Superacids: Definition and Hammett Acidity

Drop a paraffin wax candle into fluoroantimonic acid and it dissolves. It becomes protonated and cracked into smaller cations. This happens at room temperature and without a catalyst — something concentrated sulfuric acid cannot touch. This single demonstration announces the existence of a class of acids so aggressive that the ordinary pH scale simply stops making sense. That scale was built for dilute aqueous solutions. Superacids protonate substrates that are functionally inert toward every acid found on a laboratory shelf. These substrates include alkanes, noble-gas compounds, even the C–H bonds of methane. Doing so requires both a new definition of "how acidic" and a new physical picture of what makes an acid strong. The problem superacids solve is one of measurement as much as synthesis. Water levels all acids stronger than H3O+\text{H}_3\text{O}^+. Put HCl, HNO3_3, or HClO4_4 into water and each simply protonates the solvent completely. So all "appear" equally strong — the leveling effect familiar from Differentiating Solvents and Extending the pH Scale. To rank acids far stronger than aqueous acids, chemists needed a differentiating medium. They also needed an acidity scale untethered from water activity: the Hammett acidity function H0H_0. Superacidity is then defined operationally. An acid is a superacid if it is stronger than 100% sulfuric acid, i.e. H0<−12H_0 < -12. The champions of the field are fluorosulfuric acid activated by SbF5\text{SbF}_5 ("magic acid," FSO3H⋅SbF5\text{FSO}_3\text{H}\cdot\text{SbF}_5) and the fluoroantimonic acid system (HF⋅SbF5\text{HF}\cdot\text{SbF}_5). These reach H0H_0 values below −25-25. That is more than a trillion-fold stronger than pure sulfuric acid on the Hammett scale. The chemistry behind this strength is a story in Lewis acid–Brønsted acid synergy. Antimony pentafluoride is an extraordinarily strong fluoride-ion acceptor. This is a direct consequence of the Lewis Acidity Trends in Main-Group Halides governing the group 15 pentahalides. It does its work not by donating a proton itself. Instead, it rips the conjugate base away from a Brønsted acid. This generates an enormous, exquisitely non-coordinating anion. Removing the conjugate base removes the only thing holding the proton back. The resulting "naked" proton, solvated only weakly, becomes ferociously electrophilic. This coupling of Brønsted donor and Lewis acceptor into one conjugate superacid system is the mechanistic heart of the subject. It is the reason superacid chemistry opens doors — stable carbocations, protonated methane, cationic noble-gas species. No purely aqueous or even purely Brønsted acidic medium can open these doors. This article builds the Hammett acidity function from its thermodynamic definition. It works through the fluoride-ion-affinity argument that explains why SbF5\text{SbF}_5 is the premier Lewis-acid activator. It quantifies magic acid and fluoroantimonic acid with real H0H_0 values. It also gives structural detail on the resulting anions. It finishes with worked numerical examples, common misconceptions, and the modern uses of these systems in petrochemistry and cation chemistry. It sets up the companion territory of non-aqueous Brønsted media explored in Reactions in Anhydrous Sulfuric Acid and BrF3.

Key takeaways
  • Superacids are defined operationally: any medium with Hammett acidity H0H_0 more negative than −12-12, the value for pure H2SO4\text{H}_2\text{SO}_4.
  • H0H_0 replaces pH because water and dilute aqueous scales cannot rank acids stronger than H3O+\text{H}_3\text{O}^+ (the leveling effect).
  • H0H_0 is measured using Hammett indicator bases via H0=pKBH+−log⁡([BH+]/[B])H_0 = \mathrm{p}K_{\mathrm{BH^+}} - \log([\text{BH}^+]/[\text{B}]).
  • Magic acid (FSO3H⋅SbF5\text{FSO}_3\text{H}\cdot\text{SbF}_5) and fluoroantimonic acid (HF⋅SbF5\text{HF}\cdot\text{SbF}_5) owe their power to SbF5\text{SbF}_5 stripping fluoride from the conjugate base, generating huge, weakly coordinating anions like Sb2F11−\text{Sb}_2\text{F}_{11}^-.
  • A "naked," poorly solvated proton is far more electrophilic than one paired with a good nucleobase — this is why conjugate Brønsted–Lewis superacids beat any single-component acid.
  • Key idea: superacidity is maximized not by making the proton donor stronger in isolation, but by making its conjugate base as large, delocalized, and non-basic as possible.
The core insight

A Brønsted acid becomes a superacid when a strong Lewis acid removes its conjugate base as a stable, low-basicity fluoro-anion, leaving behind a proton so poorly stabilized that it protonates substrates ordinary acids cannot touch.

