Redox Potentials in Proteins
How ligands and protein environments tune electron transfer
Lesson 3790 of 4,500 · Bioinorganic Chemistry
Learning objectives
- Relate reduction potential to the relative stability of oxidised and reduced metal centres
- Explain how donor atoms, charge, solvent exposure and hydrogen bonding tune protein redox potentials
- Use Marcus ideas of driving force, reorganisation energy and distance to explain electron-transfer rates
Introduction
Many metalloproteins exist to move electrons. Respiration, photosynthesis and many enzymes depend on handing electrons from one metal site to another at the right rate and with the right energy. The key number is the reduction potential, which tells us how strongly a centre wants to gain an electron. A remarkable feature of biology is that the same Fe³⁺/Fe²⁺ or Cu²⁺/Cu⁺ couple can have potentials spread over more than a volt, depending on the protein. This page explains how that tuning works and what controls electron-transfer rates.
Core explanation
Potential and free energy. For a reduction Ox + e⁻ → Red, ΔG°′ = −nFE°′. A more positive E°′ means the reduced form is relatively more stable, so the centre is a better electron acceptor. Biochemists quote E°′ at pH 7 against the standard hydrogen electrode. For comparison, aqueous Fe³⁺/Fe²⁺ has E° of about +0.77 V, while iron in proteins ranges from about −0.4 V in some iron–sulfur proteins to above +0.3 V in some cytochromes.
Ligand effects. Anionic donors such as thiolate or carboxylate stabilise the higher, more positive oxidation state and lower E°′. Neutral donors such as imidazole or thioether favour the lower oxidation state and raise E°′. Methionine sulfur in cytochrome c and in blue copper proteins helps give relatively high potentials. Soft donors favour soft, lower-charge ions: thioether and thiolate donors stabilise Cu(I), raising the Cu²⁺/Cu⁺ potential. Strong π-acceptor ligands also stabilise reduced metals.
Geometry. If the protein enforces a geometry preferred by one oxidation state, that state is favoured. A tetrahedral-like copper site favours Cu(I), increasing E°′. The entatic principle thus affects potential as well as rate.
Electrostatics and solvent. A centre buried in a hydrophobic, low-dielectric pocket disfavours the more highly charged form, because charge is poorly stabilised there. Burying a heme therefore raises E°′ in many cytochromes. Nearby positive charges (lysine, arginine, a helix dipole's N-terminus) raise E°′ by stabilising the extra electron; negative charges lower it. Hydrogen bonds to ligand atoms, especially to cysteine sulfur, withdraw electron density and raise E°′. Changes of a few hydrogen bonds can shift potentials by around 0.1 V.
Proton coupling. If reduction is accompanied by protonation, E°′ depends on pH, falling by about 59 mV per pH unit at 25 °C for one proton per electron. Proton-coupled electron transfer lets proteins link redox chemistry to pumping protons or to substrate chemistry.
Rates: Marcus theory. Electron transfer is fast when the driving force (−ΔG°) is comparable to the reorganisation energy λ. The rate falls off roughly exponentially with distance through protein, by about a factor of ten for every 1.7 Å at long range. Redox chains space centres at less than about 14 Å to keep transfer faster than turnover. Rigid sites with small structural change between oxidation states, such as cytochromes and blue copper proteins, have small λ, typically around 0.7 eV or less, enabling rapid transfer even with modest driving force.
Formulae
ΔG°′ = −nFE°′, with F = 96 485 C mol⁻¹. Nernst equation: E = E°′ − (RT/nF) ln([Red]/[Ox]). Marcus: k ∝ exp[−(ΔG° + λ)² / (4λk BT)].
Step-by-step reasoning
1. Write the redox couple and identify both oxidation states. 2. Consider donor charge: anionic donors lower E°′, neutral soft donors raise it. 3. Consider geometry: which state does the site's enforced shape favour? 4. Consider burial, nearby charges and hydrogen bonds. 5. Check for proton coupling and pH dependence. 6. Combine to predict whether E°′ is high or low compared with the aqueous couple.
