# Molar conductivity

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{{Short description|Conductivity per molar concentration of electrolyte}}
The '''molar conductivity''' of an [electrolyte](/source/electrolyte) solution is defined as its [conductivity](/source/Conductivity_(electrolytic)) divided by its molar concentration:<ref>''The best test preparation for the GRE Graduate Record Examination Chemistry Test''. Published by the Research and Education Association, 2000, {{ISBN|0-87891-600-8}}. p.&nbsp;149.</ref><ref name=Atk762>{{cite book |last1=Atkins |first1=P. W. |authorlink1=Peter Atkins|last2=de Paula |first2=J. |date=2006 |title=Physical Chemistry |url=https://archive.org/details/atkinsphysicalch00atki |url-access=limited |edition=8th |isbn=0198700725 |publisher=Oxford University Press |page=[https://archive.org/details/atkinsphysicalch00atki/page/n794 762]}}</ref>
: <math>\Lambda_\text{m} = \frac{\kappa}{c},</math>
where
: ''κ'' is the measured conductivity (formerly known as specific conductance),<ref>[http://goldbook.iupac.org/C01245.html Conductivity], IUPAC Gold Book.</ref>
: ''c'' is the [molar concentration](/source/molar_concentration) of the electrolyte.

The [SI unit](/source/International_System_of_Units) of molar conductivity is [siemens](/source/Siemens_(unit)) metres squared per mole (S&nbsp;m<sup>2</sup>&nbsp;mol<sup>−1</sup>).<ref name=Atk762/> However, values are often quoted in S&nbsp;cm<sup>2</sup>&nbsp;mol<sup>−1</sup>.<ref name=LM/> In these last units, the value of Λ<sub>m</sub> may be understood as the [conductance](/source/Electrical_resistance_and_conductance) of a volume of solution between parallel plate electrodes one centimeter apart and of sufficient area so that the solution contains exactly one mole of electrolyte.<ref>[Laidler K. J.](/source/Keith_J._Laidler) and Meiser J. H., ''Physical Chemistry'' (Benjamin/Cummings 1982) p.&nbsp;256. {{ISBN|0-8053-5682-7}}.</ref>

==Variation of molar conductivity with dilution==

There are two types of electrolytes: strong and weak. [Strong electrolyte](/source/Strong_electrolyte)s usually undergo complete ionization, and therefore they have higher conductivity than weak electrolytes, which undergo only partial ionization. For [strong electrolyte](/source/strong_electrolyte)s, such as [salts](/source/salt_(chemistry)), [strong acid](/source/strong_acid)s and [strong base](/source/strong_base)s, the molar conductivity depends only ''weakly'' on concentration. On dilution there is a regular increase in the molar conductivity of strong electrolyte, due to the decrease in solute–solute interaction. Based on experimental data [Friedrich Kohlrausch](/source/Friedrich_Kohlrausch_(physicist)) (around the year 1900) proposed the non-linear law for strong electrolytes:

: <math>\Lambda_\text{m} =\Lambda_\text{m}^\circ - K\sqrt{c} = \alpha f_\lambda \Lambda_\text{m}^\circ,</math> 
where 
: Λ{{su|b=m|p=∘}} is the molar conductivity at infinite dilution (or ''limiting molar conductivity''), which can be determined by extrapolation of Λ<sub>m</sub> as a function of {{sqrt|''c''}},
: ''K'' is the Kohlrausch coefficient, which depends mainly on the [stoichiometry](/source/stoichiometry) of the specific salt in solution,
: ''α'' is the dissociation degree even for strong concentrated electrolytes,
: ''f<sub>λ</sub>'' is the lambda factor for concentrated solutions.

This law is valid for low electrolyte concentrations only; it fits into the [Debye–Hückel–Onsager equation](/source/Debye%E2%80%93H%C3%BCckel_theory).<ref>{{cite book |last=Atkins |first=P. W. |title=The Elements of Physical Chemistry |publisher=Oxford University Press |year=2001 |isbn=0-19-879290-5}}</ref>

For weak electrolytes (i.e. incompletely dissociated electrolytes), however, the molar conductivity ''strongly'' depends on concentration: The more dilute a solution, the greater its ''molar'' conductivity, due to increased [ionic dissociation](/source/ionic_dissociation). For example, acetic acid has a higher molar conductivity in dilute aqueous acetic acid than in concentrated acetic acid.

== Kohlrausch's law of independent migration of ions==

[Friedrich Kohlrausch](/source/Friedrich_Kohlrausch_(physicist)) in 1875–1879 established that to a high accuracy in dilute solutions, molar conductivity can be decomposed into contributions of the individual ions. This is known as '''Kohlrausch's law of independent ionic migration'''.<ref>Castellan, G. W. ''Physical Chemistry''. Benjamin/Cummings, 1983.</ref>
For any electrolyte A<sub>''x''</sub>B<sub>''y''</sub>, the limiting molar conductivity is expressed as ''x'' times the limiting molar conductivity of A<sup>''y''+</sup> and ''y'' times the limiting molar conductivity of B<sup>''x''−</sup>.

