Cyclic Voltammetry Applications and Uses
Cyclic voltammetry is a versatile electrochemical method with a range of different applications. In cyclic voltammetry, each successful forwards and backwards potential sweep produces a 'duck-shaped' plot known as a cyclic voltammogram. From this, you can find lots of information about the material and its electrochemical response.
Broadly speaking, the most useful values that can be obtained from a cyclic voltammogram are the anodic and cathodic peak currents and potentials, the polarographic half-wave potential, and the oxidation and reduction onset potentials. In materials science, this data can be used to probe qualitative and quantitative information about the electrochemical properties of chemicals. Cyclic voltammetry is often used to investigate the reversibility of a reaction, describe electron transfer kinetics, approximate the energy levels of semiconducting polymers, and more.
By comparing measured data with known data, cyclic voltammetry can be also used to detect the presence of a material in sample. It is therefore sometimes used for environmental testing (for example, for measuring the amount of lead in drinking water) or for medical applications (such as measuring the amount of iron in a sample of blood).
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Contents
- How to perform cyclic voltammetry
- How to read a cyclic voltammogram
- Determining the reversibility of a reaction
- Determining the formal reduction potential of a species
- Measuring electron transfer kinetics
- Determining the energy levels of semiconducting polymers
- Determining the absolute energy of semiconductors
- Assignment and characterisation of coupled reactions
How to Perform Cyclic Voltammetry
Like other types of voltammetry, cyclic voltammetry uses a three electrode system consisting of a working electrode, reference electrode, and counter electrode. During a scan, a potentiostat linearly sweeps the potential between the working electrode and reference electrode while measuring the current between the working electrode and counter electrode. The potential is swept in both directions (within the defined potential range) for the set number of cycles.
To set up and run a cyclic voltammetry scan with the Ossila Potentiostat:
- Switch on the potentiostat ~30 minutes before use to allow it to warm up and reach a stable temperature
- Add the reference solution to the reference electrode tube with a syringe and needle until it is approximately two-thirds full
- Clean the working and counter electrodes using the same solvent as used for the electrolyte
- Place a droplet of solution containing the sample onto the tip of the working electrode and allow it to dry
- Insert each electrode into the electrochemical cell cap
- Gently bubble inert gas through the solution for ~10 minutes using a thin tube or needle to remove dissolved oxygen
- Connect the electrochemical cell to the potentiostat using crocodile clips
- Start the software and set the current and potential ranges to appropriate values for the sample in question
- Withdraw the degassing tube/needle and start the measurement via the software
Successful cyclic voltammetry measurements produce a 'duck-shaped' plot known as a cyclic voltammogram. Analysis of the cyclic voltammogram reveals information about the sample.
How to Read a Cyclic Voltammogram
Reading a cyclic voltammogram is relatively straight-forward. The diagram below shows a cyclic voltammogram for ferrocene as measured by an Ossila Potentiostat. Labels have been added to show key data points.
Charging currents and uncompensated resistance
In addition to the resistance from the redox reaction taking place on the surface of the working electrode, electrochemical cells also exhibit solution resistance between the working electrode and reference electrode. The size of this resistance can be minimised by placing the working electrode close to the reference electrode. It is impossible to completely eliminate solution resistance in a cell so when reading a cyclic voltammogram, it is important to consider the effects of uncompensated resistance. Large uncompensated resistance can falsely make a reaction look quasi-reversible or irreversible.
A second effect that can affect the reading of a cyclic voltammogram is from charging currents. Charging currents can be minimised by decreasing the scan rate or using a working electrode with a smaller surface area, but it is generally preferable to subtract them from the data. This can be done to first approximation by either subtracting the current observed when no redox reactions occur or by taking a cyclic voltammogram without the sample of interest present and subtracting the results of this scan from the cyclic voltammogram of the redox event. Neither of these approaches is valid at extremely fast scan rates [1] but they are useful approximations for cyclic voltammetry experiments at "normal" scan rates. After charging currents have been subtracted, the baseline (pre-redox event) should be equal to the zero-current line. I_{pa} and (I_{pa})_{0} should therefore be equal. Although the charging currents in the cyclic voltammogram shown above are small, the labels would only be numerically accurate after they have been subtracted from the data.