Where this lives today

Superacid chemistry is not a museum piece; it underlies real industrial and analytical processes. Solid superacids (sulfated zirconia, sulfated titania, and related sulfate-promoted metal oxides, which mimic the local H0H_0 environment of liquid superacids on a surface) are used industrially as heterogeneous catalysts for alkane isomerization and alkylation, replacing older liquid HF- or H2SO4\text{H}_2\text{SO}_4-based processes in some refinery contexts because solids are easier to separate, recycle, and contain safely. Superacid-mediated alkylation and isomerization chemistry underlies the production of high-octane branched alkanes for gasoline blending, a direct descendant of the same Brønsted–Lewis conjugate-acid chemistry described here. In fundamental and preparative inorganic chemistry, fluoroantimonic-acid-type media remain the tool of choice for generating and stabilizing exotic cations that are too reactive to exist in any conventional solvent: protonated noble-gas compounds, halogen and interhalogen cations, and a wide range of main-group Lewis-acid-stabilized cations used to probe the limits of chemical bonding. Superacid systems are also central to modern mechanistic organic chemistry, where stable-ion NMR studies in SbF5\text{SbF}_5-based media continue to test computational predictions of nonclassical carbocation structures (bridged, "non-classical" cations analogous to the norbornyl cation problem) against experiment. The conceptual machinery built here — a differentiating acidity scale detached from water, and a Lewis-acid/Brønsted-acid synergy that both strengthens the acid and shrinks the basicity of its conjugate base — recurs directly in the chemistry of anhydrous sulfuric acid and of halogen fluorides such as BrF3\text{BrF}_3, both of which are self-ionizing, highly differentiating, non-aqueous solvent systems where the same Hammett-style logic and the same "weakly coordinating anion" strategy reappear in new structural clothing.

Ask the tutor: How does the Hammett acidity function get extended and calibrated when no single indicator's protonation ratio is measurable across the whole range from water to fluoroantimonic acid?

The physical picture

Ordinary acid strength in water is bounded above by the strength of H3O+\text{H}_3\text{O}^+: any acid HA with pKa\text{p}K_a more negative than about −1.7-1.7 transfers its proton to water essentially quantitatively, and the solution's acidity is capped at whatever [H3O+][\text{H}_3\text{O}^+] the concentration allows. This is the leveling effect, and it means pH — defined via water activity and hydronium concentration — cannot distinguish HClO4_4 from HI in water: both look "100% dissociated." To go further, chemists move to a non-leveling, non-aqueous solvent (concentrated H2SO4\text{H}_2\text{SO}_4, HF\text{HF}, FSO3H\text{FSO}_3\text{H}) and define acidity through the equilibrium behavior of a dissolved neutral indicator base B that protonates to BH+^+:

B+H+⇌BH+\text{B} + \text{H}^+ \rightleftharpoons \text{BH}^+

Because the indicator's protonation state can be read spectrophotometrically (B and BH+^+ typically have very different UV-visible spectra, usually a color change), and because a chain of overlapping indicators with known aqueous pKBH+\text{p}K_{\text{BH}^+} values can be used to "walk" the scale from water into the superacid regime, the acidity of the medium can be quantified far beyond where pH electrodes or water-based indicators would work at all. This walk is exactly how Louis Hammett built the H0H_0 function in the 1930s for concentrated sulfuric acid solutions, and it was later extended by Ronald Gillespie and George Olah into the superacid regime. Structurally, the "magic" of magic acid and fluoroantimonic acid is a Lewis-acid/Brønsted-acid handshake. SbF5\text{SbF}_5 is a strong fluoride-ion acceptor because antimony(V) is a small, highly electrophilic d0d^0 center that becomes octahedral (or forms fluorine-bridged oligomers) upon accepting F−^-, releasing considerable lattice/coordination stabilization. When SbF5\text{SbF}_5 is dissolved in HF or FSO3_3H, it abstracts a fluoride (or fluorosulfate) from the solvent's conjugate base pathway, producing large, delocalized, weakly basic anions such as SbF6−\text{SbF}_6^-, Sb2F11−\text{Sb}_2\text{F}_{11}^-, or Sb2F10(SO3F)−\text{Sb}_2\text{F}_{10}(\text{SO}_3\text{F})^-. The proton left behind in solution is now paired with an anion that has essentially no desire to take it back — hence "superacid."

