Q.Conductivity κ, is equal to ____________. (Two or more than two options may be correct.)
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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 Molar Conductivity — but the question is about conductivity κ, not molar conductivity. Conductivity is the reciprocal of resistivity, and resistivity is RlA.
Step 1: From Ohm’s law, resistance R=ρAl, so resistivity ρ=RlA.
Step 2: Conductivity κ=ρ1=R1Al. This matches option (i).
Step 3: The cell constant G∗=Al, so κ=RG∗. This matches option (ii). …
Conductivity κ is the reciprocal of resistivity, so it equals R1⋅Al and also RG∗ (where G∗ is the cell constant). Options (i) and (ii) are correct; (iii) and (iv) are not.
The key here is to remember what conductivity actually means physically. Conductivity (κ) is a measure of how easily a solution conducts electricity — it’s the conductance of a 1 cm cube of the solution. That’s the intuitive picture: imagine a cube of the electrolyte, 1 cm on each side; the conductance you measure across opposite faces is the conductivity.
Now, how do we get there from measurable quantities? In the lab, you measure resistance R of a solution placed in a cell with two electrodes of area A separated by distance l. The relationship between resistance and the geometry is:
R=ρAl
where ρ is resistivity. Since conductivity is the reciprocal of resistivity:
κ=ρ1=R1⋅Al
That’s option (i) directly.
But there’s a practical twist. In a real conductivity cell, you rarely know l and A separately — instead, you calibrate the cell and determine its cell constant G∗=Al. So the same formula becomes:
κ=RG∗
That’s option (ii).
Now let’s check the others:
-
Option (i): R1Al — This is exactly the definition from R=ρAl and κ=1/ρ. So this is correct.
-
Option (ii): RG∗ — Since G∗=l/A, this is just a repackaging of (i). Also correct. …
Method: Direct Formula Application for Conductivity (κ)
This method uses the definition of conductivity in terms of resistance and cell geometry.
Step 1: Recall the basic relation
Conductivity κ is the reciprocal of resistivity (ρ):
κ=ρ1
Step 2: Express resistivity in terms of resistance and cell dimensions
Resistivity is given by:
ρ=R⋅lA
where:
- R = resistance
- A = cross-sectional area of electrodes
- l = distance between electrodes
Step 3: Substitute to get conductivity
κ=R⋅lA1=R1⋅Al
This matches option (i).
Step 4: Introduce cell constant
The term Al is called the cell constant, G∗:
G∗=Al
Thus:
κ=RG∗
This matches option (ii). …
The Core Concept First
Conductivity (κ) is the ability of a solution to conduct electricity. It is defined as:
κ=ρ1
where ρ is resistivity.
From the resistance formula:
R=ρAl
we get:
κ=R1⋅Al
Also, the cell constant G∗=Al, so:
κ=RG∗
Correct Answer
✓ Options (i) and (ii) are correct.
- (i) R1Al — direct formula.
- (ii) RG∗ — using cell constant.
✗ (iii) Λm is molar conductivity, not conductivity.
✗ (iv) Al is the cell constant, not conductivity.
Common Mistakes & How to Avoid Them
Mistake 1: Confusing κ with Λm
- Why it happens: Both are measures of conductance, and symbols look similar.
- How to avoid: Remember:
- κ = conductivity (S cm⁻¹ or S m⁻¹)
- Λm = molar conductivity (S cm² mol⁻¹ or S m² mol⁻¹)
- Relation: Λm=cκ (where c is concentration)
Mistake 2: Thinking Al alone is conductivity
- Why it happens: Students see l/A in the formula and forget the 1/R factor.
- How to avoid: Always write the full definition:
κ=R1⋅Al
The l/A part is just the cell constant, not conductivity.
Mistake 3: Forgetting the reciprocal relationship
- Why it happens: Mixing up R=ρAl with κ=ρ1.
- How to avoid: Draw a quick memory chain: …
- GUJCET 2025Set 031 markMCQQ.Which relation is correct for Λm(H2O)0? (A) Λm(HCl)0+Λm(NH4Cl)0−Λm(NH4OH)0 (B) Λm(HCl)0+Λm(NaOH)0−Λm(NaCl)0 (C) Λm(HNO3)0+Λm(NaNO3)0−Λm(NaOH)0 (D) Λm(HNO3)0+Λm(Ba(OH)2)0−Λm(Ba(NO3)2)0
›Reveal solutionSolution
[!TLDR]
Adding HCl and NaOH conductivities and subtracting NaCl cancels Na+ and Cl−, giving Λm0(H2O)=Λ0(H+)+Λ0(OH−).
Concept
Kohlrausch's law: at infinite dilution the molar conductivity is the sum of independent ionic contributions. So conductivities of appropriate electrolytes can be combined to obtain that of a weak electrolyte like water.
Solution
We need Λm0(H2O)=λ0(H+)+λ0(OH−).
Take option (B):
Λm0(HCl)+Λm0(NaOH)−Λm0(NaCl) …
- GSEB Higher Secondary Certificate (HSC) Examination 2025Set ANNUAL1 markMCQQ.The conductivity of 0.40M solution of KCl at 298K is 0.0248 S cm-1. Its Molar conductivity is _____ S cm2 mol-1.(a) 62(b) 96(c) 124(d) 48
›Reveal solutionSolution
Molar conductivity = conductivity x 1000 / molarity (with conductivity in S/cm and molarity in mol/L).
