Pourbaix (E-pH) Diagrams

Drop an iron nail into four beakers. One is strongly acidic, one neutral, one alkaline, one bleach-spiked. Four different things happen: vigorous dissolution, slow rusting, passivation, or rapid oxidative attack. A single map predicts all four outcomes before you ever open a beaker: the Pourbaix diagram. It is a plot of electrode potential EE against pH. It partitions the plane into domains where one chemical species is thermodynamically dominant. It is the periodic table of aqueous redox chemistry — compact, quantitative, and drawn directly from the Nernst equation and solubility equilibria. Pourbaix diagrams matter because almost every practical question in aqueous inorganic chemistry is really the same question in disguise. Will this metal corrode? Will this ore leach? Will this pollutant precipitate? Will this battery electrode survive water contact? Each of these asks: at this pH, at this potential, what is the stable form of the element? Marcel Pourbaix built these diagrams in the 1930s–40s. He designed them to give corrosion engineers a tool as indispensable as the phase diagram is to a metallurgist. Today they underpin corrosion protection design and hydrometallurgical extraction. They also guide environmental remediation of heavy metals. And they inform the choice of buffer and potential window in electrochemical synthesis. The big picture is that a Pourbaix diagram is nothing more than a graphical solution to a family of coupled equilibria. There are purely electrochemical reactions, involving electron transfer only. These appear as vertical or sloped lines, depending on whether protons participate. There are purely acid–base reactions, involving proton transfer only. These appear as vertical lines independent of EE. There are also mixed proton–electron transfers. These give sloped lines whose slope is fixed by the stoichiometric ratio of electrons to protons. Every boundary line is a Nernst equation in disguise. Each is evaluated at the condition where two species have equal activity. This turns a stack of KspK_{sp}, pKapK_a, and E∘E^\circ values into a single navigable picture. This article builds the diagram from first principles. It writes every half-reaction and derives every line's slope and intercept. It reads real diagrams for iron and copper. It then applies the machinery to corrosion, and to immunity/passivation/corrosion zones, and to hydrometallurgy. It finishes with the scope limits that every practicing chemist must respect. Pourbaix diagrams are purely thermodynamic. They say nothing about rate.

Key takeaways
  • A Pourbaix diagram plots EE (vertical) vs. pH (horizontal); each region is the predominance domain of one species at a chosen total metal activity.
  • Three line types: horizontal (electron transfer only, pH-independent), vertical (proton transfer only, potential-independent), sloped (coupled electron + proton transfer, slope =−0.0592 (m/n)= -0.0592\,(m/n) V/pH unit at 25 °C).
  • Boundaries are Nernst-equation equalities: set Eox=EredE_{ox} = E_{red} (or [A]=[B][A]=[B] for acid–base lines) and solve for the locus in (E,pH)(E,\text{pH}) space.
  • The two dashed lines for water's own oxidation (O2/H2OO_2/H_2O) and reduction (H2O/H2H_2O/H_2) bound the region where water itself is thermodynamically stable against electrolysis.
  • Diagrams identify corrosion (soluble ion stable), immunity (metal itself stable), and passivation (insoluble oxide/hydroxide stable) zones — the basis of cathodic protection and stainless-steel design.
  • Key idea: every line on a Pourbaix diagram is a Nernst/equilibrium condition set equal at the phase boundary; the whole diagram is a coordinate transform of thermodynamic data into (pH,E)(pH, E) space.

Where this lives today

Corrosion engineering remains the diagrams' home turf: choosing a cathodic-protection potential for a buried steel pipeline, or predicting whether a stainless-steel implant will passivate in physiological fluid (pH ≈ 7.4, mildly oxidizing), starts with locating the operating point on the relevant Pourbaix diagram before any kinetic (Tafel, EIS) data are collected. Nuclear-plant primary-circuit chemistry uses temperature-corrected Pourbaix diagrams (rescaling the 0.05920.0592 V factor for T≈300 ∘T\approx300\,^\circC) to keep zirconium alloy cladding and steel piping inside immunity or tightly protective-oxide domains, since even brief excursions into corrosion domains can seed stress-corrosion cracking. Hydrometallurgy leans on the same tool from the opposite direction: extracting copper, uranium, or gold from ore relies on deliberately pushing pH and potential (via oxidants like O₂, Fe³⁺, or Mn⁴⁺, and acids/bases) into the region where the metal ion is soluble, then later precipitating it by shifting the same coordinates back into a solid-phase domain — leach-then-precipitate flowsheets are literally paths traced across a Pourbaix diagram. Environmental geochemistry uses element-specific diagrams (arsenic, chromium, uranium, selenium) to predict the mobile versus immobile speciation of contaminants in groundwater as a function of redox condition and pH, directly informing remediation strategy (e.g., whether reducing conditions will immobilize chromium as insoluble Cr(OH)₃ rather than mobile, carcinogenic CrO₄²⁻). Battery and electrolyzer chemistry uses the water-stability lines specifically: any aqueous battery or electrolyzer operating outside the narrow ~1.23 V window between the O₂/H₂O and H₂O/H₂ lines risks parasitic water electrolysis, which is why aqueous zinc, lead-acid, and nickel-metal-hydride chemistries are engineered to keep working potentials inside (or only briefly, kinetically, outside) that window — the same water lines that bound every metal's own Pourbaix diagram.

