Q.A negligibly small current is passed through a wire of length 15 m and uniform cross-section 6.0×10−7 m2, and its resistance is measured to be 5.0 Ω. What is the resistivity of the material at the temperature of the experiment?
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Temperature Dependence of Resistance
Imagine you're trying to walk through a crowded market. When the market is cool and calm, people move slowly and you can weave through easily. Now imagine the same market on a hot, chaotic day — everyone is jostling, moving faster, bumping into each other. Getting from one end to the other becomes much harder.
That's exactly what happens inside a metal wire when you heat it up.
The Intuition
In a metal, electric current is carried by free electrons drifting through a fixed lattice of positive ions. At room temperature, these ions are vibrating slightly around their positions. When you heat the metal, the ions vibrate more vigorously — they shake faster and with larger amplitude.
Think of the vibrating ions as a row of swinging doors. At low temperature, the doors barely move, so electrons slip through easily. At high temperature, the doors swing wildly, and electrons get knocked off course constantly. Each collision with a vibrating ion scatters the electron, making it harder for the current to flow.
The result: resistance increases as temperature increases — for most conductors.
The Precise Statement
For a metallic conductor over a moderate temperature range (not too close to absolute zero), the resistance changes linearly with temperature:
R(T)=R0[1+α(T−T0)]
Where:
- R(T) is the resistance at temperature T
- R0 is the resistance at a reference temperature T0 (often 0∘C or 20∘C)
- α is the temperature coefficient of resistance (units: per °C or per K)
R=R0(1+αΔT)
The coefficient α tells you how sensitive the material is to temperature changes. For copper, α≈0.0039/∘C — meaning for every 1°C rise, resistance increases by about 0.39%.
What About Other Materials?
Not everything behaves like metals.
Semiconductors (like silicon, germanium) do the opposite: their resistance decreases sharply as temperature rises. Why? Because heating frees more electrons from their bonds, creating many more charge carriers. Even though the lattice vibrates more, the huge increase in available carriers overwhelms that effect, so resistance drops.
Insulators also show decreasing resistance with temperature, but the effect is much smaller than in semiconductors.
Alloys like constantan (copper-nickel) have a very small α — their resistance barely changes with temperature. This is useful for making precision resistors that stay stable.
Superconductors are a special case: below a critical temperature, resistance drops to exactly zero. …
Why this formula?
Temperature Dependence of Resistance — Why the Formula Holds
Let’s build this from the ground up. The key formula you’ll see in exams is:
RT=R0(1+αT)
But why does resistance change with temperature? It’s not magic — it’s about what happens inside the wire.
1. What determines resistance?
Resistance R of a conductor depends on three things:
- Length L (longer → more resistance)
- Cross-sectional area A (thicker → less resistance)
- Resistivity ρ — a material property
The formula is:
R=ρAL
When temperature changes, L and A change very slightly (thermal expansion), but the big effect is on ρ.
2. Why does resistivity change with temperature?
Resistivity ρ depends on how easily electrons can move through the material.
- In metals: Atoms vibrate more as temperature rises. These vibrations scatter electrons, making it harder for them to flow. So ρ increases.
- In semiconductors: More electrons get enough energy to jump into the conduction band. So ρ decreases.
For most metals (and many conductors), the change is linear over a moderate temperature range.
3. Deriving the linear formula
Let ρ0 be resistivity at a reference temperature T0 (often 0∘C or 20∘C).
For a small change ΔT=T−T0, the change in resistivity is proportional to ΔT and to ρ0:
Δρ∝ρ0ΔT
Introduce the temperature coefficient of resistivity α:
Δρ=αρ0ΔT
So the new resistivity is:
ρ=ρ0+Δρ=ρ0(1+αΔT)
Now, since R=ρAL, and L and A change negligibly (for small ΔT), we get:
R=ρAL=ρ0(1+αΔT)AL=R0(1+αΔT)
That’s the formula:
RT=R0(1+αΔT)
Where:
- RT = resistance at temperature T
- R0 = resistance at reference temperature T0
- α = temperature coefficient of resistance (unit: ∘C−1 or K−1)
- ΔT=T−T0
--- …
The key idea is that resistance depends on the material’s resistivity, length, and cross-sectional area through R=ρAL.
Step 1: Write the formula for resistance in terms of resistivity:
R=ρAL
Step 2: Rearrange to solve for resistivity:
ρ=RLA
Step 3: Substitute the given values — R=5.0 Ω, A=6.0×10−7 m2, L=15 m: …
Using the relation R=ρAL, the resistivity is found by rearranging to ρ=LRA. Substituting the given values gives ρ=2.0×10−7 Ω⋅m.
The key idea here is that resistance depends on both the material's intrinsic property (resistivity) and the geometry of the wire. When we pass a negligibly small current, we avoid heating the wire, so the measurement is at the ambient temperature — exactly what the question asks for.