Figure
Fluoride abstraction: how SbF5 converts HF into a superacid
Step 1: HF autoionization equilibrium (weak, restrained by F⁻ basicity) 2 HF ⇌ H₂F⁺ + F⁻ F⁻ is a decent base — it recombines readily, keeping acidity modest Step 2: SbF5 intercepts F⁻, forming a huge non-basic anion F⁻ + SbF₅ → SbF₆⁻ SbF₆⁻ + SbF₅ → Sb₂F₁₁⁻ Charge delocalized over two Sb centers and eleven F atoms: anion basicity collapses, H⁺ is left almost "naked" Sb₂F₁₁⁻ sketch Sb Sb F (bridge) each Sb: 5 more terminal F (octahedral, not drawn) total charge −1 spread over 2 Sb + 11 F
Figure
Hammett acidity ladder: from water to fluoroantimonic acid
H₀ scale (more negative = more acidic) 0 pure water, pH 7 region −12 100% H₂SO₄ (H₀ = −12), the superacid threshold −15 HF (anhydrous), H₀ ≈ −15 −19 FSO₃H (anhydrous), H₀ ≈ −15 to −19 dep. on purity −21 to −23 FSO₃H·SbF₅ "magic acid" (10–90 mol% SbF₅) −21 to −28 HF·SbF₅ "fluoroantimonic acid" — strongest known Note: exact H₀ depends sensitively on SbF₅ mole fraction and water content

The picture that emerges is that superacidity is not primarily about a stronger O–H or F–H bond being easier to break; it is about what happens to the fragment left behind. Removing basicity from the conjugate base is the lever, and SbF5\text{SbF}_5's exceptional fluoride-ion affinity — among the highest of any simple molecule — is what pulls that lever hardest.

The core ideas

The central quantitative object is the Hammett acidity function, defined for a neutral indicator base B that protonates according to B+H+⇌BH+\text{B} + \text{H}^+ \rightleftharpoons \text{BH}^+:

H0=pKBH+−log⁡[BH+][B]H_0 = \mathrm{p}K_{\mathrm{BH^+}} - \log\frac{[\text{BH}^+]}{[\text{B}]}

where:

  • pKBH+\mathrm{p}K_{\mathrm{BH^+}} is the (aqueous-referenced) acid dissociation constant of the protonated indicator, −log⁡KBH+-\log K_{\mathrm{BH^+}}, determined in dilute aqueous acid where normal pH applies,
  • [BH+]/[B][\text{BH}^+]/[\text{B}] is the ratio of protonated to neutral indicator measured spectrophotometrically in the medium of interest,
  • H0H_0 reduces to ordinary pH in dilute aqueous solution, since there [BH+]/[B]→KBH+[H+]/γ[\text{BH}^+]/[\text{B}] \to K_{\mathrm{BH^+}}[\text{H}^+]/\gamma-type ideal behavior and the activity coefficient terms cancel to leading order.

Reading it: H0H_0 measures the proton-donating power per unit indicator conversion, referenced back to water through the indicator's known pKBH+\mathrm{p}K_{\mathrm{BH^+}}. A more negative H0H_0 means the medium can push a much weaker base (more electron-poor B, more negative intrinsic pKBH+\mathrm{p}K_{\mathrm{BH^+}}) over to the protonated form. Because indicators overlap in usable range, a "ladder" of nitroanilines and related weak bases lets H0H_0 be extended continuously from water's mild acids down to −25-25 or beyond. The underlying thermodynamic definition, from which the operational formula is derived, is

H0=−log⁡aH+−log⁡γBγBH+H_0 = -\log a_{\mathrm{H^+}} - \log\frac{\gamma_{\mathrm{B}}}{\gamma_{\mathrm{BH^+}}}

where:

  • aH+a_{\mathrm{H^+}} is the (formally undefined-in-isolation, but thermodynamically consistent) proton activity in the medium,
  • γB\gamma_{\mathrm{B}} and γBH+\gamma_{\mathrm{BH^+}} are activity coefficients of the neutral base and its conjugate acid,
  • the ratio of activity coefficients is assumed approximately constant across a family of structurally similar indicators (the "Hammett postulate"), which is what allows different indicators to be strung together onto one continuous scale.

Reading it: H0H_0 is explicitly not −log⁡[H+]-\log[\text{H}^+]; it folds in the non-ideality of a concentrated, often highly structured medium (ion pairing, hydrogen-bonded networks, extensive solvation change) that makes naive concentration-based pH meaningless in these solvents. The second governing relationship connects Lewis acidity of the activator to the acidity gain, via fluoride-ion affinity (FIA), the enthalpy of the gas-phase reaction MFn+F−→MFn+1−\text{MF}_n + \text{F}^- \to \text{MF}_{n+1}^-:

ΔHFIA=−ΔH∘(MFn(g)+F−(g)→MFn+1−(g))\Delta H_{\mathrm{FIA}} = -\Delta H^\circ\left(\text{MF}_n(g) + \text{F}^-(g) \rightarrow \text{MF}_{n+1}^-(g)\right)

where:

  • larger positive ΔHFIA\Delta H_{\mathrm{FIA}} means the Lewis acid MFn_n binds F−^- more strongly (a more negative reaction enthalpy, reported as a positive affinity by convention),
  • SbF5\text{SbF}_5 has one of the largest known fluoride-ion affinities among simple molecular fluorides (of order 100 kJ mol−1^{-1} larger than typical group 13/14 fluorides like BF3_3 or PF5_5),
  • this affinity is the thermodynamic driving force that pulls F−^- away from HF or FSO3_3H and traps it as SbF6−\text{SbF}_6^- or Sb2F11−\text{Sb}_2\text{F}_{11}^-.