Ask the tutor: How would the iron Pourbaix diagram change qualitatively if chloride ions were present at high concentration, and why does this explain pitting corrosion of stainless steel?

The physical picture

Start from what you already know: the pH Dependence of Redox Potentials tells you that when a half-reaction consumes or produces H⁺, its potential shifts linearly with pH via the Nernst equation. A Pourbaix diagram simply performs this calculation for every relevant couple of an element simultaneously, then finds where each pair of species has equal free energy — i.e., equal activity under the Nernst equation — and plots that condition as a line in the (pH,E)(pH, E) plane. The regions between lines are named for whichever species is thermodynamically dominant there, exactly as in a phase diagram, where a species is "stable" in the coexistence sense used throughout Redox Stability in Water. Three families of reactions generate three families of lines. A pure electron-transfer reaction, such as

Fe3++e−⇌Fe2+\text{Fe}^{3+} + e^- \rightleftharpoons \text{Fe}^{2+}

involves no protons, so its Nernst potential does not depend on pH: it is drawn as a horizontal line at E=E∘E = E^\circ (for unit activities). A pure acid–base reaction, such as

Fe(OH)2+2H+⇌Fe2++2H2O\text{Fe(OH)}_2 + 2\text{H}^+ \rightleftharpoons \text{Fe}^{2+} + 2\text{H}_2\text{O}

involves no electron transfer, so the equilibrium is fixed by pH alone (via KspK_{sp} and the proton stoichiometry) and independent of EE: a vertical line. A mixed reaction, such as

Fe(OH)3+3H++e−⇌Fe2++3H2O\text{Fe(OH)}_3 + 3\text{H}^+ + e^- \rightleftharpoons \text{Fe}^{2+} + 3\text{H}_2\text{O}

couples electron and proton transfer, so the Nernst potential depends on both; the line has a nonzero slope in EE–pH space, fixed by the ratio of protons to electrons in the balanced equation. Layered underneath every metal diagram are two universal dashed reference lines for water itself, because water can act as both oxidant and reductant:

O2+4H++4e−⇌2H2OE=1.229−0.0592 pH\text{O}_2 + 4\text{H}^+ + 4e^- \rightleftharpoons 2\text{H}_2\text{O} \qquad E = 1.229 - 0.0592\,\text{pH}
2H++2e−⇌H2E=0−0.0592 pH2\text{H}^+ + 2e^- \rightleftharpoons \text{H}_2 \qquad E = 0 - 0.0592\,\text{pH}

Both have slope −0.0592-0.0592 V/pH (four electrons/four protons and two electrons/two protons respectively, giving the same m/n=1m/n=1 ratio). Above the upper line, water oxidizes to O₂; below the lower line, water reduces to H₂; between them, water is thermodynamically stable — the "water stability window" that frames every aqueous Pourbaix diagram.

Figure
Anatomy of a Pourbaix diagram: line types and the water-stability window
E (V) pH 0 14 O₂ / H₂O (slope −0.0592) H₂O / H₂ (slope −0.0592) M³⁺ / M²⁺ (horizontal — e⁻ only) M(OH)₂ / M²⁺ (vertical — H⁺ only) M(OH)₃ / M²⁺ (sloped — e⁻ + H⁺) M³⁺ M²⁺ M(OH)₃

Reading such a diagram is an exercise in localization: pick a point (pH,E)(pH, E) representing your solution and applied potential (or open-circuit corrosion potential), and whichever region contains that point names the thermodynamically stable species. Everything else — corrosion rate, kinetics of passivation, whether a film is protective — lies outside the diagram's remit and must come from kinetic data, exactly as Predicting Redox Behavior from Diagrams cautions when interpreting any predominance map.