: <math>\Lambda_\text{m}^\circ = \sum_i \nu_i \lambda_i,</math>
where:
: ''λ<sub>i</sub>'' is the limiting molar ionic conductivity of ion ''i'',
: ''ν<sub>i</sub>'' is the number of ions ''i'' in the [formula unit](/source/formula_unit) of the electrolyte (e.g. 2 and 1 for [Na<sup>+</sup>](/source/sodium_ion) and [{{chem|SO|4|2−}}](/source/sulfate) in [Na<sub>2</sub>SO<sub>4</sub>](/source/sodium_sulfate)).

Kohlrausch's evidence for this law was that the limiting molar conductivities of two electrolytes with two different cations and a common anion differ by an amount which is independent of the nature of the anion. For example, {{nowrap|Λ<sub>0</sub>(KX) − Λ<sub>0</sub>(NaX)}} = {{nowrap|23.4 S cm<sup>2</sup> mol<sup>−1</sup>}} for X = [Cl<sup>−</sup>](/source/chloride), [I<sup>−</sup>](/source/iodide) and {{sfrac|1|2}}&nbsp;{{chem|SO|4|2−}}. This difference is ascribed to a difference in ionic conductivities between [K<sup>+</sup>](/source/potassium_ion) and Na<sup>+</sup>. Similar regularities are found for two electrolytes with a common anion and two cations.<ref>[Laidler K. J.](/source/Keith_J._Laidler) and Meiser J. H., ''Physical Chemistry'' (Benjamin/Cummings 1982) p. 273. {{ISBN|0-8053-5682-7}}.</ref>

==Molar ionic conductivity==
The molar ionic conductivity of each ionic species is proportional to its [electrical mobility](/source/electrical_mobility) (''μ''), or [drift velocity](/source/drift_velocity) per unit [electric field](/source/electric_field), according to the equation
: <math>\lambda = z \mu F,</math>
where ''z'' is the ionic charge, and ''F'' is the [Faraday constant](/source/Faraday_constant).<ref>{{cite book |last1=Atkins |first1=P. W. |authorlink1=Peter Atkins|last2=de Paula |first2=J. |date=2006 |title=Physical Chemistry |url=https://archive.org/details/atkinsphysicalch00atki |url-access=limited |edition=8th |isbn=0198700725 |publisher=Oxford University Press |page=[https://archive.org/details/atkinsphysicalch00atki/page/n798 766]}}</ref>

The limiting molar conductivity of a weak electrolyte cannot be determined reliably by extrapolation. Instead it can be expressed as a sum of ionic contributions, which can be evaluated from the limiting molar conductivities of strong electrolytes containing the same ions. For aqueous [acetic acid](/source/acetic_acid) as an example,<ref name=LM/> 
: <math chem>\begin{aligned}
 \Lambda_\text{m}^\circ(\ce{CH3COOH}) &= \lambda(\ce{CH3COO-}) + \lambda(\ce{H+}) \\
  &= \Lambda_\text{m}^\circ(\ce{CH3COONa}) + \Lambda_\text{m}^\circ(\ce{HCl}) - \Lambda_\text{m}^\circ(\ce{NaCl}).
\end{aligned}</math>
 
Values for each ion may be determined using measured [ion transport number](/source/ion_transport_number)s. For the cation:
: <math>\lambda^+ = t_+ \cdot \frac{\Lambda_0}{\nu^+},</math>
and for the anion:
: <math>\lambda^- = t_- \cdot \frac{\Lambda_0}{\nu^-}.</math>

Most monovalent ions in water have limiting molar ionic conductivities in the range of {{nowrap|40–80 S cm<sup>2</sup> mol<sup>−1</sup>}}. For example:<ref name=LM>[Laidler K. J.](/source/Keith_J._Laidler) and Meiser J. H., ''Physical Chemistry'' (Benjamin/Cummings 1982) p. 281–283. {{ISBN|0-8053-5682-7}}.</ref>

{|
|
{| class="wikitable"
! Cation !! ''λ'', {{nowrap|S cm<sup>2</sup> mol<sup>−1</sup>}}
|-
| [Li<sup>+</sup>](/source/lithium) || 38.6
|-
| [Na<sup>+</sup>](/source/sodium) || 50.1
|-
| [K<sup>+</sup>](/source/potassium) || 73.5
|-
| [Ag<sup>+</sup>](/source/silver) || 61.9
|}
|
{| class="wikitable"
! Anion !! ''λ'', {{nowrap|S cm<sup>2</sup> mol<sup>−1</sup>}}
|-
| [F<sup>−</sup>](/source/fluoride) || 55.4
|-
| [Cl<sup>−</sup>](/source/chloride) || 76.4
|-
| [Br<sup>−</sup>](/source/bromide) || 78.1
|-
| [CH<sub>3</sub>COO<sup>−</sup>](/source/acetate) || 40.9
|}
|}