Reading it: whichever Lewis acid has the largest FIA will, all else equal, generate the strongest conjugate superacid when paired with a given Brønsted acid, because it most effectively suppresses the basicity of the leaving conjugate-base fragment.

Derivation AWhy H0 becomes more negative than pH — leaving the dilute, ideal regime

Goal: show explicitly how H0H_0 generalizes pH and why it can run far past the aqueous pH scale's floor.

Step 1 — start from the protonation equilibrium. For indicator B in any acidic medium, thermodynamic equilibrium requires

KBH+=aB aH+aBH+K_{\mathrm{BH^+}} = \frac{a_{\mathrm{B}}\, a_{\mathrm{H^+}}}{a_{\mathrm{BH^+}}}

where activities ai=γicia_i = \gamma_i c_i for each species. This is exact; no assumption about the solvent has been made yet.

Step 2 — rearrange for the proton activity. Solving for aH+a_{\mathrm{H^+}},

aH+=KBH+⋅aBH+aB=KBH+⋅γBH+γB⋅[BH+][B]a_{\mathrm{H^+}} = K_{\mathrm{BH^+}} \cdot \frac{a_{\mathrm{BH^+}}}{a_{\mathrm{B}}} = K_{\mathrm{BH^+}} \cdot \frac{\gamma_{\mathrm{BH^+}}}{\gamma_{\mathrm{B}}}\cdot\frac{[\mathrm{BH^+}]}{[\mathrm{B}]}

Taking −log⁡-\log of both sides,

−log⁡aH+=pKBH+−log⁡[BH+][B]−log⁡γBH+γB-\log a_{\mathrm{H^+}} = \mathrm{p}K_{\mathrm{BH^+}} - \log\frac{[\mathrm{BH^+}]}{[\mathrm{B}]} - \log\frac{\gamma_{\mathrm{BH^+}}}{\gamma_{\mathrm{B}}}

Step 3 — define H0 to absorb the activity-coefficient ratio. Hammett's insight was to define the acidity function as

H0≡pKBH+−log⁡[BH+][B]H_0 \equiv \mathrm{p}K_{\mathrm{BH^+}} - \log\frac{[\mathrm{BH^+}]}{[\mathrm{B}]}

which is exactly −log⁡aH++log⁡(γBH+/γB)-\log a_{\mathrm{H^+}} + \log(\gamma_{\mathrm{BH^+}}/\gamma_{\mathrm{B}}). Provided the activity coefficient ratio is roughly the same for structurally similar indicators (the Hammett postulate), H0H_0 is a medium-only property, transferable between different indicator molecules, and closely tracks −log⁡aH+-\log a_{\mathrm{H^+}}.

Step 4 — why this escapes the pH floor. In dilute aqueous acid, γi→1\gamma_i \to 1 and aH+→[H+]a_{\mathrm{H^+}} \to [\mathrm{H^+}], so H0→pHH_0 \to \mathrm{pH}: the two scales coincide exactly in the ideal, dilute limit, which is the required limiting-case check. But in concentrated H2SO4\text{H}_2\text{SO}_4 or fluoroantimonic acid, water activity is essentially removed from the system (there may be no bulk water at all), hydrogen-bonded proton-transport networks massively lower the effective solvation energy penalty for full protonation, and γB/γBH+\gamma_{\mathrm{B}}/\gamma_{\mathrm{BH^+}} departs enormously from unity. The proton activity aH+a_{\mathrm{H^+}} — not concentration — can become astronomically large in the thermodynamic sense because the reference state (dilute aqueous solution) is so different from the medium. H0H_0 correctly tracks this because it is built from equilibrium indicator behavior, not from a concentration that has no meaningful upper bound analogue to [H+][\mathrm{H}^+] in water.

Step 5 — chaining indicators. Because no single indicator has a measurable [BH+]/[B][\mathrm{BH^+}]/[\mathrm{B}] ratio across the entire range (weak bases are fully protonated in strong acid; strong bases are fully protonated even in weak acid), the scale is built by overlapping a sequence of indicators B1,B2,…\mathrm{B}_1, \mathrm{B}_2, \ldots of decreasing intrinsic basicity. Each new indicator's pKBH+\mathrm{p}K_{\mathrm{BH^+}} is calibrated in a solution where the previous indicator's ratio is still measurable, and H0H_0 is extended monotonically. This iterative overlap is exactly how the scale reaches values like −24-24 for magic acid — far below where any single spectrophotometric measurement alone could reach.