Figure
Simplified iron Pourbaix diagram: immunity, corrosion, and passivation zones
E (V vs SHE) pH 0 7 14 Fe²⁺ / Fe Fe³⁺ Fe²⁺ (CORROSION) Fe₂O₃ (PASSIVATION) Fe (IMMUNITY) Fe(OH)₂

The core ideas

The entire construction rests on the Nernst equation, applied systematically and combined with mass-balance (solubility) equilibria. For a general half-reaction written as the reduction

a Ox+m H++n e−⇌b Red+m2H2Oa\,\text{Ox} + m\,\text{H}^+ + n\,e^- \rightleftharpoons b\,\text{Red} + \tfrac{m}{2}\text{H}_2\text{O}

the potential is

E=E∘−0.0592nlog⁡[Red]b[Ox]a−0.0592 mn pHE = E^\circ - \frac{0.0592}{n}\log\frac{[\text{Red}]^b}{[\text{Ox}]^a} - \frac{0.0592\,m}{n}\,\text{pH}

where:

  • E∘E^\circ is the standard potential (all activities unity, pH 0),
  • nn is the number of electrons transferred,
  • mm is the number of protons transferred,
  • [Ox],[Red][\text{Ox}], [\text{Red}] are activities (approximated by concentrations) of the oxidized/reduced species,
  • the factor 0.05920.0592 V is RTln⁡10/FRT\ln10/F at T=298.15T = 298.15 K.

Reading it: the coefficient of pH, −0.0592 m/n-0.0592\,m/n, is the slope of the boundary line in EE–pH space. When m=0m=0 (no protons), the slope is zero — a horizontal line. When n=0n=0 is not possible for an electron-transfer reaction but is the case for a pure acid–base equilibrium, the reaction has no EE-dependence at all and the line is vertical, governed instead by

pH=1m(log⁡Ksp−(activity terms))\text{pH} = \frac{1}{m}\Big(\log K_{sp} - \text{(activity terms)}\Big)

which is just the mass-action law for the solubility/hydrolysis equilibrium, entirely independent of potential. For mixed lines, the slope in mV per pH unit follows directly:

slope=−0.0592 mn V per pH unit at 298 K\text{slope} = -0.0592\,\frac{m}{n} \ \text{V per pH unit at 298 K}

where: m/nm/n is the proton-to-electron ratio fixed by how you balance the half-reaction. A 1e⁻/1H⁺ process (like Fe(OH)₃/Fe²⁺ shown above, once fully balanced) gives slope −0.0592×3=−0.1776-0.0592\times3 = -0.1776 V/pH for that particular 1-electron/3-proton case; a 2e⁻/2H⁺ process gives the same slope as water's lines, −0.0592-0.0592 V/pH; a 1e⁻/2H⁺ process gives −0.1184-0.1184 V/pH. The slope is a direct fingerprint of stoichiometry — a chemist can read the electron:proton ratio of a reaction straight off the graph. Finally, every diagram is drawn for a chosen total dissolved-metal activity, conventionally 10−610^{-6} M for corrosion diagrams (the operational definition of "negligible corrosion"). Changing this reference concentration slides the vertical/sloped solid-line boundaries between soluble ion and solid phases, because

E (mixed line)=E∘−0.0592nlog⁡[ion]−0.0592 mnpHE \text{ (mixed line)} = E^\circ - \frac{0.0592}{n}\log[\text{ion}] - \frac{0.0592\,m}{n}\text{pH}

where: lowering [ion][\text{ion}] (a more demanding corrosion criterion) shifts the intercept and hence the whole boundary, enlarging the "immunity"/passivation domains at the expense of the "corrosion" domain — this activity-dependence is itself diagnostic and is exploited deliberately in corrosion engineering.

Derivation AThe Nernst-slope rule for a mixed proton–electron line

Goal: show that any half-reaction transferring nn electrons and mm protons produces a Pourbaix line with slope exactly −0.0592 (m/n)-0.0592\,(m/n) V per pH unit at 298 K, and locate its intercept.