The order of the values for alkali metals is surprising, since it shows that the smallest cation Li<sup>+</sup> moves more slowly in a given electric field than Na<sup>+</sup>, which in turn moves more slowly than K<sup>+</sup>. This occurs because of the effect of [solvation](/source/solvation) of water molecules: the smaller Li<sup>+</sup> binds most strongly to about four water molecules so that the moving cation species is effectively {{chem|Li(H|2|O)|4|+}}. The solvation is weaker for Na<sup>+</sup> and still weaker for K<sup>+</sup>.<ref name=LM/> The increase in halogen ion mobility from F<sup>−</sup> to Cl<sup>−</sup> to Br<sup>−</sup> is also due to decreasing solvation.

Exceptionally high values are found for [H<sup>+</sup>](/source/hydrogen_ion) ({{nowrap|349.8 S cm<sup>2</sup> mol<sup>−1</sup>}}) and [OH<sup>−</sup>](/source/hydroxide) ({{nowrap|198.6 S cm<sup>2</sup> mol<sup>−1</sup>}}), which are explained by the [Grotthuss proton-hopping mechanism](/source/Grotthuss_mechanism) for the movement of these ions.<ref name=LM/> The H<sup>+</sup> also has a larger conductivity than other ions in [alcohol](/source/Alcohol_(chemistry))s, which have a [hydroxyl](/source/hydroxyl) group, but behaves more normally in other solvents, including liquid [ammonia](/source/ammonia) and [nitrobenzene](/source/nitrobenzene).<ref name=LM/>

For multivalent ions, it is usual to consider the conductivity divided by the [equivalent ion concentration](/source/equivalent_concentration) in terms of equivalents per litre, where 1 equivalent is the quantity of ions that have the same amount of electric charge as 1&nbsp;mol of a monovalent ion: {{sfrac|1|2}}&nbsp;mol Ca<sup>2+</sup>, {{sfrac|1|2}}&nbsp;mol {{chem|SO|4|2−}}, {{sfrac|1|3}}&nbsp;mol Al<sup>3+</sup>, {{sfrac|1|4}}&nbsp;mol {{chem|Fe(CN)|6|4−}}, etc. This quotient can be called the ''equivalent conductivity'', although [IUPAC](/source/IUPAC) has recommended that use of this term be discontinued and the term molar conductivity be used for the values of conductivity divided by equivalent concentration.<ref>Yung Chi Wu and Paula A. Berezansky, [http://nvlpubs.nist.gov/nistpubs/jres/100/5/j15wu.pdf Low Electrolytic Conductivity Standards], J. Res. Natl. Inst. Stand. Technol. 100, 521 (1995).</ref> If this convention is used, then the values are in the same range as monovalent ions, e.g. {{nowrap|59.5 S cm<sup>2</sup> mol<sup>−1</sup>}} for {{sfrac|1|2}}&nbsp;Ca<sup>2+</sup> and {{nowrap|80.0 S cm<sup>2</sup> mol<sup>−1</sup>}} for {{sfrac|1|2}}&nbsp;{{chem|SO|4|2−}}.<ref name=LM/>

From the ionic molar conductivities of cations and anions, effective ionic radii can be calculated using the concept of [Stokes radius](/source/Stokes_radius). The values obtained for an ionic radius in solution calculated this way can be quite different from the [ionic radius](/source/ionic_radius) for the same ion in crystals, due to the effect of hydration in solution.

== Applications ==
[Ostwald's law of dilution](/source/Law_of_dilution), which gives the dissociation constant of a weak electrolyte as a function of concentration, can be written in terms of molar conductivity. Thus, the [p''K''<sub>a</sub>](/source/pKa) values of acids can be calculated by measuring the molar conductivity and extrapolating to zero concentration. Namely, p''K''<sub>a</sub> = p({{sfrac|''K''|1&nbsp;mol/L}}) at the zero-concentration limit, where ''K'' is the dissociation constant from Ostwald's law.

==References==
{{reflist}}

Category:Electrochemical concepts
Category:Physical chemistry
Category:Molar quantities

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Adapted from the Wikipedia article [Molar conductivity](https://en.wikipedia.org/wiki/Molar_conductivity) by Wikipedia contributors ([contributor history](https://en.wikipedia.org/wiki/Molar_conductivity?action=history)). Available under [Creative Commons Attribution-ShareAlike 4.0 International](https://creativecommons.org/licenses/by-sa/4.0/). Changes may have been made.