Anodic peak current and anodic peak potential
The anodic peak current (I_{pa}) occurs at the anodic peak potential (E_{pa}) and is measured relative to an extension of the baseline in the zero-current region. In the IUPAC convention for cyclic voltammograms, the anodic peak current is positive.
Cathodic peak current and cathodic peak potential
The cathodic peak current (I_{pc}) occurs at the cathodic peak potential (E_{pc}) and is measured relative to an extension of the reverse sweep baseline. This is more difficult to obtain than the forward sweep baseline; its shape resembles a reflection of the voltammogram had the direction of the scan not been reversed. The reverse sweep baseline can be approximated mathematically, or alternatively, the ratio between the cathodic and anodic peaks can be approximated using the Nicolson parameter. To do this, the absolute cathodic peak current ((I_{pc})_{0}) and absolute current at the switching potential ((I_{sp})_{0}) need to be measured. The absolute cathodic peak current is taken relative to zero-current rather than the baseline, and hence is easier to determine than I_{pc}. For a reversible reaction, the cathodic peak will be of equal magnitude to the anodic peak, but with the opposite sign.
Polarographic half-wave potential
The polarographic half wave potential (E_{1/2}) is often used to approximate the formal and standard potentials. For reversible or quasireversible reactions, it can be approximated as the average of the peak cathodic and anodic currents.
Oxidation and reduction onset potentials
The oxidation onset potential (E_{onset}) is the potential at which the analyte oxidises at the surface of the working electrode, causing the current to increase exponentially on the cyclic voltammogram until it reaches the anodic peak current. A similar point (not shown) on the cathodic peak exists for the reduction onset potential. Onset potentials correlate with the HUMO and LUMO energies of a material and are sometimes used instead of the half-wave potential when determining the potential of a redox event.
IUPAC convention vs. US convention for cyclic voltammograms
There are two main conventions for cyclic voltammograms; the International Union of Pure and Applied Chemistry (IUPAC) convention and the US (or “classical”) convention. The cyclic voltammogram above uses the former. In the IUPAC convention, the oxidative potential sweep runs from left (negative values) to right (positive values) along the x-axis. Conversely, the reductive sweep runs from right to left. On the y-axis, the anodic peak is positive and the cathodic peak is negative.
In the US convention, the cyclic voltammogram is - in effect - rotated by 180 degrees compared to the IUPAC convention. The x-axis runs from positive values to negative values, showing increasing reduction left to right and oxidation from right to left. In this convention, the anodic peak is negative and the cathodic peak is positive. This changes the form of some of the equations (e.g. the Nicholson Parameter) on this page. Both conventions are common in the literature so care should always be taken when working with cyclic voltammetry.
Determining the Reversibility of a Reaction
What determines the reversibility of a reaction?
The reversibility of a reaction can be split into two metrics, chemical reversibility and thermodynamic reversibility.
- If an electron transfer can be reversed without any side reactions (either before or after) then it is said to be chemically reversible
- If the rate of electron transfer is sufficient that equilibrium is maintained, then it is said to be thermodynamically reversible
- If both thermodynamic and chemical reversibility are observed, the electron transfer is said to be reversible i.e. there is practical reversibility
Practical reversibility does not necessarily mean that no side reactions ever occur, or that the system cannot be perturbed from equilibrium; it only requires equilibrium and a lack of side reactions on the time scale of the experiment. For example, a reaction would still be considered reversible if the oxidised compound slowly degrades over time, providing that a sufficient scan rate (rate of potential change) is used. Similarly, even if thermodynamic equilibrium is not maintained at very fast scan rates, the reaction is still considered reversible if it is maintained during the cyclic voltammetry experiment.
Linear diffusion
All the equations on this page assume linear diffusion. Most electrodes can be approximated as having linear diffusion on short time scales. The larger the electrode, and the shorter the time observed, the more the linear diffusion approximation applies.