Step 1 — Write the general half-reaction and its Gibbs energy. Take the reduction

a Ox+m H++n e−⇌b Red+m2H2O(l)a\,\text{Ox} + m\,\text{H}^+ + n\,e^- \rightleftharpoons b\,\text{Red} + \tfrac{m}{2}\text{H}_2\text{O}(l)

The reaction quotient is

Q=[Red]b[Ox]a [H+]mQ = \frac{[\text{Red}]^b}{[\text{Ox}]^a\,[\text{H}^+]^m}

(water activity is unity in dilute aqueous solution, so it drops out). The Gibbs energy of reaction is ΔG=ΔG∘+RTln⁡Q\Delta G = \Delta G^\circ + RT\ln Q.

Step 2 — Convert to potential via ΔG=−nFE\Delta G = -nFE. Dividing through by −nF-nF:

E=E∘−RTnFln⁡Q=E∘−RTnFln⁡[Red]b[Ox]a [H+]mE = E^\circ - \frac{RT}{nF}\ln Q = E^\circ - \frac{RT}{nF}\ln\frac{[\text{Red}]^b}{[\text{Ox}]^a\,[\text{H}^+]^m}

Expand the logarithm of the product/quotient:

E=E∘−RTnFln⁡[Red]b[Ox]a−RTnFln⁡1[H+]mE = E^\circ - \frac{RT}{nF}\ln\frac{[\text{Red}]^b}{[\text{Ox}]^a} - \frac{RT}{nF}\ln\frac{1}{[\text{H}^+]^m}

The second term simplifies because ln⁡(1/[H+]m)=−mln⁡[H+]\ln(1/[\text{H}^+]^m) = -m\ln[\text{H}^+]:

E=E∘−RTnFln⁡[Red]b[Ox]a+mRTnFln⁡[H+]E = E^\circ - \frac{RT}{nF}\ln\frac{[\text{Red}]^b}{[\text{Ox}]^a} + \frac{mRT}{nF}\ln[\text{H}^+]

Step 3 — Convert natural log to base-10 pH and insert constants. Using ln⁡x=2.303log⁡x\ln x = 2.303\log x and log⁡[H+]=−pH\log[\text{H}^+] = -\text{pH}, and evaluating 2.303 RT/F=0.05922.303\,RT/F = 0.0592 V at 298.15 K:

E=E∘−0.0592nlog⁡[Red]b[Ox]a−0.0592 mn pHE = E^\circ - \frac{0.0592}{n}\log\frac{[\text{Red}]^b}{[\text{Ox}]^a} - \frac{0.0592\,m}{n}\,\text{pH}

The coefficient multiplying pH is exactly −0.0592 (m/n)-0.0592\,(m/n), independent of the activities chosen — this term alone fixes the slope; the log-activity term only shifts the intercept (vertically, at fixed pH) and does not affect the slope.

Step 4 — Identify the two degenerate cases. If m=0m = 0 (no protons transferred, e.g. Fe³⁺/Fe²⁺), the pH term vanishes identically and E=E∘−(0.0592/n)log⁡([Red]/[Ox])E = E^\circ - (0.0592/n)\log([\text{Red}]/[\text{Ox}]): a horizontal line, confirming the claim for pure electron-transfer reactions. If instead the process transfers protons but no electrons (an acid–base/solubility equilibrium, formally n→n\to "not applicable" because there is no redox step), the entire derivation above does not apply; instead one uses KspK_{sp} or KaK_a directly, and the resulting relation involves pH but no EE — a vertical line, as asserted. Both limits are consistent with the general slope formula only in the sense that m/n→0m/n\to 0 recovers "horizontal," while the vertical case is a genuinely different (non-Nernstian) equilibrium type. This single algebraic manipulation — Nernst equation, log⁡\log split into an activity part and a proton part — generates every solid line, sloped or horizontal, in every Pourbaix diagram that exists.

Go deeper · Derivation B · 1 minLocating a phase boundary: the Fe(OH)₃/Fe²⁺ line worked symbolically
Derivation BLocating a phase boundary: the Fe(OH)₃/Fe²⁺ line worked symbolically

Goal: derive the explicit line equation for the boundary between soluble Fe²⁺ and solid Fe(OH)₃, given the half-reaction

Fe(OH)3(s)+3H++e−⇌Fe2++3H2O(l),E∘=1.057 V (formal value used in Pourbaix’s tables)\text{Fe(OH)}_3(s) + 3\text{H}^+ + e^- \rightleftharpoons \text{Fe}^{2+} + 3\text{H}_2\text{O}(l), \quad E^\circ = 1.057\ \text{V (formal value used in Pourbaix's tables)}

