The General Titration Curve
A single S-shaped curve describes almost every titration ever run. It is steep in the middle and flat at the ends. Whether you are neutralizing acetic acid with sodium hydroxide, precipitating chloride with silver nitrate, or oxidizing iron(II) with cerium(IV), the pattern holds. The plot of a monitored signal (pH, electrode potential, pM) against titrant volume has the same qualitative shape. There is a gentle pre-equivalence slope, a sharp central inflection, and a gentle post-equivalence slope. Understanding why this shape is universal matters greatly. So does knowing exactly how steepness, symmetry, and inflection position depend on concentration and equilibrium constants. This is the difference between memorizing individual titration types and predicting the behavior of any new one. This matters because the titration curve is the analytical chemist's diagnostic tool. Its inflection point locates the equivalence point. Its steepness dictates which indicator or instrumental method can detect that point reliably. Its overall shape reveals whether a titration is even feasible before a single drop of titrant is dispensed. A flat, sluggish curve near the equivalence point means no indicator will give a sharp color change. No instrumental method will give a crisp signal jump either. The reaction must then be abandoned or reformulated. A steep curve means centimeter-scale volume errors translate into negligible concentration errors. The big picture is that every titration curve is generated by the same three-region logic. This holds regardless of chemical type. There is an excess-reagent region governed by simple stoichiometric dilution. There is a transition region governed by the reaction's equilibrium constant. And there is a mirror-image excess-titrant region on the other side. The reaction type (acid–base, complexometric, precipitation, redox) only changes which equilibrium expression computes the monitored quantity. The mathematical skeleton is identical. This universality is why one master curve underlies many different systems. Built from mass balances and an equilibrium constant, it describes the strong-acid/strong-base curve, the Fajans precipitation curve, and the potentiometric redox curve alike. This article builds that master curve from first principles. It uses mass and charge balances, an equilibrium expression, and a definition of the fraction titrated. It derives the standard shape parameters: where the curve is flattest, where it is steepest, and how steepness scales with the equilibrium constant and analyte concentration. It shows, with fully worked numerical examples, how these parameters change across acid–base, precipitation, and redox systems. The treatment assumes familiarity with Titer and Titrimetric Calculations and the Theory of Titrimetric Analysis. It sets up the more detailed treatment of the equivalence point and end-point detection that follows elsewhere.
- Every titration curve is sigmoidal: flat pre-equivalence, steep transition, flat post-equivalence, because the monitored quantity depends logarithmically on concentration ratios that swing wildly near stoichiometric balance.
- The fraction titrated, , is the natural universal coordinate; marks the equivalence point regardless of reaction type.
- Curve steepness at the equivalence point scales with for 1:1 reactions of comparable dilution — larger equilibrium constants (more complete reactions) give sharper breaks.
- Dilution during titration (titrant added to a fixed initial volume) systematically damps the curve at high , an effect often neglected in textbook sketches but real and calculable.
- The same mass-balance/charge-balance machinery generates acid–base pH curves, precipitation pM curves, and redox potential curves — only the Nernst or / expression differs.
- Curve symmetry about the equivalence point holds exactly only for 1:1 stoichiometry with negligible dilution asymmetry; unequal analyte/titrant concentrations or n:1 stoichiometry skew the curve.
- Key idea: the sigmoidal shape and its steepness are consequences of a logarithmic response to a concentration ratio that changes by orders of magnitude within a few percent of stoichiometric equivalence.
Where this lives today
Automated potentiometric titrators — instruments standard in pharmaceutical quality control, water-treatment laboratories, and petrochemical assay labs — digitize the entire sigmoidal curve at fine volume increments and locate the equivalence point from the maximum of the first derivative or the zero-crossing of the second derivative, rather than relying on a human eye watching an indicator; the theory in this article is exactly what such firmware implements. Karl Fischer titrators for water content, acid-value and base-value titrators for petroleum products, and chloride titrators for food-salt content all report results derived from fitting or differentiating a curve of precisely this general shape. In pharmaceutical analysis, non-aqueous acid–base titrations of weak organic bases (many active pharmaceutical ingredients are amines) rely on predicting curve steepness from the effective in the non-aqueous solvent to choose a compatible indicator or electrode system, directly applying the steepness scaling derived above. In environmental and geochemical analysis, alkalinity titrations of natural waters (carbonate/bicarbonate systems) produce titration curves with two inflection points, requiring exactly the same mass-balance machinery extended to a diprotic system, where two overlapping sigmoids must be resolved. Complexometric titrations with EDTA — used to determine water hardness (Ca²⁺/Mg²�ic content) and to assay metal ion content in alloys and pharmaceutical excipients — generate pM curves whose sharpness depends on the conditional formation constant (itself a function of pH and competing side reactions), a direct generalization of the -controlled precipitation curve worked out in Example 2. Biosensor and ion-selective electrode (ISE) research groups continue to use the general titration-curve framework to design new potentiometric sensors, predicting from first principles how sharp a response a new ionophore-based membrane will give when challenged with a titration-like concentration ramp, connecting directly to the theory of Theory of Titrimetric Analysis and anticipating the more detailed treatment of The Equivalence Point and the End Point and practical Indicators and End-Point Detection used to read these curves out in real time.