Go deeper · Derivation B · 2 minFluoride-ion affinity and the "naked proton" argument for superacid strength
Derivation BFluoride-ion affinity and the "naked proton" argument for superacid strength

Goal: derive, from a thermodynamic cycle, why pairing HF (or FSO3_3H) with SbF5_5 produces a far stronger acid than either component alone, and quantify the driving force.

Step 1 — write the overall protonation the superacid must perform. For a generic substrate S being protonated in the HF/SbF5_5 system,

S+2 HF+SbF5→SH++SbF6−\text{S} + 2\,\text{HF} + \text{SbF}_5 \rightarrow \text{SH}^+ + \text{SbF}_6^-

This can be decomposed into a thermodynamic cycle: (i) autoionization of HF to give H+\text{H}^+ (formally) and F−\text{F}^-; (ii) capture of F−^- by SbF5_5; (iii) transfer of the resulting "free" proton to S.

Step 2 — isolate the fluoride-capture step. The key intermediate equilibrium is

HF⇌H++F−,ΔH1=+(large, unfavorable)\text{HF} \rightleftharpoons \text{H}^+ + \text{F}^-, \qquad \Delta H_1 = +\text{(large, unfavorable)}
F−+SbF5→SbF6−,ΔH2=−ΔHFIA(SbF5)(large, favorable)\text{F}^- + \text{SbF}_5 \rightarrow \text{SbF}_6^-, \qquad \Delta H_2 = -\Delta H_{\mathrm{FIA}}(\text{SbF}_5) \quad \text{(large, favorable)}

Adding these,

HF+SbF5→H++SbF6−,ΔH=ΔH1−ΔHFIA(SbF5)\text{HF} + \text{SbF}_5 \rightarrow \text{H}^+ + \text{SbF}_6^-, \qquad \Delta H = \Delta H_1 - \Delta H_{\mathrm{FIA}}(\text{SbF}_5)

Because ΔHFIA(SbF5)\Delta H_{\mathrm{FIA}}(\text{SbF}_5) is very large (among the largest of any simple fluoride), this composite step is far less endothermic than bare HF ionization alone, i.e. HF is effectively "helped" to ionize by SbF5_5 soaking up the fluoride.

Step 3 — compare conjugate-base basicity before and after. F−^- itself is a moderately strong Brønsted base (conjugate to HF, itself a weak acid in water, Ka∼10−3.2K_a \sim 10^{-3.2}): it readily recombines with H+^+, which is exactly why pure HF is not a superacid outright (H0≈−15H_0 \approx -15, respectable but well short of magic acid). Once F−^- is captured as SbF6−\text{SbF}_6^-, or further oligomerized to Sb2F11−\text{Sb}_2\text{F}_{11}^- (by a second equivalent of SbF5_5 attacking SbF6−\text{SbF}_6^-), the negative charge is delocalized over two metal centers and eleven fluorine atoms. The basicity of this anion toward H+\text{H}^+ is dramatically suppressed relative to F−^-: its conjugate acid ("H–Sb2_2F11_{11}") is effectively nonexistent as a discrete species, meaning the anion simply will not take the proton back.

Step 4 — quantify the acidity gain via the pKa-shift picture. Treating this as a Brønsted-type free-energy relationship, the overall driving force to protonate substrate S can be written as a sum of two terms,

ΔGoverall=ΔGionize(H–A)−ΔGFIA(Lewis acid)+ΔGsolv(SH+,anion)\Delta G_{\text{overall}} = \Delta G_{\text{ionize}}(\text{H–A}) - \Delta G_{\text{FIA}}(\text{Lewis acid}) + \Delta G_{\text{solv}}(\text{SH}^+, \text{anion})

where the second term is large and negative for SbF5_5 (strong Lewis acid) and the third term is small in magnitude because the huge, diffuse, low-charge-density anion solvates and ion-pairs only weakly with SH+^+ — it neither pulls the proton back electrostatically nor engages in strong hydrogen bonding. The near-absence of anion basicity, not a uniquely strong H–F or H–OSO2_2F bond, is what pushes H0H_0 from about −15-15 (HF alone) to below −25-25 (HF·SbF5_5).

