Q.Suggest a way to determine the Λm0 value of water.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Molar Conductivity
From Resistance to Conductance: Flipping the Idea
You already know resistance (R) — it tells you how much a material opposes the flow of current. A high resistance means the wire fights the current; a low resistance means it lets current through easily.
Now flip that thought. Instead of asking "how much does it resist?", ask "how easily does it let current flow?" That's exactly what conductance measures.
Conductance (G) is the reciprocal of resistance:
G=R1
Unit: siemens (S) — named after Werner von Siemens. 1 S = 1 A/V (ampere per volt).
If a wire has R=10 Ω, its conductance is G=0.1 S. If R=0.5 Ω, G=2 S — it conducts twice as well.
Ohm's Law in Conductance Form
You know V=IR. Rearranging:
I=RV=GV
So current = conductance × voltage. A high-conductance material draws a large current for the same voltage — it's a "good conductor."
Now, Conductivity: The Material's Intrinsic Property
Resistance depends on two things: the material itself (its "resistivity" ρ) and the geometry (length L, cross-sectional area A):
R=ρAL
Conductance also depends on geometry. A thicker wire (larger A) or a shorter wire (smaller L) has higher conductance. To isolate the material's inherent ability to conduct, we define conductivity (σ):
σ=ρ1
And for a uniform wire:
G=σLA
Conductivity is the reciprocal of resistivity. It tells you how well the material itself conducts, independent of shape and size.
- Unit: siemens per metre (S/m).
- High σ → good conductor (copper: ≈5.8×107 S/m).
- Low σ → poor conductor / insulator (glass: ≈10−12 S/m).
Don't confuse conductance (property of a specific object, depends on geometry) with conductivity (property of the material, independent of geometry). A short thick copper wire has high conductance; a long thin copper wire has lower conductance — but both have the same conductivity.
The Big Picture in One Table
| Quantity | Symbol | Definition | Depends on | Unit |
|---|---|---|---|---|
| Resistance | R | V/I | Material + geometry | Ω |
| Resistivity | ρ | RA/L | Material only | Ω⋅m |
| Conductance | G | 1/R | Material + geometry | S |
| Conductivity | σ | 1/ρ | Material only | S/m |
Intuitive Analogy
Think of a water pipe:
- Resistance = how hard it is to push water through (narrow, long pipe).
- Conductance = how easily water flows (wide, short pipe). …
Why this formula?
Conductance and Conductivity: Why the Formulas Hold
Let's build this from first principles — understanding the why before the what.
1. The Core Idea: How Easily Does Current Flow?
Think of a conductor (like a copper wire). When you apply a voltage across it, electrons drift through the material. Two questions arise:
- How much current flows for a given voltage? → This is conductance (G).
- How well does the material itself allow current? → This is conductivity (σ).
The key distinction: Conductance depends on the size and shape of the object. Conductivity is an intrinsic property of the material.
2. Ohm's Law in Terms of Conductance
You know Ohm's law:
V=IR
But we can rewrite it as:
I=RV
Define conductance G as the reciprocal of resistance:
G=R1
So:
I=GV
Why this makes sense:
- A larger G means more current for the same voltage — the conductor "conducts" better.
- G has units of siemens (S) = A/V.
3. From Resistance to Conductivity: The Geometry Factor
Resistance of a uniform conductor depends on:
- Length L (longer → more resistance)
- Cross-sectional area A (thicker → less resistance)
- Material property ρ (resistivity)
The formula:
R=ρAL
Now, conductivity σ is the reciprocal of resistivity:
σ=ρ1
So:
R=σ1⋅AL
Why this form?
- If you double the length, electrons have to travel twice as far, colliding more → resistance doubles.
- If you double the area, there's twice as many "lanes" for electrons → resistance halves.
4. The Key Formula: Conductance in Terms of Conductivity
Since G=1/R, we get:
G=σLA
This is the central relationship. Let's see why it holds:
- σ tells you how well the material conducts (intrinsic).
- A/L tells you how the geometry amplifies or reduces that.