Ask the tutor: How does the shape of this general curve change when the analyte is a weak acid instead of a strong acid, and why does the pre-equivalence region become a buffer region rather than a simple dilution region?
The physical picture
Picture a beaker holding a fixed volume of analyte at concentration , into which titrant of concentration is dispensed from a buret. At every instant the solution contains some leftover, unreacted analyte (before equivalence), or some excess, unconsumed titrant (after equivalence), plus whatever product the reaction has generated. A detector — glass electrode, ion-selective electrode, redox electrode, or the human eye watching an indicator — reports some monotonic function of one of these species' concentrations. That is the entire physical picture: a mass balance tracks how much of each species is present, an equilibrium constant fixes how that species partitions among its possible forms, and the response is typically the logarithm of a concentration (pH, pM, or potential via the Nernst equation). The logarithmic response is the key to the sigmoid. Consider titrating a strong acid with a strong base. Far from equivalence, adding one more milliliter of base neutralizes a tiny fraction of the large excess of acid present, so barely changes and pH creeps upward slowly. But near equivalence, the excess acid has been whittled down to a small residual amount; the same one-drop addition now neutralizes a much larger fraction of what remains, so can fall by two or three orders of magnitude in that single drop. Because pH is , an order-of-magnitude concentration change is a full pH unit — hence the near-vertical jump. Immediately past equivalence, the base itself becomes the "excess reagent" and the same logic runs in reverse: the curve flattens again because now a large excess of titrant dominates and one more drop is a small fractional perturbation. This qualitative story is identical for precipitation titrations (monitoring pAg or pCl via ), for complexometric titrations (monitoring pM via a formation constant), and for redox titrations (monitoring via the Nernst equation and the reaction's combined formal potential). In every case there are three algebraic regimes: (1) pre-equivalence, where leftover analyte, diluted by added titrant volume, controls the response; (2) the equivalence region itself, a narrow window where the mass balance must be solved from the equilibrium constant because neither reactant is in stoichiometric excess; (3) post-equivalence, where excess titrant, diluted by total volume, controls the response. The curve's inflection point, its slope there, and its overall symmetry are all consequences of stitching these three regimes together smoothly.
The core ideas
The universal coordinate for any titration is the fraction titrated,
where: is titrant concentration (mol L⁻¹), is volume of titrant delivered, is initial analyte concentration, is initial analyte volume. Reading: is stoichiometric equivalence for a 1:1 reaction; means analyte is in excess; means titrant is in excess. For an :1 stoichiometry (analyte : titrant), replace with in the denominator, or equivalently define relative to moles of reactive equivalents. In the pre-equivalence region, the concentration of unreacted analyte, diluted into the growing total volume, is
where: the numerator is moles of analyte not yet consumed, the denominator is total solution volume at that point. Reading: this term dominates the monitored response whenever leftover analyte concentration is much larger than what the reaction's equilibrium would otherwise dictate — which is true away from equivalence for any reaction with a reasonably large equilibrium constant. In the post-equivalence region the mirror expression holds for excess titrant,
where: symbols as above. Reading: exactly analogous logic, with titrant now in stoichiometric excess. At neither approximation is valid — trace amounts of both species are present in stoichiometric balance, and the true concentration must be obtained from the reaction's equilibrium constant directly, e.g. , , , or a Nernst-derived equilibrium constant for redox systems. The steepness of the curve at , expressed as , is what a general derivation below makes explicit; it turns out to scale with (or, for redox, with the number of electrons transferred and the difference in formal potentials), which is the master relationship that determines titration feasibility. The relative sharpness of the break can be quantified with the slope at the equivalence point,
where: denotes a -type response (pH, pM, pAg…), is the equilibrium constant governing the reverse of the titration reaction (i.e., how far the "completed" reaction still dissociates back into reactants). Reading: a reaction that goes essentially to completion (tiny , i.e. huge forward ) gives an enormous slope — a razor-sharp break; a reaction that is only weakly favorable gives a gentle, hard-to-detect break.
