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Chemistry · Ch 7 — Electrochemistry

Molar Conductivity and Its Variation with Concentration

7.11

Molar Conductivity and Its Variation with Concentration

Specific conductivity, κ\kappa, describes how well a given volume of solution conducts, but it mixes together two separate effects: how many ions are actually present, and how well each individual ion conducts. To separate out the conducting contribution of the electrolyte itself, independent of how concentrated the solution happens to be, chemists define molar conductivity, Λm\Lambda_m, as the conductivity contributed by exactly one mole of dissolved electrolyte: Λm=1000 κC\Lambda_m = \frac{1000\,\kappa}{C} where CC is the molar concentration in mol L−1\text{mol L}^{-1} and the factor of 10001000 converts κ\kappa (naturally expressed per cm3\text{cm}^3) onto the same per-litre basis as CC. Its unit works out to S cm2 mol−1\text{S cm}^2\ \text{mol}^{-1}.

Unlike κ\kappa, which falls on dilution, Λm\Lambda_m rises as a solution is diluted — for two distinct physical reasons that apply to different degrees for different electrolytes. First, in every electrolyte solution, ions in close proximity exert a retarding electrostatic drag on one another's motion (sometimes pictured as each ion dragging a loosely-bound 'ionic atmosphere' of opposite charge behind it); diluting the solution increases the average distance between ions, weakening this drag and increasing each ion's mobility. Second, for a weak electrolyte specifically, dilution also shifts its dissociation equilibrium further toward the ionized form (by Le Chatelier's principle, since dissociation increases the total number of particles, which is favoured at lower concentration), genuinely increasing the number of ions present per mole of electrolyte.

A strong electrolyte, such as KCl\text{KCl} or NaCl\text{NaCl}, is essentially completely dissociated at every concentration normally studied, so only the mobility effect operates; its Λm\Lambda_m therefore rises gradually and predictably on dilution, following the Debye-Huckel-Onsager relation Λm=Λm0−AC\Lambda_m = \Lambda_m^{0} - A\sqrt{C} (a straight line when Λm\Lambda_m is plotted against C\sqrt{C}), and its limiting value Λm0\Lambda_m^{0} (molar conductivity at infinite dilution, where inter-ionic effects vanish entirely) can be obtained simply by extrapolating this line to C=0C=0. …