Q3(e). Debye–Hückel limiting law for an ion i
Write down Debye-Huckel limiting equation for i^(th) type of ionic species in a salt solution with symbolic significances and units.
Answer in brief
γᵢ=-A zᵢ²√I, with I=12Σⱼ bⱼzⱼ²; A=0.509 (mol kg⁻¹)^(-1/2) for water at 25°C; γᵢ and zᵢ have no units.
Key points
- ₁₀γᵢ=-A zᵢ² √I
- γᵢ: activity coefficient of ion i, defined by aᵢ=γᵢ bᵢ/b°; dimensionless. γᵢ→1 as I→0.
- charge number of the ion (+1 for Na⁺, -2 for SO₄²⁻); dimensionless. It enters as zᵢ², so the sign does not matter.
- ionic strength, I=12Σⱼ bⱼzⱼ², summed over all ions in the solution; unit mol kg⁻¹ (molality bⱼ). In dilute water molar concentrations may be used.
The full model answer
Written out in full, as it should go in the answer booklet. The solution page with its diagrams follows it.
The equation and its symbols
- ₁₀γᵢ=-A zᵢ² √I
- γᵢ: activity coefficient of ion i, defined by aᵢ=γᵢ bᵢ/b°; dimensionless. γᵢ→1 as I→0.
- zᵢ: charge number of the ion (+1 for Na⁺, -2 for SO₄²⁻); dimensionless. It enters as zᵢ², so the sign does not matter.
- I: ionic strength, I=12Σⱼ bⱼzⱼ², summed over all ions in the solution; unit mol kg⁻¹ (molality bⱼ). In dilute water molar concentrations may be used.
- A: a constant for the solvent and temperature, A=1.825×10⁶(εᵣT)^(3/2); for water at 25°C A=0.509 (mol kg⁻¹)^(-1/2). It becomes dimensionless when I is written as I/b°.
Meaning and use
- Origin: each ion is surrounded by an ionic atmosphere of net opposite charge; the atmosphere lowers the energy (chemical potential) of the ion, so γᵢ<1. The effect grows with charge (z²) and with I (thinner atmosphere).
- Mean coefficient, the measurable quantity: γ_±=-A |z₊z₋| √I
- Example, ZnCl₂ at 0.0050 mol kg⁻¹: I=12(0.0050×4+0.010×1)=0.015 mol kg⁻¹; γ(Zn²⁺)=0.563, γ(Cl⁻)=0.866, γ_±=0.750.
- Limits: valid only for very dilute solutions (point ions). At higher I the extended law γ_±=-A|z₊z₋|√I/(1+B√I) is used.
Application. the law corrects measured cell potentials and equilibrium constants to activities (for example, the standard potential of the calomel electrode is found by extrapolating to √I=0), and it explains the salt effect on the solubility of sparingly soluble salts.
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