal contributor to redox potentials dissociation constants, Kd, for radical ions paired with counterions from the electrolyte. Few of these are known in the literature, but this work also reported several of these. The two methods described above used pulse radiolysis to determine Kd’s from 6.8 x 10−11 to 1.8 x 10−3 M.

In addition, these pulse radiolysis methods will enable testing of new internal references and “weakly coordinating” anions [30, 31] and cations [32], which could lead to better candidates for use in electrochemistry, particularly in low-polarity solvents. Furthermore, these methods enable the measurement of referenced redox potentials in the absence of electrolyte and can go beyond typical electrochemical potential windows [33].

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Acknowledgments

This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences & Bioscience, through Grant DE-SC0012704, including use of the LEAF and Van de Graaff facilities of the BNL Accelerator Center for Energy Research. We are grateful to Tomokazu Iyoda, Matthew Pearson, Abram Ledbetter, and Nick Bonura for their contributions to references [14, 15].

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Appendices and nomenclature

E°′[XY] = 0.1is the redox potential in 0.1 M of electrolyte, XY.
E°′[XY] = 0.0is the redox potential without electrolyte.
ΔE°′is the difference between the redox potential with and without electrolyte,
KeqCis the composite equilibrium constant for an electron transfer coupled to two ion pairing equilibria (see Figure 4).
Mis the concentration in moles/l.

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Written By

John R. Miller and Matthew J. Bird

Submitted: December 14th, 2021 Reviewed: February 2nd, 2022 Published: April 8th, 2022