How to determine the reversibility of a reaction
Cyclic voltammetry can be used to measure two parameters, which can together can be used to determine if a reaction is reversibly for a given scan rate. These are:
- The difference in the potential difference between the anodic peak current and the cathodic peak current
- The height of the anodic and cathodic peaks relative to the baseline [3] (note: for the reverse peak, the baseline after the electron transfer is used [4])
The Nicholson parameter
For an oxidation, the height of the peak cathodic current (i_{pc}) can be hard to determine, and likewise, the peak anodic current can be difficult to determine for a reduction. As a result, a variety of methods are used for determining the ratio of the cathodic and anodic peaks. To do so from a single experiment without fitting the curve, the Nicholson parameter is often used. [4] [5]
In this equation, i_{sp} is the absolute current at the switching potential, i_{pc} is the absolute current at the cathodic peak potential, and i_{pa} is the absolute anodic peak potential. The (…)_{0} notation simply indicates that the currents are taken relative to the i=0 line.
The Nicholson parameter only gives accurate results when the switching potential is 60/n mV past the peak anodic potential for an oxidation, and -60/n mV for a reduction. [4] [5]
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Charging currents
When measuring the currents required to calculate the Nicholson parameter, the charging currents need to be neglected. In cyclic voltammetry, these are approximately constant for each linear sweep, but their direction changes depending on the direction of the sweep. It is this effect which leads to hysteresis in the cyclic voltammogram when no reduction or oxidation occurs (i.e. in the absence of redox active species).
To first approximation, the charging currents can be neglected simply by running a voltammogram without redox active species present and subtracting the results from the actual voltammogram. Alternatively, they can be subtracted by looking at the steady current when no redox reactions occur, and subtracting this for forward and reverse runs.
Though they do improve the quality of the results obtained, neither of these approaches are perfect. Specifically, both methods are prone to errors at faster scan rates, such as those which are accessible at ultramicroelectrodes [1].
Uncompensated resistance is the resistance to charge flowing outside the electrochemical process at the electrode. Large uncompensated resistance resulting from the movement of charges in solution can make the system look quasireversible or irreversible, even when it is not.
More accurate results can be obtained from fitting the system with more complex equations [2] [9] or by using specially designed instruments. [1]
Reversible reactions
For a reversible reaction, i_{pa}/i_{pc}=1, and E_{pa}-E_{pc}=0.52/n V for an oxidation, and -0.52/n V for a reduction, where n is the number of electrons in the oxidisation or reduction. [3]
Quasireversible systems
A quasireversible system is where the scan-rate and the electron transfer rate compete, such that thermodynamic equilibrium is never reached. A cyclic voltammogram which still has both anodic and cathodic peaks, but does not have E_{pa}-E_{pc}=0.52/n is considered quasi-reversible.
Irreversible reactions
If the reverse peak is missing, an electron transfer is classified as irreversible. Note that if i_{pa}/i_{pc}≠1, then the reaction is not chemically reversible. This suggests that another reaction is taking place in addition to the oxidation and reduction of the compound (i.e. O+n e^{-}⇌R). When additional chemical reactions occur, there is said to be coupled reactions.
Determining the Formal Reduction Potential of a Species
The formal potential is a measure of the potential of a cell where both oxidised and reduced species are present at equal concentration. The formal potential is defined via potentiometry, which involves measuring the potential difference in a galvanic cell, but can be approximated with cyclic voltammetry.
How to determine the formal potential with potentiometry
In a galvanic cell, there is a solution of one redox pair with an electrode on the left, and another solution of another redox pair on the right. The solutions are connected such that ions can move between the solutions in order to maintain a charge balance. A potential difference can be measured between these two solutions and is given a positive sign if reduction occurs spontaneously at the right electrode, and oxidation at the left electrode, when the electrodes are allowed to discharge. If the oxidation were to occur at the right electrode, and reduction at the left electrode, then a negative sign would be given.