Goal. Show that for a general 1:1 titration reaction with equilibrium constant , the monitored quantity passes through the point with a slope that scales as , and that the curve is symmetric about in the limit of negligible dilution.
Step 1 — set up the mass and equilibrium balances. Let be the total analytical concentration of species originally present as A (diluted appropriately), and the total titrant added, both referenced to total volume . Define as the free (unreacted) concentration of A at any point. By mass balance, the amount of P formed equals the amount of T consumed, so
assuming stoichiometric 1:1 consumption and that is the free (excess or deficient) titrant concentration. The equilibrium constant is
Step 2 — write the overall balance in terms of f. Using and , the difference is the "signed excess" — positive past equivalence, negative before. Mass balance requires (excess titrant equals free titrant minus free leftover A, since whatever A remains free was never consumed and so did not contribute to titrant consumption beyond stoichiometry). Substituting into the equilibrium expression and eliminating gives a quadratic in :
This quadratic is the exact equation of the titration curve; it applies for all , not just near equivalence.
Step 3 — evaluate exactly at f = 1. At the linear coefficient collapses to alone (the term vanishes), leaving
For a reaction with large (favorable, as almost all titrations require), the product dominates over the linear term except when is very small, and to leading order
This is the free-analyte concentration exactly at equivalence — small when is large, as expected physically (the reaction has gone essentially to completion, leaving only a trace of unreacted A governed by the reverse equilibrium).
Step 4 — differentiate to get the slope at equivalence. Differentiating the exact quadratic implicitly with respect to , holding approximately constant over the narrow region near (dilution effects are treated separately), gives
At this simplifies, using , to
for large . Converting to the scale via ,
which is a striking result: to leading order in large , the slope of versus at equivalence is nearly independent of for the -scale itself, but the width of the region over which the curve stays "sharp" (in terms of raw concentration , not ) shrinks as — meaning a small volume error near a large- equivalence point produces a much larger swing in than the same volume error would for small , because the curve's curvature (not just its instantaneous slope) tightens around . The practically useful measure is the total across a fixed small window (e.g. ±0.1%), which does scale with ; this is developed quantitatively in the worked examples.
Step 5 — symmetry. Because the quadratic in Step 2 is, apart from the sign of , unchanged under simultaneous exchange and appropriate relabeling of "excess A" and "excess T" concentrations (valid when for the forward and notional reverse-excess equilibria are reciprocal, and dilution is symmetric), the curve is antisymmetric about in this idealized limit: for small . Real curves break this symmetry whenever changes non-negligibly between and (dilution asymmetry) or when the reaction is not exactly 1:1.
Go deeper · Derivation B · 2 minDilution-corrected steepness and the volume at which the curve is steepest
Goal. Derive the general expression for (steepness with respect to volume, the experimentally relevant quantity) including the dilution factor, and show explicitly where it peaks.
Step 1 — write the pre-equivalence response with dilution. For a strong-acid/strong-base type titration (as the simplest concrete case, generalizable to other systems by replacing with the appropriate species), before equivalence
so that
Step 2 — differentiate with respect to titrant volume. Using for , apply the quotient rule inside the logarithm:
Both terms are positive (pH rises as increases, as physically required), and both diverge as — i.e., as the equivalence volume is approached, since the first term's denominator goes to zero. This divergence is the mathematical signature of the sharp break; it is tamed in reality only by the finite equilibrium constant taking over exactly at (Step 3 of the first derivation), which caps the actual maximum slope at a large but finite value.
Step 3 — identify the location of maximum slope for the exact (equilibrium-capped) curve. Because the idealized excess-reagent formula diverges at , the true maximum slope of the full curve — the quadratic solution from the first derivation, valid through the transition — occurs extremely close to, but not always exactly at, . For a symmetric 1:1 reaction with negligible dilution asymmetry (Step 5 above), the inflection point of coincides with to a very good approximation whenever ; the residual shift is of order in -units and is negligible (parts per million of ) for , but becomes appreciable (percent-level shifts) for , which is precisely the regime in which titrations become unreliable.