Visual explanation
Draw a vertical potential scale from −0.5 V to +0.8 V. Place aqueous Fe³⁺/Fe²⁺ near +0.77 V, then mark a range of iron–sulfur proteins near the bottom and cytochromes in the middle. Add arrows labelled "anionic ligands", "exposure to water" pointing down and "buried heme", "positive charge nearby", "extra hydrogen bonds" pointing up.
Real-world analogy
A redox centre is like a ball on a stepped staircase. Each protein is a step at a particular height, and electrons roll downhill from low-potential steps to high-potential ones. The protein builder can raise or lower each step by changing ligands and surroundings. Unlike a ball, however, an electron must tunnel between steps, so the gap between them matters as much as their heights.
Real-world example
Cytochrome c carries electrons between complexes III and IV of the respiratory chain with E°′ of about +0.25 V. Its heme iron has histidine and methionine axial ligands and is largely buried. Replacing the methionine with a histidine by mutagenesis lowers the potential substantially, showing how a single axial donor tunes the centre's role in the chain.
Why?
Why does biology need so many different potentials for the same metal? Electrons must flow from low-potential donors such as NADH (about −0.32 V) to O₂ (about +0.82 V) in small steps so that the released free energy can be captured to pump protons. A ladder of tuned centres converts one large drop into many manageable ones.
Common misconception
"A metal's reduction potential is a fixed property of the element." Potentials in proteins depend strongly on ligands, geometry, charge and solvent exposure. Another misconception is that a large driving force always means a faster rate; Marcus theory predicts an inverted region where rates decrease when −ΔG° greatly exceeds λ.
Worked example
Question: Calculate ΔG°′ for transfer of one electron from cytochrome c (E°′ = +0.25 V) to a copper centre with E°′ = +0.35 V.
Reasoning: ΔE°′ = 0.35 − 0.25 = +0.10 V. ΔG°′ = −nFΔE°′ = −1 × 96 485 × 0.10 = −9650 J mol⁻¹.
Answer: About −9.6 kJ mol⁻¹; the transfer is favourable.
Quick check
1. Would adding a hydrogen bond to a cysteine thiolate ligand raise or lower the reduction potential? Answer: Raise it, because the hydrogen bond withdraws charge and makes the reduced state relatively more stable.
Exam focus
Use ΔG°′ = −nFE°′ correctly with signs. Give at least three factors that tune E°′ and state their direction. Explain why redox centres in chains lie within about 14 Å of one another and why small reorganisation energy speeds electron transfer.
Advanced insight
Theoretical models estimate potentials by calculating the electrostatic energy of adding charge to a site within a protein of low dielectric. In practice, protein reorganisation, protonation changes and water penetration all contribute, and accurate prediction remains challenging. Engineered proteins have used these principles to design sites with potentials spread over several hundred millivolts using the same metal.
Summary
Protein redox potentials are set by donor charge and softness, enforced geometry, burial, local electrostatics, hydrogen bonding and proton coupling. ΔG°′ = −nFE°′ links potential to driving force. Electron-transfer rates depend on driving force, reorganisation energy and distance, and biological chains arrange tuned centres at short separations for rapid, controlled flow.
Practice questions
1. State whether a thiolate ligand or a thioether ligand gives a higher reduction potential for a copper site, and explain. Answer: A thioether, because a neutral soft donor stabilises the lower oxidation state, while an anionic thiolate stabilises the higher one. 2. How does burying a heme in a hydrophobic pocket usually change its reduction potential? Answer: It raises E°′, because the low-dielectric environment disfavours the more highly charged oxidised form. 3. Calculate ΔG°′ for a one-electron transfer with ΔE°′ = +0.30 V. Answer: ΔG°′ = −1 × 96 485 × 0.30 ≈ −29 kJ mol⁻¹. 4. Why are redox centres in electron-transfer chains usually placed within about 14 Å of each other? Answer: Tunnelling rates fall roughly exponentially with distance, so closer spacing keeps transfer fast enough for biological turnover.