Editing Law of dilution

{{Short description|Law of Ostwald for dissociation of electrolytes}}
[[Wilhelm Ostwald]]’s '''dilution law''' is a relationship proposed in 1888<ref>{{cite book |last1=Laidler |first1=Keith J. |last2=Meiser |first2=John H. |date=1982 |title=Physical Chemistry |page=259 |isbn=978-0-8053-5682-3 |publisher=Benjamin/Cummings }}</ref> between the [[dissociation constant]] ''{{math|K<sub>d</sub>}}'' and the [[Dissociation (chemistry)#Dissociation degree|degree of dissociation]] ''{{math|α}}'' of a weak [[electrolyte]]. The law takes the form<ref>{{cite book|title=The Development of Chemical Principles|publisher=Courier Corporation|last1=Langford|first1=von Cooper Harold|last2=Beebe|first2=Ralph Alonzo|isbn=978-0486683591|page=[https://archive.org/details/developmentofche00lang/page/135 135]|url=https://archive.org/details/developmentofche00lang|url-access=registration|quote=law of dilution ostwald.|date=1995-01-01}}</ref>

:<math chem>K_d = \cfrac{\ce{[A+] [B^{-}]}}{\ce{[AB]}} = \frac{\alpha^2}{1-\alpha} \cdot c_0 </math>

Where the square brackets denote concentration, and {{math|''c''<sub>0</sub>}} is the total concentration of electrolyte.

Using <math>\alpha=\Lambda_c/\Lambda_0</math>, where <math>\Lambda_c</math> is the [[molar conductivity]] at concentration c and <math>\Lambda_0</math> is the limiting value of molar conductivity [[extrapolated]] to zero concentration or infinite dilution, this results in the following relation:

:<math>K_d = \cfrac{\Lambda_c^2}{(\Lambda_0 - \Lambda_c)\Lambda_0} \cdot c_0 </math>

==Derivation==

Consider a binary electrolyte AB which dissociates reversibly into A<sup>+</sup> and B<sup>−</sup> ions. Ostwald noted that  the [[law of mass action]] can be applied to such systems as dissociating electrolytes. The equilibrium state is represented by the equation:

:<chem>AB <=> {A+} + B^-</chem>

If ''{{math|α}}'' is the fraction of dissociated electrolyte, then ''{{math|αc<sub>0</sub>}}'' is the concentration of each ionic species. {{math|(1 - ''α'')}} must, therefore be the fraction of ''undissociated'' electrolyte, and {{math|(1 - ''α'')''c<sub>0</sub>''}} the concentration of same. The dissociation constant may therefore be given as

:<math chem>K_d = \cfrac{\ce{[A+ ] [B^- ]}}{\ce{[AB]}} = \cfrac{(\alpha c_0 )(\alpha c_0 )}{(1-\alpha) c_0 } = \cfrac{\alpha^2}{1-\alpha} \cdot c_0 </math>

For very weak electrolytes {{tmath|\alpha \ll 1}}, implying that {{math|(1 - ''α'') ≈ 1}}.

:<math>K_d = \frac{\alpha^2}{1-\alpha} \cdot c_0 \approx \alpha^2 c_0 </math>

This gives the following results;

:<math>\alpha = \sqrt{\cfrac{K_d }{c_0 }} </math>

Thus, the degree of dissociation of a weak electrolyte is proportional to the inverse square root of the concentration, or the square root of the dilution. The concentration of any one ionic species is given by the root of the product of the dissociation constant and the concentration of the electrolyte.

:<math chem>\ce{[A+ ]} = \ce{[B^- ]} = \alpha c_0 = \sqrt{K_d c_0 } </math>

==Limitations==

The Ostwald law of dilution provides a satisfactory description of the concentration dependence of the conductivity of weak electrolytes like CH<sub>3</sub>COOH and NH<sub>4</sub>OH.<ref>{{cite book |last=Laidler |first=Keith J. |date=1978 |title=Physical chemistry with biological applications |publisher=Benjamin/Cummings |page=266 |isbn=978-0-8053-5680-9 |author-link=Keith J. Laidler }}</ref> <ref>{{cite book |last1=Laidler |first1=Keith J. |last2=Meiser |first2=John H.|date=1982 |title=Physical chemistry |publisher=Benjamin/Cummings |page=260 |isbn=978-0-8053-5682-3 }}</ref> The variation of molar conductivity is essentially due to the incomplete dissociation of weak electrolytes into ions. 

For strong electrolytes, however, [[Gilbert N. Lewis|Lewis]] and [[Merle Randall|Randall]] recognized that the law fails badly since the supposed equilibrium constant is actually far from constant.<ref>{{cite journal |last1=Lewis |first1=Gilbert N. |last2=Randall |first2=Merle |title=The Activity Coefficient of Strong Electrolytes.1 |date=1921 |journal=Journal of the American Chemical Society |volume=43 |issue=5 |pages=1112–1154 |doi=10.1021/ja01438a014 |url=https://zenodo.org/record/2306457 }}</ref> This is because the dissociation of strong electrolytes into ions is essentially complete below a concentration threshold value. The decrease in molar conductivity as a function of concentration is actually due to attraction between ions of opposite charge as expressed in the [[Debye-Hückel-Onsager equation]] and later revisions.

Even for weak electrolytes the equation is not exact. [[Chemical thermodynamics]] shows that the true equilibrium constant is a ratio of [[thermodynamic activity|thermodynamic activities]], and that each concentration must be multiplied by an [[activity coefficient]]. This correction is important for ionic solutions due to the strong forces between ionic charges. An estimate of their values is given by the [[Debye–Hückel theory]] at low concentrations.

==See also==
*[[Autosolvolysis]]
*[[Osmotic coefficient]]
*[[Activity coefficient]]
*[[Ion transport number]]
*[[Ion association]]
*[[Molar conductivity]]
{{DEFAULTSORT:Law Of Dilution}}
[[Category:Physical chemistry]]
[[Category:Enzyme kinetics]]

==References==
{{reflist}}