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The ionic strength of a solution is a measure of the concentration of ions in that solution. Ionic compounds, when dissolved in water, dissociate into ions. The total electrolyte concentration in solution will affect important properties such as the dissociation constant or the solubility of different salts. One of the main characteristics of a solution with dissolved ions is the ionic strength. Ionic strength can be molar (mol/L solution) or molal (mol/kg solvent) and to avoid confusion the units should be stated explicitly.[1] The concept of ionic strength was first introduced by Lewis and Randall in 1921 while describing the activity coefficients of strong electrolytes.[2]
The molar ionic strength, I, of a solution is a function of the concentration of allions present in that solution.[3]
where one half is because we are including both cations and anions, ci is the molar concentration of ion i (M, mol/L), zi is the charge number of that ion, and the sum is taken over all ions in the solution. For a 1:1 electrolyte such as sodium chloride, where each ion is singly-charged, the ionic strength is equal to the concentration. For the electrolyte MgSO4, however, each ion is doubly-charged, leading to an ionic strength that is four times higher than an equivalent concentration of sodium chloride:
Multivalent ions, having a large , contribute strongly to the ionic strength.
As a more complex example, the ionic strength of a mixed solution containing 0.050 M in Na2SO4 and 0.020 M KCl is (assuming complete dissociation):
Because in non-ideal solutions volumes are no longer strictly additive it is often preferable to work with molalityb (mol/kg of H2O) rather than molarity c (mol/L). In that case, molal ionic strength is defined as:
in which
The ionic strength plays a central role in the Debye–Hückel theory that describes the strong deviations from ideality typically encountered in ionic solutions.[5][6] It is also important for the theory of double layer and related electrokinetic phenomena and electroacoustic phenomena in colloids and other heterogeneous systems. That is, the Debye length, which is the inverse of the Debye parameter (κ), is inversely proportional to the square root of the ionic strength. Both molar and molal ionic strength have been used, often without explicit definition. Debye length is characteristic of the double layer thickness. Increasing the concentration or valence of the counterions compresses the double layer and increases the electrical potentialgradient.
Media of high ionic strength are used in stability constant determination in order to minimize changes, during a titration, in the activity quotient of solutes at lower concentrations. Natural waters such as mineral water and seawater have often a non-negligible ionic strength due to the presence of dissolved salts which significantly affects their properties.
![{\displaystyle I={\frac {1}{2}}[c(+2)^{2}+c(-2)^{2}]={\frac {1}{2}}[4c+4c]=4c}](https://wikimedia.org/api/rest_v1/media/math/render/svg/4c3153d34f527dc9229f3cd4402029e72d149cb1)
![{\displaystyle {\begin{aligned}I&={\tfrac {1}{2}}\times \left[{\begin{array}{l}\{({\text{concentration of }}{\mathrm {Na} {\vphantom {A}}_{\smash[{t}]{2}}\mathrm {SO} {\vphantom {A}}_{\smash[{t}]{4}}}{\text{ in M}})\times ({\text{number of }}{\mathrm {Na} {\vphantom {A}}^{+}})\times ({\text{charge of }}{\mathrm {Na} {\vphantom {A}}^{+}})^{2}\}\ +\\\{({\text{concentration of }}{\mathrm {Na} {\vphantom {A}}_{\smash[{t}]{2}}\mathrm {SO} {\vphantom {A}}_{\smash[{t}]{4}}}{\text{ in M}})\times ({\text{number of }}{\mathrm {SO} {\vphantom {A}}_{\smash[{t}]{4}}{\vphantom {A}}^{2-}})\times ({\text{charge of }}{\mathrm {SO} {\vphantom {A}}_{\smash[{t}]{4}}{\vphantom {A}}^{2-}})^{2}\}\ +\\\{({\text{concentration of }}{\mathrm {KCl} }{\text{ in M}})\times ({\text{number of }}{\mathrm {K} {\vphantom {A}}^{+}})\times ({\text{charge of }}{\mathrm {K} {\vphantom {A}}^{+}})^{2}\}\ +\\\{({\text{concentration of }}{\mathrm {KCl} }{\text{ in M}})\times ({\text{number of }}{\mathrm {Cl} {\vphantom {A}}^{-}})\times ({\text{charge of }}{\mathrm {Cl} {\vphantom {A}}^{-}})^{2}\}\end{array}}\right]\\&={\tfrac {1}{2}}\times [\{0.050M\times 2\times (+1)^{2}\}+\{0.050M\times 1\times (-2)^{2}\}+\{0.020M\times 1\times (+1)^{2}\}+\{0.020M\times 1\times (-1)^{2}\}]\\&=0.17M\end{aligned}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/a16117298873a1e76082bbf2fbbbaa9f94c27df3)