Step 1 — Apply the Nernst equation with solids at unit activity. Since Fe(OH)₃ is a pure solid, its activity is 1 and drops from the reaction quotient. With n=1n=1, m=3m=3:

E=E∘−0.0592log⁡[Fe2+][H+]3⋅1=E∘−0.0592log⁡[Fe2+]−0.0592×3 pHE = E^\circ - 0.0592\log\frac{[\text{Fe}^{2+}]}{[\text{H}^+]^{3}\cdot 1}= E^\circ - 0.0592\log[\text{Fe}^{2+}] - 0.0592\times3\,\text{pH}

because log⁡(1/[H+]3)=3log⁡(1/[H+])=3 pH\log(1/[\text{H}^+]^3) = 3\log(1/[\text{H}^+]) = 3\,\text{pH}, carried with the correct sign as in the general derivation.

Step 2 — Fix the reference activity for the boundary. By the corrosion-engineering convention, the boundary is drawn at [Fe2+]=10−6[\text{Fe}^{2+}] = 10^{-6} M (the traditional "corrosion negligible" cutoff). Then log⁡[Fe2+]=−6\log[\text{Fe}^{2+}] = -6, so:

E=1.057−0.0592×(−6)−0.1776 pH=1.057+0.355−0.1776 pHE = 1.057 - 0.0592\times(-6) - 0.1776\,\text{pH} = 1.057 + 0.355 - 0.1776\,\text{pH}
E=1.412−0.1776 pH  VE = 1.412 - 0.1776\,\text{pH}\ \text{ V}

Step 3 — Sanity-check the slope against the general rule. The general rule predicts slope −0.0592 (m/n)=−0.0592×(3/1)=−0.1776-0.0592\,(m/n) = -0.0592\times(3/1) = -0.1776 V/pH, matching exactly. This is the diagnostic signature of a 1-electron, 3-proton process.

Step 4 — Check a numeric point. At pH 4.00 (asymmetric, non-round test value): E=1.412−0.1776×4.00=1.412−0.7104=0.7016E = 1.412 - 0.1776\times4.00 = 1.412 - 0.7104 = 0.7016 V. So at pH 4 and a potential above about +0.70 V vs. SHE, solid Fe(OH)₃ is the stable phase (rather than dissolved Fe²⁺) even though the metal ion concentration is vanishingly small — this is precisely how passivating oxide films form on iron in mildly acidic, oxidizing conditions, and it is the thermodynamic seed of stainless-steel passivation logic extended to Cr and Ni alloys.

Limiting-case check: as pH → 0 (strongly acidic, the historical reference state), E→1.412E \to 1.412 V, close to the tabulated standard potential region for this couple once activity corrections are included — consistent with the boundary collapsing toward the standard-state value at the acidic extreme, as it must.

Worked examples

Example 1 — Foundational: classify three lines by inspection. Consider three half-reactions relevant to a hypothetical metal M: (a) M3++e−⇌M2+\text{M}^{3+} + e^- \rightleftharpoons \text{M}^{2+} (b) M(OH)2+2H+⇌M2++2H2O\text{M(OH)}_2 + 2\text{H}^+ \rightleftharpoons \text{M}^{2+} + 2\text{H}_2\text{O} (c) MO2+4H++2e−⇌M2++2H2O\text{MO}_2 + 4\text{H}^+ + 2e^- \rightleftharpoons \text{M}^{2+} + 2\text{H}_2\text{O} For (a): no H⁺ appears, so m=0m=0 — a horizontal line at E=Ea∘−0.0592log⁡([M2+]/[M3+])E = E^\circ_{a} - 0.0592\log([\text{M}^{2+}]/[\text{M}^{3+}]). For (b): no electrons appear — this is a pure solubility/acid–base equilibrium, so it is a vertical line located at the pH fixed by KspK_{sp}: from Ksp=[M2+]/[H+]2K_{sp} = [\text{M}^{2+}]/[\text{H}^+]^2 (schematically), pH=12(log⁡Ksp−log⁡[M2+])\text{pH} = \tfrac12(\log K_{sp}-\log[\text{M}^{2+}]), independent of EE. For (c): m=4m=4, n=2n=2, so slope =−0.0592×(4/2)=−0.1184= -0.0592\times(4/2) = -0.1184 V/pH — a sloped line with half the slope of a 4e−/4H+4e^-/4H^+ process (like O₂/H₂O) at the same mm, because here nn is twice as large per proton transferred. This triage — horizontal/vertical/sloped by simply counting H⁺ and e−e^- in the balanced equation — is the first and most important reading skill for any Pourbaix diagram, and it requires no numerical data at all.