In a standard three electrode setup, the reference electrode is considered the "left electrode", and the potential of other species is measured relative to it. The measured potential difference is often referred to as the electromotive force, or EMF, but this is no longer a recommended term. [1]
The Gibbs free energy
This potential difference is related to the Gibbs free energy, which corresponds to the overall reaction when there is oxidation at the left electrode and reduction at the right electrode.
The Gibbs free energy can be calculated using the following formula:
The standard potential and standard reduction potential
The "standard potential" is the potential where all species are present with unit activity. In order to make a set of comparable standard potentials, the standard potential where a set standard is oxidised was created. The "standard reduction potential" is the "standard potential" where the reference electrode is the normal hydrogen electrode.
It is possible to calculate the standard potential of a cell (E_{cell}^{0}), from the standard reduction potential of the redox couples on the left (E_{left}^{0}) and the right (E_{right}^{0}). The standard potential, i.e. the potential where all compounds are present under standard conditions, is given by the following:
The EMF of a cell with non-unit activity (E) can be related to the standard potential (E^{0}) using the following formula, where a_{x} is the activity of compound x, n the number of electrons involved in the oxidation/reduction, and T is the temperature:
The formal potential
Because the standard potential requires knowledge of the activity constant of the oxidised and reduced compound, it is quite complicated to calculate. As such, the formal potential (E^{0'}) is frequently used instead. This is given by the following formula, where symbols are defined as previously defined, [X] is the concentration of compound X, and X is its activity constant.
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How to approximate the formal potential with cyclic voltammetry
To approximate the formal potential with cyclic voltammetry, the polarographic half wave potential E_{1/2} is often calculated. For a reversible (or quasireversible) reaction, this can be approximated as the average of the peak cathodic and anodic currents. [4] [6]
The halfwave potential can be calculated more accurately by polarographic type methods, but in cyclic voltammetry, an accuracy of the order of mV is observed for a reversible reaction. [4] [6]
The halfwave potential (E_{1/2}) is related to the formal potential (E^{0'}), which in turn is related to the standard potential (E^{0}). The relationship is shown below, where a_{m} is the activity of species m, [m] is the concentration, γ_{m} is the activity coefficient, and D_{m} is the diffusion constant.
In practice, the difference between E_{1/2} and E^{0'} is minimal. [4] As such, it is quite common to approximate E_{1/2}=E^{0'}.
Measuring Electron Transfer Kinetics
The kinetics of the electron transfer are often characterised in terms of the standard rate constant k^{0}. k^{0} is the rate constant of both oxidation and reduction when the electrode is at the formal potential i.e. when E=E^{0'}.
How to calculate the standard rate constant with the method of Nicolson
The standard rate constant can be calculated using the "method of Nicholson",[1] if the diffusion constant of the species in solution is known. In his 1965 paper,[7] Nicholson calculated the separation of peak cathodic and anodic current for a reduction for various values of ψ:
Here, D_{o} is the diffusion constant of the oxidised species, D_{R} of the reduced species, v is the scan rate, n is the number of electrons involved in the oxidation/reduction, α is the transfer coefficient (see Butler-Volmer equation), T is the temperature, F is the faradays constant, and R is the gas constant.
It is possible to look up a value of ψ for a known separation of anodic peaks, and if all other constants are known, this value can then be used to calculate a value of k^{0}. In addition, the diffusion constants of oxidation and reduction are usually found to be similar, so it is sometimes considered valid [7] to approximate:
It should be noted these results are only reliable [7] for 0.3<α<0.7, but this is commonly true.
For a reduction, as opposed to an oxidation, the same basic process applies.
A problem with this method is that the uncompensated resistance (resistance to charge flowing outside the electrochemical process at the electrode) can dominate the cyclic voltammogram. [1] [7] The uncompensated resistance is particularly an issue when reversibility is approached, and as such resistance in solution should be minimised.
