This problem is a beautiful symphony of multiple electrochemical concepts playing together. We are given a conductivity cell filled with a weak monobasic acid, and we need to find its limiting molar conductivity, Λm0. Let's break down the journey step-by-step.
Decoding the Conductivity Cell
Imagine the physical setup: a conductivity cell with two platinized platinum electrodes. The distance between them, l, is 120 cm, and their cross-sectional area, A, is 1 cm2. The conductance, G, is measured as 5×10−7 S.
First, we need to find the specific conductivity, κ. The formula connects conductance to the cell geometry:
Plugging in our values, we get:
κ=5×10−7×1120=6×10−5 S cm−1
This κ represents the conducting power of all the ions present in 1 cm3 of the solution.
Bridging Conductance to Molar Conductivity
Now that we have κ, we can calculate the molar conductivity, Λm, at the given concentration C=0.0015 M. Molar conductivity tells us the conducting power of all the ions produced by dissolving one mole of the electrolyte in the solution.
The formula is:
Substituting our values:
Λm=0.00156×10−5×1000=1.5×10−36×10−2=40 S cm2 mol−1
The pH Connection
Unlocking Dissociation
The problem also gives us the pH of the solution, which is 4. This is a crucial piece of the puzzle because it directly gives us the hydrogen ion concentration:
For a weak monobasic acid (let's call it HX), the dissociation can be represented as HX⇌H++X−. If the initial concentration is C and the degree of dissociation is α, the equilibrium concentration of H+ is Cα. Therefore:
We can rearrange this to find α:
We will leave α in this fractional form to avoid messy decimals and rounding errors in our final calculation.
The Grand Finale
Arrhenius Meets Kohlrausch
According to Arrhenius theory, the degree of dissociation α is the ratio of molar conductivity at a given concentration to the limiting molar conductivity at infinite dilution:
Rearranging this to solve for our target, Λm0:
Now, we substitute the values we've painstakingly calculated:
Flipping the denominator, we get:
Λm0=10−440×0.0015=10−40.06=600 S cm2 mol−1
The problem states that Λm0=Z×102 S cm2 mol−1. Comparing this with our result of 600, which is 6×102, we can clearly see that:
Z=6
This problem elegantly weaves together the physical geometry of a conductivity cell, the chemical equilibrium of weak acids, and the fundamental laws of electrochemistry.