Intuition:
- A fat, short wire (A large, L small) has high conductance.
- A thin, long wire (A small, L large) has low conductance.
- A material with high σ (like copper) gives higher G than one with low σ (like iron), for the same shape.
5. Microscopic Derivation (Why σ Exists)
At the microscopic level, conductivity arises from electron motion:
σ=neμ
Where:
- n = number of free electrons per unit volume
- e = electron charge …
The key idea is that molar conductivity at infinite dilution (Λm0) is additive for ions (Kohlrausch’s law), but water is a weak electrolyte — it does not fully dissociate, so direct extrapolation fails.
Reasoning:
-
Water dissociates as H2O⇌H++OH−. Its Λm0 cannot be measured directly because the dissociation is incomplete and conductivity is very low.
-
Use Kohlrausch’s law: Λm0(H2O)=λ0(H+)+λ0(OH−).
-
Obtain λ0(H+) and λ0(OH−) from the Λm0 values of strong electrolytes containing these ions, e.g.:
- Λm0(HCl)=λ0(H+)+λ0(Cl−) …
The limiting molar conductivity Λm0 of water is determined indirectly using Kohlrausch’s law of independent migration of ions — by adding the Λm0 values of its constituent ions (HX+ and OHX−), which are obtained from the Λm0 of strong electrolytes like HCl, NaOH, and NaCl.
Why we can’t measure it directly
Water is a weak electrolyte. It dissociates only slightly:
HX2OHX++OHX−
If you try to measure its molar conductivity directly, the concentration of ions is tiny, and the conductivity is dominated by impurities. Extrapolating to infinite dilution is impossible because the dissociation itself changes with concentration. So we need an indirect route.
The key idea is Kohlrausch’s law: at infinite dilution, each ion contributes a fixed amount to the molar conductivity, independent of the other ion it came from. That means:
Λm0(electrolyte)=ν+λ+0+ν−λ−0
where ν are the number of ions per formula unit, and λ0 are the limiting ionic conductivities.
For water, we want:
Λm0(HX2O)=λ0(HX+)+λ0(OHX−)
So if we can find λ0(HX+) and λ0(OHX−) from known strong electrolytes, we’re done.
Step-by-step determination
1. Choose three strong electrolytes that contain HX+, OHX−, and a common counterion.
A classic set is:
- HCl — gives λ0(HX+)+λ0(ClX−)
- NaOH — gives λ0(NaX+)+λ0(OHX−)
- NaCl — gives λ0(NaX+)+λ0(ClX−)
All three are strong electrolytes, so their Λm0 values can be measured directly by extrapolating conductivity vs. c to zero concentration (Kohlrausch’s plot).
2. Write the three equations.
Let:
- A=Λm0(HCl)=λ0(HX+)+λ0(ClX−)
- B=Λm0(NaOH)=λ0(NaX+)+λ0(OHX−)
- C=Λm0(NaCl)=λ0(NaX+)+λ0(ClX−)
3. Combine them to isolate λ0(HX+)+λ0(OHX−).
Notice that:
A+B−C=[λ0(HX+)+λ0(ClX−)]+[λ0(NaX+)+λ0(OHX−)]−[λ0(NaX+)+λ0(ClX−)]
The λ0(NaX+) and λ0(ClX−) cancel, leaving:
A+B−C=λ0(HX+)+λ0(OHX−)
And that sum is exactly Λm0(HX2O). …
Method: Kohlrausch’s Law of Independent Migration of Ions
This method uses the principle that at infinite dilution, each ion contributes a fixed amount to the total molar conductivity, independent of the other ion present.
Why this is needed for water
Water is a weak electrolyte — it does not dissociate completely. So we cannot directly measure Λm0 for water by extrapolating a graph of Λm vs. c (as we do for strong electrolytes). Instead, we use Kohlrausch’s law.