Step 5 — limiting case check. As the mole fraction of SbF5_5 is decreased toward zero, ΔGFIA\Delta G_{\mathrm{FIA}} contribution vanishes and the system smoothly recovers the acidity of pure HF (H0≈−15H_0 \approx -15) or pure FSO3_3H (H0≈−15H_0 \approx -15 to −19-19), confirming the derivation collapses correctly onto the single-component limit. Conversely, as SbF5_5 mole fraction approaches unity in the FSO3_3H system, the acidity strengthens further as more Sb2F11−\text{Sb}_2\text{F}_{11}^- and even Sb3F16−\text{Sb}_3\text{F}_{16}^- form, tracking the increasing effective FIA of the oligomerized antimony fluoride species — consistent with the experimentally observed dependence of magic acid's H0H_0 on SbF5_5 loading.

Worked examples

Example 1 (foundational): computing H0 from an indicator ratio. Suppose an indicator base B (a substituted nitroaniline) has aqueous pKBH+=−0.94\mathrm{p}K_{\mathrm{BH^+}} = -0.94 (a typical Hammett indicator value), and in a given sulfuric acid mixture the spectrophotometrically measured ratio is [BH+]/[B]=6.3[\mathrm{BH^+}]/[\mathrm{B}] = 6.3. Then

H0=pKBH+−log⁡[BH+][B]=−0.94−log⁡(6.3)H_0 = \mathrm{p}K_{\mathrm{BH^+}} - \log\frac{[\mathrm{BH^+}]}{[\mathrm{B}]} = -0.94 - \log(6.3)
log⁡(6.3)=0.799\log(6.3) = 0.799
H0=−0.94−0.799=−1.74H_0 = -0.94 - 0.799 = -1.74

This corresponds to roughly 20–25 wt% aqueous sulfuric acid, well within the range where the Hammett scale was originally calibrated against real solution composition data — far from superacid territory (H0<−12H_0 < -12), illustrating that most of the useful "acid strength differentiation" work happens long before superacidity is reached. As a limiting-case check: if the ratio were exactly 1 (equal populations of B and BH+^+), H0=pKBH+H_0 = \mathrm{p}K_{\mathrm{BH^+}} exactly, which is the defining calibration point for any indicator — the acidity at which that particular indicator is half-protonated.

Example 2 (applied): estimating the acid strength needed to protonate a very weak base, and comparing HF to HF·SbF5. Suppose we want to protonate a very weakly basic ketone-type substrate with intrinsic pKBH+=−8.2\mathrm{p}K_{\mathrm{BH^+}} = -8.2 to the extent of 95% conversion (i.e. [BH+]/[B]=19[\mathrm{BH^+}]/[\mathrm{B}] = 19). The required medium acidity is

H0required=pKBH+−log⁡(19)=−8.2−1.28=−9.48H_0^{\text{required}} = \mathrm{p}K_{\mathrm{BH^+}} - \log(19) = -8.2 - 1.28 = -9.48

Pure water obviously cannot reach H0=−9.48H_0 = -9.48 (it levels out near pH 0–1 at best for concentrated strong acid, since H3O+\text{H}_3\text{O}^+ is the strongest acid species present). Concentrated sulfuric acid, with H0≈−12H_0 \approx -12 at 100% concentration, comfortably clears this threshold, achieving well over 95% conversion. But now consider a substrate with pKBH+=−21.5\mathrm{p}K_{\mathrm{BH^+}} = -21.5 (representative of extremely weak bases such as simple alkanes being protonated toward carbonium-ion-like transition states, or CH4_4 itself) requiring the same 95% conversion:

H0required=−21.5−1.28=−22.8H_0^{\text{required}} = -21.5 - 1.28 = -22.8

Sulfuric acid (H0=−12H_0 = -12) fails by ten orders of magnitude in the underlying activity ratio. Magic acid, with H0H_0 typically in the −21-21 to −24-24 range depending on SbF5_5 loading, sits right at the edge, while fluoroantimonic acid, capable of H0H_0 below −25-25, clears the threshold decisively — consistent with the experimental observation that superprotonation of alkanes (giving nonclassical carbonium ions such as protonated methane, CH5+\text{CH}_5^+) is achieved specifically in HF⋅SbF5\text{HF}\cdot\text{SbF}_5 and not in ordinary strong acids.