Step 4 — general n:1 and asymmetric-concentration correction. If titrant and analyte concentrations differ substantially (e.g., titrating a dilute analyte with concentrated titrant to minimize volume), the dilution term in Step 2 no longer varies negligibly across the transition window, and the inflection point shifts slightly toward smaller relative to the naive equivalence volume; the shift is second order in and is calculated case-by-case rather than by a universal formula, which is why real curves are always checked numerically (or graphically) rather than assumed perfectly symmetric when concentrations differ by more than roughly a factor of ten.
Worked examples
Example 1 — foundational: strong acid titrated with strong base, full curve construction. Titrate mL of M HCl with M NaOH. Compute pH at , , , , , , , and mL. Equivalence volume: mL. At mL: M, pH . At mL (pre-equivalence, dilution matters):
pH , report pH . At mL:
At mL:
At mL (exact equivalence): the solution is 0.0500 M NaCl (neutral salt of strong acid/strong base), so M at 25 °C, pH . At mL (post-equivalence, excess OH⁻):
pOH , pH . At mL:
At mL:
Tabulating: pH rises from 1.00 to only 3.00 over the first 49 mL (48 pH-unit-per-49-mL average, essentially flat), then rockets from 3.00 to 11.00 (an 8.00-unit jump) across just 2.10 mL bracketing equivalence (49.00 to 51.10 mL), then flattens again, reaching only 11.96 after ten more milliliters. This is the sigmoid quantitatively: essentially all of the useful signal change is compressed into roughly ±0.2% of the equivalence volume. The maximum slope, from the derivation, indeed sits almost exactly at mL — consistent with for being , an enormous number that pins the inflection essentially exactly at .
Example 2 — applied: precipitation titration of chloride with silver nitrate, and comparison of curve sharpness. Titrate mL of M NaCl with M AgNO₃ (). Find pCl at mL (pre-equivalence), at the equivalence point, and at mL (post-equivalence), and compare the sharpness of the break to a hypothetical titration of iodide (using ) under identical volumes/concentrations. Equivalence volume: mL. At mL (pre-equivalence, excess Cl⁻ dominates over the tiny solubility contribution):
pCl . (Check that this dominates the equilibrium solubility contribution: M, utterly negligible next to M — approximation valid.) At equivalence ( mL): here from the stoichiometric precipitation of AgCl leaving only its own solubility equilibrium, diluted appropriately but with no net excess of either ion, so
At mL (post-equivalence, excess Ag⁺ dominates):
So pCl swings from 2.15 → 4.87 → 7.54 across just 5.00 mL: a total change of 5.39 pCl units. For the hypothetical AgI titration under identical volumes and concentrations, the pre-equivalence value of pI at mL is identical in form (excess-halide-controlled, no solubility correction needed since is even smaller), giving pI as well; but at equivalence,
a jump of 5.89 pI units already just from excess-halide to equivalence (compare 2.72 for chloride over the same span), demonstrating explicitly that the smaller (more favorable) gives the sharper break, exactly as the scaling in the derivation predicts (here plays the role of the "reaction" equilibrium constant, since precipitation is the forward direction being driven to completion).
Example 3 — exam/competition level: redox titration curve and locating the true inflection point for asymmetric electron stoichiometry. A solution containing mL of M Fe²⁺ is titrated with M Ce⁴⁺ ( V, V vs. SHE, both formal potentials in 1 M H₂SO₄, 1-electron transfers each, so the reaction is 1:1 despite both being one-electron couples — a genuinely symmetric case is chosen deliberately here to set up the asymmetric follow-up). Find at mL, at equivalence, and at mL ( mL), and then show how the equivalence potential formula changes if instead a two-electron oxidant such as (n=2) is titrated against the same one-electron Fe²⁺/Fe³⁺ couple, to illustrate the asymmetric-stoichiometry correction to the equivalence potential. Equivalence volume: mL.
Pre-equivalence ( mL), Fe couple controls (excess Fe²⁺/Fe³⁺ present in known ratio): Moles Fe²⁺ initial mol. Moles Ce⁴⁺ added mol, which oxidizes an equal number of moles of Fe²⁺ to Fe³⁺ (1:1 stoichiometry). So:
Using the Nernst equation for the Fe³⁺/Fe²⁺ couple (volume cancels in the ratio since both species are in the same total volume):
At equivalence: for two one-electron couples with equal electron stoichiometry (), the equivalence potential is the simple weighted average
This follows from adding the two Nernst equations (one for each couple, both valid simultaneously at equivalence since both redox pairs share the same solution) and using the stoichiometric fact that at equivalence and (charge/mass balance at exact stoichiometric balance), which lets the log terms cancel upon addition when .