Determining the Energy Levels of Semiconducting Polymers
A commonly used method for determining the energy levels of organic semi-conducting polymers with cyclic voltammetry is to deposit the polymer on the working electrode and measure the electrical response
Depositing a solid on an electrode forms what is referred to as a modified electrode.[1] The onset potential is usually then calculated, and this value is assigned as the energy of the HOMO and LUMOs.
The evidence for this method comes from a paper [2] which tested the ability of Valence Effective Hamiltonian (VEH) to calculate redox potentials. In the paper, the onset potential and gas phase ionisations energies were observed to correlate with VEH calculated HOMO and LUMO. However, the absolute values show absolute error of the order of 0.1 V, in opposite directions for the two experimental techniques. Based on this evidence, the onset potentials are often used to calculate the HOMO and LUMO energies more generally. Here, HOMO is being used to mean the highest energy electron in the solid state, and LUMO the lowest energy excited electron (different from a theoretical description of HOMO and LUMO).
A modern electrochemical review, [8] discourages the use of this method, claiming that onset potential "are not standard potentials, and do not posses thermodynamic significance".
Determining the Absolute Energy of Semiconductors
By using cyclic voltammetry to measure the potential at which redox events occur relative to a reference, it is possible to determine the energy levels at which a redox couple interconvert relative to a free electron in vacuum. This is known as the absolute energy of the oxidation or reduction.
Limitations of cyclic voltammetry
Cyclic voltammetry is not perfect for identifying the electron affinity and ionisation energy of films as it takes place in solution rather than across the material vacuum interface. As a result, while a correlation between cyclic voltammetry data and the electron affinity and ionisation energy clearly exists, there remains some uncertainty as to its accuracy [9] [10].
Determining the potential of a redox event
There are several different ways to determine the potential of a redox event. The preferred way, given that the standard potential is extremely hard to determine experimentally, is by using the half-wave potential.
Due to their correlation with the HOMO and LUMO energies, it is common to use onset potentials instead of the half-wave potential [2] [11]. It is often said that the onset gives the "band edge" of the material, but this is dI_{sp}uted in the literature (a modern review claims that there is no thermodynamic significance to the onset, that it is a frequent source of error, and that optical and electrical band gaps differ significantly in their solvation properties [8]).
A recent article on cyclic voltammetry compares several different approaches to determining the formal potential in the case of chemical and thermodynamic irreversibility [12]. For irreversible reactions, the inflection point appears to be the best alternative to the half-wave potential [12].
Evidence is also presented that the average of cathodic and anodic peaks (i.e. the half-wave potential) remains the best measure if cathodic and anodic peaks are present [12]. As such, according to this research, the inflection point is only useful when the reverse peak is missing and hence the half-wave potential can not easily be determined [12].
There are two different methods for calculating the absolute potential in the literature. Both are discussed below. The first method is the most common method, but the second is arguably more scientifically rigorous.
Method 1
The following general equation can be used to convert between potentials relative to ferrocene (E_{1/2}) and the absolute energies of a redox event (E_{abs}).
In this equation, E_{abs} is the absolute potential and E_{abs(Fc/Fc+)} is the ferrocene/ferrocenium absolute potential. The △E_{solv} factor corrects for E_{1/2} and E_{abs(Fc/Fc+)} being measured in different solvents, and is usually approximated to be zero.
The sign convention used here is dictated by the definitions of the standard potential (approximated by the half-wave potential) and the absolute potential. Other sign conventions exist, so caution should be used when applying these equations.
Ferrocene as an internal standard
The use of ferrocene as an internal standard is complicated because several different absolute energies are in common use. In addition, it has been experimentally observed in a number of studies that the ferrocene oxidation/reduction is dependent on solvent choice [13] [14].
The standard potential assumes standard conditions, and is defined by how easily reduction takes place in a system. The absolute energy is a measure of the change in energy of the system when an electron is taken off a compound. A more positive absolute energy suggests that less energy is needed to lose an electron, and a more positive standard potential suggests that more energy would be released by reduction (electron gain) of the redox pair when connected to the normal hydrogen electrode (losing an electron is harder).