Example 3 (exam/competition-level): fluoride-ion affinity ranking and predicting relative H0 shift. Given approximate gas-phase fluoride-ion affinities (kJ mol−1^{-1}, illustrative literature-consistent values): BF3\text{BF}_3: 350; PF5\text{PF}_5: 410; AsF5\text{AsF}_5: 435; SbF5\text{SbF}_5: 495. A superacid chemist wants to activate FSO3_3H with the cheapest Lewis acid that still yields H0<−18H_0 < -18. Using the (empirically observed, roughly linear over this narrow range) trend that each 50 kJ mol−1^{-1} increase in FIA shifts H0H_0 by approximately −1.3-1.3 units relative to a BF3_3-activated baseline of H0≈−15.0H_0 \approx -15.0: For AsF5_5 (ΔFIA\Delta\text{FIA} relative to BF3_3 =435−350=85= 435 - 350 = 85 kJ mol−1^{-1}):

ΔH0≈−(8550)(1.3)=−2.21\Delta H_0 \approx -\left(\frac{85}{50}\right)(1.3) = -2.21
H0(AsF5-activated)≈−15.0−2.21=−17.2H_0(\text{AsF}_5\text{-activated}) \approx -15.0 - 2.21 = -17.2

This falls just short of the −18-18 target. For SbF5_5 (ΔFIA=495−350=145\Delta\text{FIA} = 495 - 350 = 145 kJ mol−1^{-1}):

ΔH0≈−(14550)(1.3)=−3.77\Delta H_0 \approx -\left(\frac{145}{50}\right)(1.3) = -3.77
H0(SbF5-activated)≈−15.0−3.77=−18.8H_0(\text{SbF}_5\text{-activated}) \approx -15.0 - 3.77 = -18.8

SbF5_5 clears the target; AsF5_5 does not, despite AsF5_5 being a respectable Lewis acid in its own right — illustrating why SbF5_5, not AsF5_5 or PF5_5, is the industry-standard activator even though it is more expensive and more corrosively reactive. (These proportionality constants are illustrative pedagogical estimates for teaching the scaling trend, not a literature-fitted regression; the qualitative ordering BF3_3 < PF5_5 < AsF5_5 < SbF5_5 in both FIA and resulting H0H_0 is the experimentally robust result.) As a limiting check: setting FIA equal to the BF3_3 reference value recovers ΔH0=0\Delta H_0 = 0 exactly, i.e. H0=−15.0H_0 = -15.0, consistent by construction with using BF3_3 as the zero-point of the relative scale.

Limiting cases, scope & common traps

RegimeWhat happensCorrect statement
Dilute aqueous acidγi→1\gamma_i \to 1H0→pHH_0 \to \mathrm{pH} exactly; the two scales coincide
Concentrated aqueous strong acid (e.g. 12 M HCl)Leveling by waterAll strong acids look identical in dilute water; H0H_0 in concentrated solutions differentiates them, but pure water itself never reaches superacid H0H_0
Pure H2SO4\text{H}_2\text{SO}_4Reference pointH0=−12H_0 = -12 by definition of the superacid threshold; not itself classified as a superacid
HF\text{HF} or FSO3H\text{FSO}_3\text{H} aloneModerate conjugate-base basicityAlready a strong acid (H0≈−13H_0\approx -13 to −15-15), but conjugate base (F−^-, FSO3−_3^-) is still basic enough to limit full superacidity
FSO3H⋅SbF5\text{FSO}_3\text{H}\cdot\text{SbF}_5 (magic acid)Fluoride/fluorosulfate abstractionH0H_0 typically −21-21 to −24-24; strongly dependent on SbF5_5 mole fraction
HF⋅SbF5\text{HF}\cdot\text{SbF}_5 (fluoroantimonic acid)Maximal anion delocalization (Sb2F11−\text{Sb}_2\text{F}_{11}^-, Sb3F16−\text{Sb}_3\text{F}_{16}^-)Strongest characterized superacid system, H0H_0 below −25-25
Excess SbF5_5 beyond saturationDiminishing returns / phase separationH0H_0 does not decrease without bound; solubility and oligomer speciation limit further gains

The chemist behind it

Origins · 1 minGeorge A. Olah and how this was discovered
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George A. Olah
1927–2017 · Cleveland, Case Western Reserve University and University of Southern California, 1960s–2000s

Hungarian-born chemist who fled the 1956 uprising and later built superacid chemistry into a mature discipline in North America. Olah's systematic use of FSO3H⋅SbF5\text{FSO}_3\text{H}\cdot\text{SbF}_5 and HF⋅SbF5\text{HF}\cdot\text{SbF}_5 let him generate and directly observe long-lived carbocations by NMR — species previously known only as fleeting reaction intermediates — overturning the assumption that carbocations were too reactive to characterize structurally. He coined the term "superacid" for these media and extended their use to protonate hydrocarbons, generating protonated methane CH5+\text{CH}_5^+ and related nonclassical cations, work recognized with the 1994 Nobel Prize in Chemistry "for his contribution to carbocation chemistry."

Olah's work rested on foundations laid by Ronald Gillespie, who characterized the fluorosulfuric acid/antimony pentafluoride and related systems structurally and quantified their Hammett acidities in the 1960s, and by Louis Hammett himself, whose 1930s acidity function work in concentrated sulfuric acid provided the entire measurement framework that superacid chemistry would later extend by two more orders of magnitude in H0H_0.

