HSAB theory

HSAB is an acronym for "hard and soft (Lewis) acids and bases". HSAB is widely used in chemistry for explaining the stability of compounds, reaction mechanisms and pathways. It assigns the terms 'hard' or 'soft', and 'acid' or 'base' to chemical species. 'Hard' applies to species which are small, have high charge states (the charge criterion applies mainly to acids, to a lesser extent to bases), and are weakly polarizable. 'Soft' applies to species which are big, have low charge states and are strongly polarizable.^[1]

The theory is used in contexts where a qualitative, rather than quantitative, description would help in understanding the predominant factors which drive chemical properties and reactions. This is especially so in transition metal chemistry, where numerous experiments have been done to determine the relative ordering of ligands and transition metal ions in terms of their hardness and softness.

HSAB theory is also useful in predicting the products of metathesis reactions. In 2005 it was shown that even the sensitivity and performance of explosive materials can be explained on basis of HSAB theory.^[2]

Ralph Pearson introduced the HSAB principle in the early 1960s^[3]^[4]^[5] as an attempt to unify inorganic and organic reaction chemistry.^[6]

Theory

Hard–soft trends for acids and bases

Acids

Bases

Essentially, the theory states that soft acids prefer to form bonds with soft bases, whereas hard acids prefer to form bonds with hard bases, all other factors being equal.^[7] It can also be said that hard acids bind strongly to hard bases and soft acids bind strongly to soft bases. The HASB classification in the original work was largely based on equilibrium constants of Lewis acid/base reactions with a reference base for comparison.^[8]

Comparing tendencies of hard acids and bases vs. soft acids and bases
Property	Hard acids and bases	Soft acids and bases
atomic/ionic radius	small	large
oxidation state	high	low or zero
polarizability	low	high
electronegativity (bases)	high	low
HOMO energy of bases^[9]^[10]	low	higher
LUMO energy of acids^[9]^[10]	high	lower (but more than soft-base HOMO)
affinity	ionic bonding	covalent bonding

Examples of hard and soft acids and bases
Acids				Bases
hard		soft		hard		soft
Hydronium	H₃O⁺	Mercury	Hg₂²⁺	Hydroxide	OH⁻	Hydride	H⁻
Alkali metals	Li⁺,Na⁺,K⁺	Platinum	Pt²⁺	Alkoxide	RO⁻	Thiolate	RS⁻
Titanium	Ti⁴⁺	Palladium	Pd²⁺	Halogens	F⁻,Cl⁻	Halogens	I⁻
Chromium	Cr³⁺,Cr⁶⁺	Silver	Ag⁺	Ammonia	NH₃	Phosphine	PR₃
Boron trifluoride	BF₃	Borane	BH₃	Carboxylate	CH₃COO⁻	Thiocyanate	SCN⁻
Carbocation	R₃C⁺	P-chloranil	C₆Cl₄O₂	Carbonate	CO₃²⁻	Carbon monoxide	CO
Lanthanides	Ln³⁺	Bulk metals	M⁰	Hydrazine	N₂H₄	Benzene	C₆H₆
Thorium, uranium	Th⁴⁺, U⁴⁺	Gold	Au⁺

Borderline cases are also identified: borderline acids are trimethylborane, sulfur dioxide and ferrous Fe²⁺, cobalt Co²⁺ caesium Cs⁺ and lead Pb²⁺ cations. Borderline bases are: aniline, pyridine, nitrogen N₂ and the azide, chloride, bromide, nitrate and sulfate anions.

Generally speaking, acids and bases interact and the most stable interactions are hard–hard (

ionogenic character) and soft–soft (covalent

character).

An attempt to quantify the 'softness' of a base consists in determining the equilibrium constant for the following equilibrium:

BH + CH₃Hg⁺ ⇌ H⁺ + CH₃HgB

Where CH₃Hg⁺ (methylmercury ion) is a very soft acid and H⁺ (proton) is a hard acid, which compete for B (the base to be classified).

Some examples illustrating the effectiveness of the theory:

Bulk metals are soft acids and are poisoned by soft bases such as phosphines and sulfides.
Hard
aprotic solvents such as dimethyl sulfoxide and acetone
are soft solvents with a preference for solvating large anions and soft bases.

In

coordination chemistry

soft–soft and hard–hard interactions exist between ligands and metal centers.