Steps to determine Λm0 of water
Step 1: Identify the ions in water
Water dissociates as:
H2O⇌H++OH−
So, Λm0(water)=λH+0+λOH−0
Step 2: Use known limiting molar conductivities of strong electrolytes
From Kohlrausch’s law, we can write:
λH+0+λCl−0=Λm0(HCl)(measured experimentally)
λNa+0+λOH−0=Λm0(NaOH)(measured experimentally)
λNa+0+λCl−0=Λm0(NaCl)(measured experimentally)
Step 3: Combine to isolate the required sum
Add the first two equations and subtract the third:
(λH+0+λCl−0)+(λNa+0+λOH−0)−(λNa+0+λCl−0)=λH+0+λOH−0
Therefore: …
Here are the common mistakes students make when tackling this question, along with the conceptual fixes to avoid them.
1. Forgetting that Water is a Weak Electrolyte
The Mistake:
Students try to extrapolate Λm vs. C for water directly, as they would for a strong electrolyte like KCl.
Why it’s wrong:
Water is a very weak electrolyte (Kw=1.0×10−14). Its molar conductivity does not follow the linear Debye-Hückel-Onsager extrapolation. Plotting Λm vs C for water gives a curve that cannot be reliably extrapolated to zero concentration.
How to avoid:
Always check the nature of the electrolyte first. For weak electrolytes, you cannot find Λm0 by direct extrapolation. You must use Kohlrausch’s law of independent migration of ions.
2. Using the Wrong Formula for Kohlrausch’s Law
The Mistake:
Writing Λm0(H2O)=Λm0(H+)+Λm0(OH−) directly, without realising that water is not a salt.
Why it’s wrong:
Kohlrausch’s law applies to electrolytes that fully dissociate at infinite dilution. Water itself does not dissociate completely — but its ions (H⁺ and OH⁻) do have known limiting molar conductivities from other strong electrolytes.
How to avoid:
Use the indirect method:
Λm0(H2O)=Λm0(HCl)+Λm0(NaOH)−Λm0(NaCl)
This works because:
- Λm0(HCl)=λH+0+λCl−0
- Λm0(NaOH)=λNa+0+λOH−0
- Λm0(NaCl)=λNa+0+λCl−0
Subtracting cancels the spectator ions (Na+ and Cl−), leaving:
Λm0(H2O)=λH+0+λOH−0
3. Confusing Λm with Λm0
The Mistake:
Using the measured molar conductivity of water (which is extremely small, ~5.5×10−6S cm2mol−1) as if it were Λm0.
Why it’s wrong:
The measured Λm of water is not at infinite dilution — it’s the conductivity of pure water at its natural, very low dissociation. The limiting molar conductivity Λm0 is a hypothetical value for complete dissociation at infinite dilution, which is much larger (~550S cm2mol−1).
How to avoid:
Remember: Λm0 is not the conductivity of the pure substance — it’s the conductivity if it were fully dissociated at infinite dilution. For water, you must calculate it via Kohlrausch’s law, never measure it directly.
4. Forgetting Units and Magnitude
The Mistake:
Writing the final answer without units, or giving a value that is orders of magnitude off (e.g., writing 55S cm2mol−1 instead of 550).
Why it’s wrong: …
- KEAM 2026Set eng-2026-04214 marksMCQQ.The molar conductivity of a weak mono basic acid, HA at 298 K is 70 Scm2mol−1. What is the percentage ionisation of HA at 298 K? [At infinite dilution λH+=340 Scm2mol−1 and λA−=80 Scm2mol−1] (A) 8.35 % (B) 16.7 % (C) 20 % (D) 32.5 % (E) 15.3 %
›Reveal solutionSolution
α=Λm/Λm∘=70/420=16.7.
Limiting molar conductivity of HA:
Λm∘=λH+∘+λA−∘=340+80=420,Scm2mol−1.
Degree of ionisation: …
- KEAM 2026Set pha-2026-0418F4 marksMCQQ.The limiting molar conductance for aqueous solution of CaCl2 at 298K is 271.6 S cm2 mol−1. If the limiting ionic conductance of Ca2+ ion at the same temperature is 119 S cm2 mol−1 what is the limiting ionic conductance of Cl− ion? (A) 152.6 S cm2 mol−1 (B) 76.3 S cm2 mol−1 (C) 135.8 S cm2 mol−1 (D) 228.7 S cm2 mol−1 (E) 114.35 S cm2 mol−1
›Reveal solutionSolution
Kohlrausch: Λm∘(CaCl2)=λ∘(Ca2+)+2λ∘(Cl−).