Origins · 1 minhow this was discovered
History
- 1932–1934 — Louis Hammett and A. J. Deyrup define the H0H_0 acidity function using nitroaniline indicators in aqueous sulfuric acid.
- 1966 — Ronald Gillespie and coworkers characterize FSO3H⋅SbF5\text{FSO}_3\text{H}\cdot\text{SbF}_5 and quantify its exceptional acidity, laying groundwork for the term "superacid."
- Early 1970s — George Olah's group uses magic acid and fluoroantimonic acid to generate and observe stable, long-lived carbocations by low-temperature NMR.
- 1973 — Olah reports direct observation of protonated methane, CH5+\text{CH}_5^+, in superacid media.
- 1994 — Olah receives the Nobel Prize in Chemistry for carbocation chemistry developed largely using superacid systems.
Why can't we just measure superacid strength with a pH meter?

A pH meter reports −log⁡aH+-\log a_{\mathrm{H^+}} referenced to dilute aqueous standards and calibrated against buffers whose behavior assumes near-ideal, dilute aqueous solution chemistry. In concentrated superacid media there may be little or no bulk water, activity coefficients depart enormously from unity, and the electrode's response mechanism (ion exchange through a hydrated glass membrane) simply breaks down or corrodes outright in HF/SbF5_5 mixtures. The Hammett function sidesteps all of this by using the equilibrium protonation state of a dissolved indicator base, measured optically, which remains well-defined and reproducible far outside the electrode's operating range.

Is 100% sulfuric acid itself a superacid?

No — by the standard operational definition, 100% sulfuric acid, with H0=−12H_0 = -12, is the reference threshold, not a member of the superacid class. A superacid must be stronger than pure sulfuric acid, i.e. H0<−12H_0 < -12. This threshold was chosen precisely because H2SO4\text{H}_2\text{SO}_4 was, for decades, the strongest common laboratory Brønsted acid, so anything surpassing it represented a genuinely new acidity regime worth naming separately.

Why does the anion's structure matter so much for acid strength?

The proton's electrophilicity in solution is controlled by how strongly its counter-anion wants it back. A small, localized, high-charge-density anion like F−^- or Cl−^- hydrogen-bonds or ion-pairs strongly with H+^+, effectively "sharing" and stabilizing the positive charge, which weakens the acid. Anions like Sb2F11−\text{Sb}_2\text{F}_{11}^- or Sb3F16−\text{Sb}_3\text{F}_{16}^- spread their negative charge over many atoms and several metal centers, which lowers charge density everywhere on the anion's surface and makes it a poor hydrogen-bond acceptor and poor nucleophile — so it barely stabilizes the proton at all, leaving it maximally reactive toward substrates.

Does increasing SbF5 concentration always increase superacidity without limit?

No. Acidity increases with SbF5_5 mole fraction up to a point, tracking the formation of progressively larger, more delocalized polyfluoroantimonate anions (SbF6−→Sb2F11−→Sb3F16−\text{SbF}_6^- \to \text{Sb}_2\text{F}_{11}^- \to \text{Sb}_3\text{F}_{16}^-), but the trend saturates: solubility limits, viscosity increases, and the marginal fluoride affinity gained by adding yet another SbF5_5 unit to an already large oligomeric anion diminishes. Experimentally, H0H_0 approaches a practical ceiling near −26-26 to −28-28 for the most concentrated, well-characterized fluoroantimonic acid mixtures.

How is the Hammett indicator method actually carried out in practice?

A small amount of a weakly basic, strongly UV-visible indicator (commonly a substituted nitroaniline or nitro-diphenylamine) is dissolved in the acid of interest, and the ratio of neutral (B) to protonated (BH+^+) forms is read from the intensity of characteristic absorption bands, since protonation typically shifts or extinguishes the neutral form's chromophore. Using the indicator's independently measured aqueous pKBH+\mathrm{p}K_{\mathrm{BH^+}}, this ratio converts directly into H0H_0 via the defining equation. A sequence of indicators of decreasing basicity, each calibrated where the previous indicator's signal is still measurable, extends the method continuously from mild acids to the superacid regime.

Are superacids dangerous to work with, and how are they handled?

Yes, systems like fluoroantimonic acid are exceptionally corrosive and reactive — they attack glass (via HF's known reactivity with silicates) and react violently with water, organic solvents, and many container materials. They are handled in specialized fluoropolymer (PTFE/PFA) or passivated metal vessels under strictly anhydrous, inert-atmosphere conditions, often at low temperature to control reactivity and to stabilize the reactive cationic intermediates (such as carbocations) that these acids are used to generate for spectroscopic study.

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