Example 2 — Applied: does iron corrode or passivate at pH 3, E=+0.40E = +0.40 V? Using the boundary derived above, EFe(OH)3/Fe2+=1.412−0.1776 pHE_{\text{Fe(OH)}_3/\text{Fe}^{2+}} = 1.412 - 0.1776\,\text{pH}, evaluate at pH = 3.00:

Eboundary=1.412−0.1776×3.00=1.412−0.5328=0.8792 VE_{\text{boundary}} = 1.412 - 0.1776\times3.00 = 1.412 - 0.5328 = 0.8792\ \text{V}

The operating point E=0.40E=0.40 V lies below 0.879 V, so at pH 3 the system sits in the Fe²⁺ (soluble) region relative to this boundary — active corrosion is thermodynamically favored, not passivation, at this potential and pH. Cross-checking against the Fe²⁺/Fe (immunity) boundary (roughly E≈−0.44−0.0592log⁡[Fe2+]E \approx -0.44 - 0.0592\log[\text{Fe}^{2+}], pH-independent for this couple since no protons participate) confirms E=0.40E=0.40 V is well above that immunity line too, so Fe²⁺ — not metallic Fe — is the stable species: the point (pH 3, +0.40 V) lands squarely in the corrosion domain, consistent with the known aggressive dissolution of iron in dilute, mildly oxidizing acid.

Example 3 — Exam/competition level: constructing a two-line intersection (triple point) and predicting a buffer's fate. A student is given two boundary lines for element M (all at the standard 10−610^{-6} M convention): Line 1 (M²⁺/M, pure electron transfer, m=0,n=2m=0,n=2): E1=−0.250E_1 = -0.250 V (horizontal, no pH dependence). Line 2 (M(OH)₂/M²⁺, pure acid–base): vertical at pH =8.50= 8.50. Line 3 (MO₂·H₂O/M²⁺, mixed, m=2,n=2m=2,n=2, from MO2⋅H2O+2H++2e−⇌M2++2H2O\text{MO}_2\cdot\text{H}_2\text{O} + 2\text{H}^+ + 2e^- \rightleftharpoons \text{M}^{2+}+2\text{H}_2\text{O}, with intercept E∘=0.700E^\circ=0.700 V and reference [M2+]=10−6[\text{M}^{2+}]=10^{-6} M): using the general formula,

E3=0.700−0.05922×(−6)−0.0592×22pH=0.700+0.1776−0.0592 pH=0.8776−0.0592 pHE_3 = 0.700 - \frac{0.0592}{2}\times(-6) - \frac{0.0592\times2}{2}\text{pH} = 0.700+0.1776-0.0592\,\text{pH}=0.8776-0.0592\,\text{pH}

Task: find the triple point where all three phases (M, M²⁺, and either M(OH)₂ or MO₂·H₂O) could in principle meet, and determine which solid phase is actually stable at pH 8.50, E=−0.10E = -0.10 V. Step 1. At pH = 8.50 (the vertical line's location), evaluate Line 3:

E3(8.50)=0.8776−0.0592×8.50=0.8776−0.5032=0.3744 VE_3(8.50) = 0.8776 - 0.0592\times8.50 = 0.8776 - 0.5032 = 0.3744\ \text{V}

This is well above Line 1's value of −0.250-0.250 V, so at pH 8.50 the ordering from low to high EE is: M (below −0.250-0.250 V) → M²⁺ (−0.250-0.250 to +0.374+0.374 V) → MO₂·H₂O (above +0.374+0.374 V). The vertical line (M(OH)₂/M²⁺) only matters below the potential where MO₂·H�2O is stable, i.e., it competes with M²⁺ in the same window; since M(OH)₂ is the lower oxidation-state solid, its true domain lies between Line 1 and Line 3, replacing part of the naive M²⁺ region wherever it is thermodynamically favored — determining this requires comparing ΔGf\Delta G_f of M(OH)₂ against dissolved M²⁺ directly, which is exactly the vertical-line construction. Step 2. At the test point (pH,E)=(8.50,−0.10 V)(pH, E) = (8.50, -0.10\ \text{V}): compare −0.10-0.10 V against Line 1 (−0.250-0.250 V) and Line 3 (+0.3744+0.3744 V). Since −0.250<−0.10<0.3744-0.250 < -0.10 < 0.3744, the point lies in the intermediate band — the M²⁺/M(OH)₂ competition zone. Because we are exactly at the vertical line's pH (8.50), this point sits precisely on the boundary between soluble M²⁺ and solid M(OH)₂: an infinitesimal decrease in pH would place the point in the "M²⁺ stable" (corroding) region, while an infinitesimal increase in pH would place it in the "M(OH)₂ stable" (passivating) region. This razor's-edge sensitivity is a completely general and practically important feature of Pourbaix diagrams: near a nearly-vertical boundary, small pH shifts (a local acidification in a crevice, for instance) can flip a system from passivation to active corrosion, which is precisely the mechanism behind crevice corrosion and pitting in engineering alloys.

