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Example · Example 21

Q.Given the limiting molar conductivities Λm0(HCl)=425.9 S cm2 mol−1\Lambda_m^{0}(\text{HCl}) = 425.9\ \text{S cm}^2\ \text{mol}^{-1}, Λm0(CH3COONa)=91.0 S cm2 mol−1\Lambda_m^{0}(\text{CH}_3\text{COONa}) = 91.0\ \text{S cm}^2\ \text{mol}^{-1} and Λm0(NaCl)=126.4 S cm2 mol−1\Lambda_m^{0}(\text{NaCl}) = 126.4\ \text{S cm}^2\ \text{mol}^{-1}, use Kohlrausch's law to calculate the limiting molar conductivity of acetic acid, Λm0(CH3COOH)\Lambda_m^{0}(\text{CH}_3\text{COOH}).

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Kohlrausch's law of independent migration of ions states that at infinite dilution, each ion contributes its own fixed limiting molar ionic conductivity, λ0\lambda^{0}, independently of the other ion it is paired with; so Λm0(CH3COOH)=λ0(CH3COO−)+λ0(H+)\Lambda_m^{0}(\text{CH}_3\text{COOH}) = \lambda^{0}(\text{CH}_3\text{COO}^{-}) + \lambda^{0}(\text{H}^{+}). These individual ionic values are not given directly, but they can be combined from strong-electrolyte data (all fully dissociated, so their Λm0\Lambda_m^{0} can be measured directly by extrapolation) using simple ionic algebra: λ0(CH3COO−)+λ0(Na+)=Λm0(CH3COONa)\lambda^{0}(\text{CH}_3\text{COO}^{-}) + \lambda^{0}(\text{Na}^{+}) = \Lambda_m^{0}(\text{CH}_3\text{COONa}), and λ0(H+)+λ0(Cl−)=Λm0(HCl)\lambda^{0}(\text{H}^{+}) + \lambda^{0}(\text{Cl}^{-}) = \Lambda_m^{0}(\text{HCl}); adding these two gives λ0(CH3COO−)+λ0(H+)+[λ0(Na+)+λ0(Cl−)]\lambda^{0}(\text{CH}_3\text{COO}^{-}) + \lambda^{0}(\text{H}^{+}) + [\lambda^{0}(\text{Na}^{+}) + \lambda^{0}(\text{Cl}^{-})], and the bracketed term is exactly Λm0(NaCl)\Lambda_m^{0}(\text{NaCl}), so subtracting it isolates the target sum: $\Lambda_m^{0}(\text{CH}_3\text{COOH}) = \Lambda_m^{0}(\text{CH}_3\text{COONa}) + \Lambda_m^{0}(\text{HC …

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