271.6=119+2λ∘(Cl−) …
- KEAM 2025Set eng-2025-04254 marksMCQQ.The molar conductivity (Λm) acetic acid is 78.1 S cm2 mol−1. Its degree of dissociation (α) is (Λm0) for acetic acid = 390.5 S cm2 mol−1 (A) 0.12 (B) 0.40 (C) 0.02 (D) 0.20 (E) 0.04
›Reveal solutionSolution
Degree of dissociation of a weak electrolyte α=Λm0Λm=390.578.1=0.20.
For a weak electrolyte such as acetic acid, the degree of dissociation is the ratio of the molar conductivity at the given concentration to the molar conductivity at infinite dilution:
α=Λm0Λm …
- KEAM 2025Set pha-2025-0424F4 marksMCQQ.The ion with the highest limiting molar conductance at 298 K is (A) H+ (B) Na+ (C) K+ (D) Ca2+ (E) Mg2+
›Reveal solutionSolution
The proton conducts by the Grotthuss (hopping) mechanism, giving H+ by far the largest limiting molar conductivity (≈350 S cm2 mol−1).
Limiting molar conductivities at 298 K (in S cm2 mol−1) are roughly:
- H+≈349.8
- K+≈73.5
- Ca2+≈119 (but per mole of charge ≈59.5)
- Na+≈50.1
- Mg2+≈106 (per mole of charge ≈53) …
- KEAM 2024Set eng-2024-06074 marksMCQQ.The conductivity of 0.02 mol L−1 KCl solution is 0.248 S m−1. Its molar conductivity is (A) 20 S m2 mol−1 (B) 1.24×10−3 S m2 mol−1 (C) 1.24×10−4 S m2 mol−1 (D) 2.48×10−2 S m2 mol−1 (E) 1.24×10−2 S m2 mol−1
›Reveal solutionSolution
Molar conductivity Λm=κ/c. With κ=0.248 S m−1 and c=0.02 mol L−1=20 mol m−3, Λm=1.24×10−2 S m2 mol−1.
Molar conductivity is related to conductivity by
Λm=cκ.
Using SI units, the concentration must be in mol m−3:
c=0.02 mol L−1=0.02×1000=20 mol m−3. …
- KEAM 2024Set eng-2024-06084 marksMCQQ.The limiting molar conductances of NaCl, HCl and CH3COONa at 300 K are 126.4, 425.9 and 91.0 S cm2 mol−1 respectively. The limiting molar conductance of acetic acid at 300 K is (A) 266 S cm2 mol−1 (B) 390.5 S cm2 mol−1 (C) 461.3 S cm2 mol−1 (D) 208 S cm2 mol−1 (E) 108 S cm2 mol−1
›Reveal solutionSolution
Kohlrausch's law of independent ion migration lets the limiting molar conductance of acetic acid be built from those of sodium acetate, HCl and NaCl: 91.0+425.9−126.4=390.5 S cm2 mol−1.
Acetic acid dissociates into CH3COO− and H+. Combining known limiting conductances:
Λm∘(CH3COOH)=Λm∘(CH3COONa)+Λm∘(HCl)−Λm∘(NaCl). …
- KEAM 2021Set eng-2021-P1-A14 marksMCQQ.The SI unit of molar conductivity is (A) S m3 mol−1 (B) S m mol−1 (C) S m mol−2 (D) S m2 mol−1 (E) S m2 mol−2
›Reveal solutionSolution
The SI unit of molar conductivity is S m2 mol−1.
Concept and Intuition
Molar conductivity is the conductivity per unit molar concentration, defined as Λm=κ/c. Its unit follows directly from the units of conductivity and concentration in SI.
Step-by-Step Solution
- Conductivity κ has SI unit S m−1.
- Concentration c in SI is mol m−3. …
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