Why this approach works:
For a uniform conductor, resistance R is directly proportional to length L and inversely proportional to cross-sectional area A. The constant of proportionality is the resistivity ρ, a material property that changes with temperature. Since the current is tiny, Joule heating is negligible, so the measured resistance corresponds to the temperature of the experiment. We simply plug into the formula.
Let’s work through it step by step.
- Write the fundamental relation For a wire of uniform cross-section,
R=ρAL
This is the standard formula — memorize it. Resistivity ρ has units Ω⋅m.
- Rearrange for resistivity Multiply both sides by A and divide by L:
ρ=LRA
-
Substitute the given values
- R=5.0 Ω
- A=6.0×10−7 m2
- L=15 m
So
ρ=15(5.0)×(6.0×10−7)
- Simplify step by step First multiply numerator: 5.0×6.0×10−7=30×10−7=3.0×10−6 …
Method: Direct Application of the Resistivity Formula
This is a straightforward problem using the resistivity definition from Ohm's law in terms of material geometry.
Concept (Why this works)
Resistance R of a wire depends on three things:
- Material (resistivity ρ)
- Length L (longer → more resistance)
- Cross-sectional area A (thicker → less resistance)
The relationship is:
R=ρAL
We know R, L, and A — so we can solve for ρ.
Steps
Step 1: Write the formula
ρ=R⋅LA
Step 2: Substitute the given values
- R=5.0 Ω
- L=15 m
- A=6.0×10−7 m2
ρ=5.0×156.0×10−7
Step 3: Simplify
ρ=5.0×156.0×10−7
ρ=5.0×0.4×10−7 …
Here are the common mistakes students make on this exact problem, along with how to avoid each one.
Mistake 1: Forgetting to convert units
The error:
Students often plug in the numbers as given without checking if all units are in SI. Here, length is in meters (15 m) and area is in m2 (6.0×10−7 m2), so no conversion is needed. But in other problems, length might be in cm or area in mm2, and forgetting to convert leads to a wrong resistivity.
How to avoid:
Always write the SI base units next to each quantity before substituting. If any value is not in SI (e.g., cm, mm²), convert it first. For this problem, confirm:
- L=15 m ✓
- A=6.0×10−7 m2 ✓
- R=5.0 Ω ✓
Mistake 2: Using the wrong formula
The error:
Some students confuse resistivity (ρ) with resistance (R) and write R=ρAL but then solve incorrectly — e.g., they might write ρ=R⋅A⋅L instead of ρ=R⋅LA.
How to avoid:
Memorise the definition:
Resistivity is the resistance of a unit cube of the material.
The formula is:
R=ρAL
Rearranging:
ρ=R⋅LA
Write the rearrangement step explicitly before plugging in numbers.
Mistake 3: Arithmetic errors with powers of ten
The error:
When substituting A=6.0×10−7 and L=15, students often mishandle the exponent — e.g., they might compute 10−7/15 incorrectly or forget to multiply by R.
How to avoid:
Do the arithmetic in two steps:
- Compute the numeric part: 5.0×156.0=5.0×0.4=2.0
- Attach the power of ten: 10−7
So:
ρ=2.0×10−7 Ω⋅m
Check:
LA=156.0×10−7=0.4×10−7=4.0×10−8
Then ρ=5.0×4.0×10−8=20×10−8=2.0×10−7 ✓
Always re-check the exponent by estimating orders of magnitude.
Mistake 4: Ignoring the phrase “at the temperature of the experiment”
The error:
Students treat the result as the standard resistivity of the material (like from a table at 0°C or 20°C). But the problem clearly states the measurement is at the experiment’s temperature, which may not be room temperature. …
- KEAM 2026Set eng-2026-04184 marksMCQQ.The temperature coefficient of resistance of a coil of wire of resistance 4Ω at 30∘C and 6Ω at 70∘C (in per ∘C) is (A) 0.04 (B) 0.06 (C) 0.004 (D) 0.006 (E) 0.02
›Reveal solutionSolution
Using Rt=R0(1+αt) at the two temperatures and eliminating R0 gives α=0.02∘C−1.
With Rt=R0(1+αt):
R1=R0(1+αt1),R2=R0(1+αt2)
Eliminating R0:
α=R1t2−R2t1R2−R1 …
- KEAM 2026Set eng-2026-04204 marksMCQQ.A copper wire of temperature coefficient of resistance 4×10−3K−1 has resistance 10 Ω at 20∘ C. Its resistance at 80∘ C is (A) 1.22 Ω (B) 12.2 Ω (C) 24.4 Ω (D) 38.8 Ω (E) 2.44 Ω
›Reveal solutionSolution
Linear resistance–temperature law: R=R0(1+αΔT) gives 12.4 Ω.
Compute. ΔT=80−20=60∘C. …
- KEAM 2026Set eng-2026-04224 marksMCQQ.With increase in temperature, the resistivity of (A) both Cu and Ge increases (B) both nichrome and Ge decreases (C) nichrome decreases and that of Ge increases (D) both Cu and nichrome increases (E) Cu, nichrome and Ge increases
›Reveal solutionSolution
Metals and alloys have positive temperature coefficients; semiconductors (Ge) have negative.