Chemical hardness

Chemical hardness in
electron volt
Acids			Bases
Hydrogen	H⁺	∞	Fluoride	F⁻	7
Aluminium	Al³⁺	45.8	Ammonia	NH₃	6.8
Lithium	Li⁺	35.1	hydride	H⁻	6.8
Scandium	Sc³⁺	24.6	carbon monoxide	CO	6.0
Sodium	Na⁺	21.1	hydroxyl	OH⁻	5.6
Lanthanum	La³⁺	15.4	cyanide	CN⁻	5.3
Zinc	Zn²⁺	10.8	phosphine	PH₃	5.0
Carbon dioxide	CO₂	10.8	nitrite	NO₂⁻	4.5
Sulfur dioxide	SO₂	5.6	Hydrosulfide	SH⁻	4.1
Iodine	I₂	3.4	Methane	CH₃⁻	4.0
Table 2. Chemical hardness data^[11]

In 1983 Pearson together with

η) as being proportional to the second derivative of the total energy of a chemical system with respect to changes in the number of electrons at a fixed nuclear environment:^[11]

\eta ={\frac {1}{2}}\left({\frac {\partial ^{2}E}{\partial N^{2}}}\right)_{Z}

.

The factor of one-half is arbitrary and often dropped as Pearson has noted.[12]

An operational definition for the chemical hardness is obtained by applying a three-point finite difference approximation to the second derivative:^[13]

{\begin{aligned}\eta &\approx {\frac {E(N+1)-2E(N)+E(N-1)}{2}}\\&={\frac {(E(N-1)-E(N))-(E(N)-E(N+1))}{2}}\\&={\frac {1}{2}}(I-A)\end{aligned}}

where I is the

ionization potential and A the electron affinity. This expression implies that the chemical hardness is proportional to the band gap

of a chemical system, when a gap exists.

The first derivative of the energy with respect to the number of electrons is equal to the chemical potential, μ, of the system,

\mu =\left({\frac {\partial E}{\partial N}}\right)_{Z}

,

from which an operational definition for the chemical potential is obtained from a finite difference approximation to the first order derivative as

{\begin{aligned}\mu &\approx {\frac {E(N+1)-E(N-1)}{2}}\\&={\frac {-(E(N-1)-E(N))-(E(N)-E(N+1))}{2}}\\&=-{\frac {1}{2}}(I+A)\end{aligned}}

which is equal to the negative of the

Mulliken scale

: μ = −χ.

The hardness and Mulliken electronegativity are related as

2\eta =\left({\frac {\partial \mu }{\partial N}}\right)_{Z}\approx -\left({\frac {\partial \chi }{\partial N}}\right)_{Z}

,

and in this sense hardness is a measure for resistance to deformation or change. Likewise a value of zero denotes maximum softness, where softness is defined as the reciprocal of hardness.

In a compilation of hardness values only that of the hydride anion deviates. Another discrepancy noted in the original 1983 article are the apparent higher hardness of Tl³⁺ compared to Tl⁺.

Modifications

If the interaction between acid and base in solution results in an equilibrium mixture the strength of the interaction can be quantified in terms of an equilibrium constant. An alternative quantitative measure is the heat (enthalpy) of formation of the Lewis acid-base adduct in a non-coordinating solvent. The ECW model is quantitative model that describes and predicts the strength of Lewis acid base interactions, -ΔH . The model assigned E and C parameters to many Lewis acids and bases. Each acid is characterized by an E_A and a C_A. Each base is likewise characterized by its own E_B and C_B. The E and C parameters refer, respectively, to the electrostatic and covalent contributions to the strength of the bonds that the acid and base will form. The equation is

-ΔH = E_AE_B + C_AC_B + W

The W term represents a constant energy contribution for acid–base reaction such as the cleavage of a dimeric acid or base. The equation predicts reversal of acids and base strengths. The graphical presentations of the equation show that there is no single order of Lewis base strengths or Lewis acid strengths.^[14] The ECW model accommodates the failure of single parameter descriptions of acid-base interactions.

A related method adopting the E and C formalism of Drago and co-workers quantitatively predicts the formation constants for complexes of many metal ions plus the proton with a wide range of unidentate Lewis acids in aqueous solution, and also offered insights into factors governing HSAB behavior in solution.^[15]

Another quantitative system has been proposed, in which Lewis acid strength toward Lewis base fluoride is based on gas-phase affinity for fluoride.^[16] Additional one-parameter base strength scales have been presented.^[17] However, it has been shown that to define the order of Lewis base strength (or Lewis acid strength) at least two properties must be considered.^[18] For Pearson's qualitative HSAB theory the two properties are hardness and strength while for Drago's quantitative ECW model the two properties are electrostatic and covalent .