Given: kappa = 0.0248 S cm-1, M = 0.40 mol/L.
Formula: Lambda_m = (kappa x 1000) / M
…
- GSEB Higher Secondary Certificate (HSC) Examination 2024Set ANNUAL1 markMCQQ.Lambda-m-degree for NaCl, HCl and NaAc are 126.4, 425.9 and 91.0 S cm2 mol-1 respectively. Calculate Lambda-degree for HAc.(a) 461.3 Scm2mol-1(b) 208.5 Scm2mol-1(c) 643.3 Scm2mol-1(d) 390.5 Scm2mol-1
›Reveal solutionSolution
Kohlrausch's law of independent migration of ions lets a weak electrolyte's limiting molar conductivity be built from strong electrolytes sharing its ions.
lambda-degree-m(HAc) = lambda-degree-m(HCl) + lambda-degree-m(NaAc) - lambda-degree-m(NaCl)
= 425.9 + 91.0 - 126.4
= 390.5 S cm2 mol-1
…
- GUJCET 2023Set 091 markMCQQ.Resistance of a conductivity cell filled with 0.1 M KCl solution is 100 Ω and conductivity of solution is 1.29 s/m. Then what will be the value of conductivity cell constant. (A) 1.29 cm−1 (B) 1.29 m−1 (C) 1.24 cm−1 (D) 0.248 m−1
›Reveal solutionSolution
Cell constant G∗=κ×R.
Concept: Conductivity κ=R1⋅Al, so the cell constant Al=κ×R.
G∗=1.29 S m−1×100 Ω=129 m−1. …
- GUJCET 2020Set 071 markMCQQ.For which of the following electrolytes the graph of Λm against C gives a negative slope. (A) Ammonium hydroxide (B) Sodium acetate (C) Acetic acid (D) Water
›Reveal solutionSolution
The linear negative slope of Λm vs C (Debye–Hückel–Onsager) is characteristic of a strong electrolyte — sodium acetate.
Concept — strong vs. weak electrolyte conductance. For strong electrolytes Λm=Λm0−bC, a straight line of negative slope. Weak electrolytes (acetic acid …
- GSEB Higher Secondary Certificate (HSC) Examination 2020Set ANNUAL1 markMCQQ.Λ°m(HAc) is equal to ______.(a) Λ°m(KCl) + Λ°m(KAc) - Λ°m(HCl)(b) Λ°m(HCl) + Λ°m(NaAc) - Λ°m(NaCl)(c) Λ°m(AcH) + Λ°m(KAc) + Λ°m(NaAc)(d) Λ°m(KCl) + Λ°m(NaAc) - Λ°m(NaCl)
›Reveal solutionSolution
Kohlrausch's law of independent migration of ions lets the limiting molar conductivity of a weak electrolyte be built from the limiting conductivities of strong electrolytes that share its ions.
HAc (acetic acid) is a weak electrolyte, so Λ°m(HAc) cannot be measured directly by extrapolation. Kohlrausch's law: Λ°m(HAc) = λ°(H+) + λ°(Ac-). Using strong electrolytes: Λ°m(HCl) = λ°(H+)+λ°(Cl-); Λ°m(NaAc) = λ°(Na+)+λ°(Ac-); Λ°m(NaCl) = λ°(Na+)+λ°(Cl-). Addin …
- GSEB Higher Secondary Certificate (HSC) Examination 2019Set ANNUAL1 markMCQQ.What is correct for the limiting molar conductivity of ammonium hydroxide, Lambda°m(NH4OH)?(a) Lambda°m(NH4Cl) + Lambda°m(NaOH) - Lambda°m(NaCl)(b) Lambda°m(NH4Cl) + Lambda°m(NaCl) - Lambda°m(NaOH)(c) Lambda°m(NaOH) + Lambda°m(NH4Cl) - Lambda°m(HCl)(d) Lambda°m(NaCl) + Lambda°m(NH4Cl) + Lambda°m(NaOH)
›Reveal solutionSolution
Kohlrausch's law lets the limiting molar conductivity of a WEAK electrolyte be built from the limiting molar conductivities of STRONG electrolytes that share its ions.
NH4OH is a weak electrolyte, so its limiting (infinite dilution) molar conductivity cannot be measured directly by extrapolation (its conductivity does not vary linearly with concentration near zero concentration). Instead, Kohlrausch's law of independent migration of ions is used: choose combinations of STRONG electrolytes that, added and subtracted, give exactly the ions NH4+ and OH-.
Lambda-degree-m(NH4Cl) supplies NH4+ and Cl-.
Lambda-degree-m(NaOH) supplies Na+ and OH-. …
- GSEB Higher Secondary Certificate (HSC) Examination 2018Set ANNUAL1 markMCQQ.The limiting molar conductivity and molar conductivity of acetic acid are 390.5 s.cm2.mol^-1 and 48.15 s.cm2.mol^-1 respectively. Calculate the degree of dissociation of the weak acid?(a) 12.33(b) 0.1233(c) 1.233(d) 0.01233
›Reveal solutionSolution
alpha = Lambda_m / Lambda_m(infinity) = 48.15/390.5 = 0.1233.
For a weak electrolyte, the degree of dissociation equals the ratio of its molar conductivity at the given concentration to its limiting (infinite-dilution) molar conductivity:
…
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