Limiting cases, scope & common traps

SituationWhat the diagram tells youWhat it does NOT tell you
Point deep inside a solid-oxide regionThat oxide is thermodynamically the most stable phaseWhether the oxide film is coherent/adherent enough to block further reaction (passivation is a kinetic fact superimposed on a thermodynamic map)
Point in the "immunity" (metal) regionThe bare metal itself is thermodynamically stable — no driving force for oxidationNothing about mixed-metal alloys, whose diagrams differ from pure-element ones
Point between the two water linesWater is thermodynamically stable there; no net electrolysis driving forceNothing about overpotential-driven side reactions (e.g., O₂ evolution kinetics on some electrodes is slow enough that other reactions dominate in practice)
Changing the reference metal-ion activity (e.g., 10−6→10−410^{-6}\to10^{-4} M)Shifts sloped/vertical boundaries; a stricter (lower) activity criterion enlarges "safe" domainsThe horizontal pure-electron-transfer lines involving only the redox couple activities shift too, if those activities are not held fixed
As T→T\to higher temperatureThe 0.05920.0592 V factor scales as RTln⁡10/FRT\ln10/F, so slopes and spacings between lines change (larger at higher TT)Standard diagrams tabulated at 298 K do not directly apply to high-temperature aqueous corrosion (e.g., PWR conditions) without re-derivation
Non-aqueous or mixed solventsThe whole water-line scaffold (and often the E∘E^\circ values) must be re-derived; the diagram concept still appliesA diagram drawn for water cannot simply be relabeled for another solvent

The chemist behind it

Origins · 1 minMarcel Pourbaix and how this was discovered
MP
Marcel Pourbaix
1904–1998 · Belgian electrochemist, ULB and CEBELCOR

Pourbaix trained as a chemical engineer in Brussels and spent his career fusing rigorous thermodynamics with the very practical problem of why metals rust and how to stop them. Working through the 1930s and publishing his systematic Atlas d'équilibres électrochimiques in 1963 (with English translation following soon after), he assembled standard potentials, solubility products, and hydrolysis constants for essentially every metallic element into a unified graphical language — the EE–pH diagram that now bears his name. He founded CEBELCOR (the Belgian Centre for Corrosion Study) to bridge this thermodynamic mapping with industrial corrosion control, insisting that the diagrams be usable by working engineers, not just theoreticians. His approach deliberately mirrored the phase-rule diagrams of physical metallurgy, explicitly borrowing the vocabulary of "predominance domains" so that corrosion scientists could reason about aqueous stability with the same visual fluency metallurgists brought to phase diagrams.

History
- 1904 — Marcel Pourbaix born in Myshega, Russia, to a Belgian engineer family.
- 1930s — Doctoral and early research work at the Université Libre de Bruxelles develops systematic thermodynamic treatment of aqueous metal equilibria.
- 1938 — First formal presentations of combined potential–pH equilibrium diagrams for iron and related systems.
- 1963 — Publication of the Atlas d'équilibres électrochimiques, compiling diagrams for nearly all metallic elements against water.
- 1974 — English-language Atlas of Electrochemical Equilibria in Aqueous Solutions published (NACE/Pergamon), cementing international adoption in corrosion engineering.
Why is the Pourbaix diagram drawn for a specific metal-ion activity, usually 10⁻⁶ M?

Because several boundaries (any line separating a dissolved ion from a solid phase) depend explicitly on the ion's activity through the Nernst/solubility relation, the diagram is not unique — it is a family of diagrams parameterized by that chosen activity. The value 10⁻⁶ M is a corrosion-engineering convention representing an operationally negligible dissolution rate; choosing a stricter (lower) value enlarges the "safe" immunity and passivation domains, while a looser value shrinks them. Whenever you read a published diagram, check the stated reference activity before drawing conclusions, since two diagrams for the same element at different activities can look meaningfully different near sloped or vertical boundaries.