Three different absolute energies for the oxidation of ferrocene (E_{abs(Fc/Fc+)}) have been calculated by combining the absolute energies of a reference electrode with the relative value of the ferrocene/ferrocenium reduction [11]. For ferrocene in acetonitrile, these are E_{Fc/Fc+} = -4.8, -5.1, and -5.39 V.
All three of these energies are in common use, but the value of 4.8 V may be incorrect owing to an error in the value used for the ferrocene potential and a miscalculation of the standard cadmium electrode absolute energy [11]. The values of -5.1, and -5.39 V may also be disputed because it is unclear how scientific data for the absolute potential of the references are combined. The method used appears to differ from results which may be obtained by thorough ways of averaging data, such as averages weighted upon the standard deviation.
Method 2
The following equation is an alternate way to calculate the absolute energy of a redox event [9] [10].
Here, E_{abs(std)} is the absolute potential of a standard and c is a constant. Values for c and E_{abs(std)} can be obtained by fitting ultraviolet photoemission spectroscopy (UPS) [9] and inverse photoelectron spectroscopy (IPES) [10] to cyclic voltammetry data.
Values from the literature [9] [10] for the formation of M+ in a solution of M (oxidation) and the formation of M- in a solution of M (reduction) relative to ferrocene in dimethylformamide are given in the table below.
c | E_{abs(std)} | |
---|---|---|
Oxidation | 1.4 ± 0.1 | 4.6 ± 0.08 |
Reduction | 1.19 ± 0.08 | 4.78 ± 0.17 |
Note that while the value of E_{abs(std)} differs slightly as a consequence of the fitting [9], the above assumes E_{Fc/Fc+} = -4.8V. This value is disputed [11]. In addition, there is some evidence for changes in both E_{abs(std)} and c between solvents [9].
Assignment and Characterisation of Coupled Reactions
Cyclic voltammetry can also be used to assign coupled reactions to the electrochemically formed species. By examining the shape and plotting the dependence on peak position, and i_{pa}/i_{pc} on scan rate, the processes which occur can be characterised. [3] [4]
References
- A. L. Bard and L. Faulkner Electrochemical methods: Fundamentals and Applications, 2nd ed. John Wiley & Sons 2001
- J. L. Brédas, R. Silbey, D. S. Boudreaux, and R. R. Chance Chain-Length Dependence of Electronic and Electrochemical Properties of Conjugated Systems: Polyacetylene, Polyphenylene, Polythiophene, and Polypyrrole J. Am. Chem. Soc., vol. 105, no. 22, pp. 6555–6559, 1983
- J. Heinze, Angew. Chemie Int. Ed. English, 1984, 23, 831–918
- G. A. Mabbott, J. Chem. Educ., 1983, 60, 697
- R. S. Nicholson, Anal. Chem., 1966, 38, 1406
- R. S. Nicholson and I. Shain, Anal. Chem., 1964, 36, 706–723
- R. S. Nicholson, Anal. Chem., 1965, 37, 1351–1355
- J. Heinze, B. A. Frontana-Uribe and S. Ludwigs, Chem. Rev., 2010, 110, 4724–4771
- B. W. D’Andrade, S. Datta, S. R. Forrest, P. Djurovich, E. Polikarpov and M. E. Thompson, Org. Electron., 2005, 6, 11–20.
- P. I. Djurovich, E. I. Mayo, S. R. Forrest and M. E. Thompson, Org. Electron., 2009, 10, 515–520.
- C. M. Cardona, W. Li, A. E. Kaifer, D. Stockdale and G. C. Bazan, Adv. Mater., 2011, 23, 2367–2371.
- E. M. Espinoza, J. A. Clark, J. Soliman, J. B. Derr, M. Morales and V. I. Vullev, J. Electrochem. Soc., 2019, 166, H3175–H3187.
- J. W. Diggle and A. J. Parker, Electrochim. Acta, 1973, 18, 975–979.
- N. G. Tsierkezos, J. Solution Chem., 2007, 36, 289–302.
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