Post-equivalence ( mL — note this is actually pre-equivalence since mL; recomputing for genuinely post-equivalence at mL instead), Ce couple controls: Moles Ce⁴⁺ added at 35.00 mL: mol; moles Fe²⁺ available to reduce it, mol, all consumed, leaving excess Ce⁴⁺ mol and Ce³⁺ formed mol (one Ce³⁺ per Fe²⁺ consumed).
So rises from 0.677 V (well before equivalence) to 1.19 V at equivalence to 1.639 V (just past) — a large, sharp break of order 1 V total, driven by the 1.02 V difference in formal potentials, consistent with redox titrations generally giving very sharp breaks when exceeds roughly 0.2 V.
Asymmetric stoichiometry correction (n₁ ≠ n₂): if instead titrant is (, V) reacting with Fe²⁺ (), the balanced reaction is , and the equivalence-potential formula must weight by electrons transferred, not by a simple average:
Note this is not the simple average of 0.68 and 0.77 (which would be 0.725 V) — the two-electron couple's potential is weighted twice as heavily, since twice as many Fe²⁺ equivalents are consumed per mole of Tl³⁺, shifting closer to . This is the essential correction that a purely "symmetric" mental model of redox titrations misses, and it is a common source of error in equivalence-potential calculations for mixed n-value systems.
Limiting cases, scope & common traps
| Limiting case | What happens to the curve | Why |
|---|---|---|
| (reaction goes to completion) | Break becomes vertical; equivalence point and steepest point coincide exactly | Free reactant concentration at vanishes as (derivation, Step 3) |
| small (weak reaction, e.g. weak acid + weak base) | Break flattens or disappears; may be undetectable by eye or simple electrode | Free reactant at remains large; curve never develops a sharp inflection |
| (very dilute analyte) | Break shrinks in -units even for large ; total across equivalence shrinks | Both pre- and post-equivalence excess terms shrink toward the equilibrium value, narrowing the achievable dynamic range |
| (unequal electron/stoichiometric coefficients, redox) | Equivalence value is an electron-weighted average, not simple average; curve is asymmetric about | Charge/mass balance at equivalence weights each couple by its electron count (Example 3) |
| Large dilution ratio or | Inflection point shifts slightly from nominal ; total volume change across titration is very asymmetric | Dilution term varies non-negligibly across the transition window (second derivation, Step 4) |
| or far from equivalence | Curve response becomes nearly volume-independent (flat) | Fractional change in a large excess concentration from one more drop is negligible |
The chemist behind it
The systematic mathematical treatment of the titration curve — expressing pH, pM, or as continuous functions of titrant volume via mass-balance and equilibrium-constant bookkeeping — crystallized through the twentieth-century development of physical and analytical chemistry, but its deepest roots trace to the study of acid–base equilibria itself.
Origins · 1 minSøren Peter Lauritz Sørensen and how this was discovered
Sørensen, a Danish chemist working at the Carlsberg Laboratory on the physical chemistry of protein and enzyme behavior, introduced the pH scale in 1909 explicitly to make hydrogen-ion concentration measurements tractable across the enormous dynamic range that acid–base systems exhibit — precisely the range that a titration curve traverses. His work on buffer solutions and hydrogen-ion activity measurement supplied the conceptual and notational scaffold (the negative logarithm convention) without which the "sharp break" language used to describe titration curves would not exist in its modern form. Sørensen's meticulous quantitative approach — treating hydrogen-ion concentration as a variable worthy of its own precise scale and measurement technique — exemplifies the same rigor that underlies the mass-balance/equilibrium-constant derivation of the general titration curve: a willingness to track a concentration across many orders of magnitude with equal care at every point, not just where it is convenient.
Why is the titration curve always S-shaped rather than, say, linear or a simple exponential?
The S-shape arises because the monitored variable (pH, pM, or potential) is a logarithm of a concentration, and that concentration itself is a ratio of two quantities — leftover analyte or excess titrant, each divided by total volume — that change from "large" to "near zero" to "large again" as titrant is added. Far from equivalence, one reactant dominates so heavily that adding more titrant changes its concentration by only a small fractional amount, giving a flat log-response. Near equivalence, the dominant reactant has been reduced to a small residual, so the same volume increment represents a huge fractional change, and the logarithm swings sharply. Stitching these two flat regions to a swiftly rising middle region necessarily produces a sigmoid; no other shape is consistent with a logarithmic response to a concentration ratio that spans many orders of magnitude across a narrow volume window.
Does every titration curve pass through its steepest point exactly at the stoichiometric equivalence point?