Kornblum's rule

An application of HSAB theory is the so-called Kornblum's rule (after

electronegative atom reacts when the reaction mechanism is S_N1 and the less electronegative one in a S_N2 reaction. This rule (established in 1954)^[19] predates HSAB theory but in HSAB terms its explanation is that in a S_N1 reaction the carbocation

(a hard acid) reacts with a hard base (high electronegativity) and that in a S_N2 reaction tetravalent carbon (a soft acid) reacts with soft bases.

According to findings, electrophilic alkylations at free CN⁻ occur preferentially at carbon, regardless of whether the S_N1 or S_N2 mechanism is involved and whether hard or soft electrophiles are employed. Preferred N attack, as postulated for hard electrophiles by the HSAB principle, could not be observed with any alkylating agent. Isocyano compounds are only formed with highly reactive electrophiles that react without an activation barrier because the diffusion limit is approached. It is claimed that the knowledge of absolute rate constants and not of the hardness of the reaction partners is needed to predict the outcome of alkylations of the cyanide ion.^[20]

Criticism

Reanalysis of a large number of various most typical ambident organic system reveals that thermodynamic/kinetic control describes reactivity of organic compounds perfectly, whereas the HSAB principle fails and should be abandoned in the rationalization of ambident reactivity of organic compounds.^[21]

References

ISBN 978-0-07-032760-3
.

^ [1] E.-C. Koch, Acid-Base Interactions in Energetic Materials: I. The Hard and Soft Acids and Bases (HSAB) Principle-Insights to Reactivity and Sensitivity of Energetic Materials, Prop.,Expl.,Pyrotech. 30 2005, 5

doi:10.1021/ja00905a001
.

doi:10.1021/ed045p581
.

doi:10.1021/ed045p643
.

^ [2] R. G. Pearson, Chemical Hardness – Applications From Molecules to Solids, Wiley-VCH, Weinheim, 1997, 198 pp

ISSN 1365-3075
.

ISSN 0002-7863
.

^
IUPAC, Glossary of terms used in theoretical organic chemistry
, accessed 16 Dec 2006.

^ ^a ^b Miessler G.L. and Tarr D.A. "Inorganic Chemistry" 2nd ed. Prentice-Hall 1999, p.181-5

^
doi:10.1021/ja00364a005
.

S2CID 96042488
.

ISBN 978-1-4020-4527-1
.

doi:10.1021/ed073p701
.

doi:10.1021/cr00098a011
.

ISSN 0022-1139
.

ISBN 978-0-470-74957-9

^ Cramer, R. E., and Bopp, T. T. (1977) Great E and C plot. Graphical display of the enthalpies of adduct formation for Lewis acids and bases. Journal of Chemical Education 54 612-613

doi:10.1021/ja01628a064

PMID 15599920
.

PMID 21726020
.

Retrieved from "https://en.wikipedia.org/w/index.php?title=HSAB_theory&oldid=1190100278"

[1] ISBN 978-0-07-032760-3
.

[2] [1] E.-C. Koch, Acid-Base Interactions in Energetic Materials: I. The Hard and Soft Acids and Bases (HSAB) Principle-Insights to Reactivity and Sensitivity of Energetic Materials, Prop.,Expl.,Pyrotech. 30 2005, 5

[3] :10.1021/ja00905a001
.

[4] :10.1021/ed045p581
.

[5] :10.1021/ed045p643
.

[6] [2] R. G. Pearson, Chemical Hardness – Applications From Molecules to Solids, Wiley-VCH, Weinheim, 1997, 198 pp

[7] ISSN 1365-3075
.

[8] ISSN 0002-7863
.

[IUPAC-9] 
IUPAC, Glossary of terms used in theoretical organic chemistry
, accessed 16 Dec 2006.

[Miessler-10] Miessler G.L. and Tarr D.A. "Inorganic Chemistry" 2nd ed. Prentice-Hall 1999, p.181-5

[abshardess-11] 
doi:10.1021/ja00364a005
.

[12] S2CID 96042488
.

[13] ISBN 978-1-4020-4527-1
.

[14] :10.1021/ed073p701
.

[15] :10.1021/cr00098a011
.

[16] ISSN 0022-1139
.

[17] ISBN 978-0-470-74957-9

[18] Cramer, R. E., and Bopp, T. T. (1977) Great E and C plot. Graphical display of the enthalpies of adduct formation for Lewis acids and bases. Journal of Chemical Education 54 612-613

[19] doi:10.1021/ja01628a064

[20] PMID 15599920
.

[21] PMID 21726020
.

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