Do Pourbaix diagrams say anything about reaction rate or corrosion speed?

No — they are strictly thermodynamic maps built from standard potentials and equilibrium constants, exactly like a phase diagram. A point in the "corrosion" domain only guarantees that dissolution is thermodynamically favorable, not that it happens quickly; a point in the "passivation" domain only guarantees the oxide is more stable than the alternatives, not that the film is continuous, adherent, or defect-free. Real corrosion rates require kinetic data — Tafel slopes, exchange current densities, film growth and breakdown kinetics — layered on top of the Pourbaix picture. Engineers use the diagram to identify where to look, then bring in electrochemical kinetics to determine how fast.

How do you decide whether a boundary line is horizontal, vertical, or sloped without doing any calculation?

Count protons and electrons in the balanced half-reaction. If protons (H⁺) appear but electrons do not (it's a solubility or acid–base equilibrium, not redox), the line is vertical, fixed only by pH. If electrons appear but protons do not (pure redox couple, like Fe³⁺/Fe²⁺), the line is horizontal, fixed only by E∘E^\circ and activity ratios. If both appear, the line is sloped, with slope −0.0592 (m/n)-0.0592\,(m/n) V per pH unit at 298 K, where mm is protons and nn is electrons. This triage requires nothing beyond correctly balancing the equation.

Why do the two water stability lines bound essentially every aqueous Pourbaix diagram?

Because water itself can be oxidized (to O₂) at sufficiently high potential or reduced (to H₂) at sufficiently low potential, independent of whatever metal or element the main diagram concerns. Any region of (pH,E)(pH, E) space above the O₂/H₂O line or below the H₂O/H₂ line is a region where water is not thermodynamically stable and would itself decompose given a suitable catalyst or long enough time; metal species that appear stable there are only "stable" relative to each other, while water itself is being consumed in the background. Overlaying these two dashed reference lines lets a chemist immediately judge whether a given metal-oxidation or metal-reduction process is thermodynamically compatible with aqueous conditions, or whether it can only proceed via decomposition of the solvent.

Can Pourbaix diagrams be extended to non-standard temperatures or to seawater/mixed electrolytes?

Yes, but not by simply relabeling axes. The 0.05920.0592 V (more precisely RTln⁡10/FRT\ln10/F) factor scales with temperature, so both the water lines and every sloped metal-species line change slope and intercept as TT rises — this matters enormously for nuclear reactor coolant chemistry at ~300 °C. For seawater or other electrolytes, the relevant activity coefficients, competing complexation (e.g., chloride complexes of many metal ions), and possibly new solid phases (chlorides, sulfides) must be incorporated, sometimes producing qualitatively different diagrams from the pure-water case — chloride-containing systems in particular can shrink or eliminate passivation domains, which is the thermodynamic seed of pitting corrosion susceptibility in chloride environments.

What's the difference between the "immunity," "corrosion," and "passivation" zones on a metal's Pourbaix diagram?

Immunity is the region where the bare metal (zero oxidation state, solid) is the thermodynamically stable species — no driving force exists for oxidation at all, and this is the target zone for cathodic protection (imposing a sufficiently negative potential). Corrosion is the region where a soluble ionic species (e.g., Fe²⁺, Fe³⁺) is stable — dissolution is thermodynamically favored, and if this happens continuously the metal is consumed. Passivation is the region where an insoluble solid compound (typically an oxide or hydroxide) is stable — the metal has reacted, but the product coats the surface rather than dissolving away, which can (if the film is coherent) drastically slow further attack. All three names describe a possible consequence of a thermodynamic prediction; only kinetic and microstructural data confirm which one actually governs a real system's behavior.

Does a Pourbaix diagram change if I use a different reference electrode?

The diagram itself, as conventionally tabulated, uses the standard hydrogen electrode (SHE) as the zero of potential, matching the convention used for all E∘E^\circ values throughout aqueous Redox Stability in Water. If you measure potentials against a different reference electrode (saturated calomel, Ag/AgCl), you must convert your measured value to the SHE scale by adding the reference electrode's known potential offset before plotting it on a standard Pourbaix diagram, or equivalently shift the whole diagram's vertical axis by that same offset. Forgetting this conversion is one of the most common practical errors when comparing corrosion-potential measurements to published diagrams.

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