Only approximately, and only under specific conditions: 1:1 stoichiometry, a sufficiently large equilibrium constant, and comparable analyte/titrant concentrations (so dilution effects are symmetric across the transition). When these hold, the curve is antisymmetric about equivalence and the inflection coincides with to high precision. When stoichiometry is n:1 (unequal electrons or unequal reacting moles), or when titrant concentration differs greatly from analyte concentration, the point of maximum slope can be measurably offset from true equivalence. High-precision titrimetry therefore fits the entire curve to the exact mass-balance equation, or uses linearization techniques like the Gran plot, rather than assuming the visual inflection is exactly correct.
How does the equilibrium constant of the titration reaction determine whether the titration is even feasible?
Feasibility requires a break sharp enough that an indicator color change or instrumental signal change reliably brackets the equivalence point within an acceptable volume tolerance (commonly ±0.1% relative or better). The derivation shows the residual, unreacted-analyte concentration exactly at equivalence scales as : a large (strongly favorable reaction) drives this residual concentration to a very small value, producing a steep, well-resolved break. If is too small — for instance, titrating a very weak acid with a very weak base, or precipitating a salt with a modestly large — the residual concentration at equivalence remains comparable to concentrations elsewhere on the curve, the inflection flattens, and no indicator or simple electrode can locate the equivalence point with useful precision. A common rule of thumb requires the product of concentration and equilibrium constant to exceed roughly – for a clearly usable break.
Why does dilution matter even though the titration reaction's stoichiometry is unaffected by adding solvent?
Dilution changes the total volume over which a fixed number of moles of leftover analyte or excess titrant is distributed, and since the monitored response depends on concentration (moles per volume), not moles alone, this directly changes the measured pH, pM, or potential at every point except exactly at equivalence for perfectly symmetric conditions. The flat tails of the sigmoid are partly a "true" reflection of stoichiometric excess and partly an artifact of the fact that as titrant volume grows, everything gets a little more dilute, further damping the response. In precision work, particularly when titrant concentration is very different from analyte concentration, this dilution correction is not negligible and is built explicitly into the exact mass-balance equations rather than approximated away.
Can the same "general titration curve" framework describe complexometric (EDTA) titrations?
Yes — the framework is identical in structure, with the equilibrium constant replaced by the (conditional) formation constant of the metal–EDTA complex, and the monitored quantity replaced by pM (the negative log of free metal-ion concentration). Pre-equivalence, excess free metal ion, diluted into total volume, controls pM; post-equivalence, excess EDTA (which competes for any trace of free metal ion via the large ) controls it; at equivalence, the residual free-metal concentration is set by the conditional formation constant exactly as sets the residual analyte at equivalence for any 1:1 reaction. The only extra complication is that itself depends on pH (through EDTA protonation) and on competing ligands, so a buffered pH is essential to keep the effective equilibrium constant — and hence the curve's sharpness — as large as possible.
Why do some titration curves show two inflection points instead of one?
Two inflection points occur when the analyte can react with titrant in two (or more) sequential, resolvable steps — for example, titrating a diprotic acid whose two dissociation constants differ by several orders of magnitude, or titrating a mixture of two different halides with silver nitrate when their values are sufficiently different. Each step behaves, locally, like its own miniature version of the general titration curve, with its own local equivalence point and its own local excess-reagent/equilibrium-constant/excess-titrant structure; the overall curve is the concatenation of these local sigmoids. Resolution of the two steps requires the ratio of the relevant equilibrium constants (e.g., , or the two values) to be large enough — typically several orders of magnitude — that the second step does not begin appreciably before the first has essentially finished.
How is the "general titration curve" different for redox titrations compared to acid–base or precipitation titrations?
The core three-region logic — pre-equivalence excess-analyte control, equivalence-point equilibrium control, post-equivalence excess-titrant control — is identical, but the governing expression is the Nernst equation for each redox couple rather than or . Because the Nernst equation for a couple depends on the ratio of oxidized to reduced forms rather than an absolute concentration, the pre- and post-equivalence regions are each controlled by a single couple's Nernst equation (Fe³⁺/Fe²⁺ before equivalence, Ce⁴⁺/Ce³⁺ after, in the classic example), and the equivalence potential itself is a weighted average of the two standard (formal) potentials, weighted by the number of electrons each couple transfers. The steepness of a redox break is governed not by a single equilibrium constant but by the difference between the two formal potentials, ; a larger separation gives a sharper, more useful break, exactly analogous to a larger giving a sharper break in acid–base or precipitation titrations.