With rising temperature: Cu (a metal) and nichrome (an alloy) both show increasing resistivity, while germanium (a semiconductor) shows decreasing resistivity. …
- KEAM 2025Set eng-2025-04264 marksMCQQ.The resistance of a wire at 30ºC and 40ºC are respectively 5 Ω and 6 Ω. The temperature coefficient of resistance of the material of the wire (in per degree Celcius) is (A) 0.04 (B) 0.05 (C) 0.02 (D) 0.03 (E) 0.01
›Reveal solutionSolution
The temperature coefficient of resistance is 0.05/∘C.
Using R=R0(1+αt) with R30=5Ω and R40=6Ω:
R30R40=1+30α1+40α=56.
Cross-multiplying: …
- KEAM 2025Set eng-2025-04264 marksMCQQ.A wire of 25 Ω resistance is cut into n pieces of equal length. If these pieces of wires are connected in parallel, their equivalent resistance is 1 Ω, then the value of n is (A) 3 (B) 6 (C) 8 (D) 5 (E) 4
›Reveal solutionSolution
Cutting the wire into n equal pieces makes each 25/n Ω; connecting n of them in parallel gives 25/n2=1 Ω, so n=5.
Resistance of each piece:
Rpiece=n25 Ω
Parallel of n equal resistors: …
- KEAM 2025Set eng-2025-04274 marksMCQQ.The current carrying rail of a subway track is made of steel and has a cross-sectional area of about 20 cm2. The resistance of 2 km of the track is (in ohm) as a multiple of the specific resistance of steel, ρ is: (A) 102ρ (B) 103ρ (C) 104ρ (D) 105ρ (E) 106ρ
›Reveal solutionSolution
R=ρL/A with L=2000 m and A=20 cm2=2×10−3 m2 gives R=106ρ.
Resistance of a uniform conductor is
R=ρAL. …
- KEAM 2025Set eng-2025-04294 marksMCQQ.If both the length and area of cross-section of a linear conductor are halved, its resistance would (A) be doubled (B) remain unchanged (C) be halved (D) be tripled (E) be quadrupled
›Reveal solutionSolution
Resistance R=ρL/A. Halving the length and the area gives R′=ρ(L/2)/(A/2)=ρL/A=R — unchanged.
The resistance of a conductor is R=AρL. If both L and A are halved, R′=(A/2)ρ(L/2)=AρL=R. The tw …
- KEAM 2024Set eng-2024-06064 marksMCQQ.The resistance of a wire at 0 ∘C is 4 Ω. If the temperature coefficient of resistance of the material of the wire is 5×10−3/∘C, then the resistance of a wire at 50 ∘C is (A) 20 Ω (B) 10 Ω (C) 6 Ω (D) 8 Ω (E) 5 Ω
›Reveal solutionSolution
Resistance rises linearly with temperature: R=R0(1+αT).
Using R=R0(1+αT) with R0=4 Ω, α=5×10−3/∘C and T=50∘C: …
- KEAM 2024Set eng-2024-06074 marksMCQQ.Masses of three copper wires are in the ratio 1 : 3 : 5 and their lengths are in the ratio 5 : 3 : 1. Then the ratio of their electric resistances is (A) 125 : 15 : 1 (B) 5 : 3 : 1 (C) 1 : 25 : 125 (D) 1 : 3 : 5 (E) 5 : 21 : 25
›Reveal solutionSolution
Resistance of a wire of fixed material is R∝L2/m, giving 25:3:0.2=125:15:1.
Resistance R=AρL. The cross-sectional area is A=Lvolume=Lm/d, where d is the (common) density. Hence R=m/(dL)ρL=mρdL2, i.e. R∝mL2. …
- KEAM 2024Set pha-2024-06104 marksMCQQ.Resistivity of a conductor increases with (A) increase in its length (B) decrease in its length (C) increase in its area of cross-section (D) decrease in its area of cross-section (E) increase in its temperature
›Reveal solutionSolution
Resistivity is a material property, independent of geometry.
Resistivity ρ depends on the material and temperature, not on length or cross-section (those affect resistance R=ρl/A, not ρ). For a metallic conductor, ρ increases with temperature due to inc …
- KEAM 2022Set eng-2022-P1-A14 marksMCQQ.The INCORRECT statement is (A) Resistivity of copper increases with increase of temperature (B) Resistivity of germanium decreases with the increase of temperature (C) Resistivity of semiconductors is higher than that of the conductors (D) Resistivity of nichrome shows a weak dependence with temperature (E) Resistivity of insulators is independent of temperature
›Reveal solutionSolution
The false statement is that insulators' resistivity is independent of temperature; it actually varies (decreasing) with temperature.
Concept and Intuition
Resistivity's temperature behaviour differs by material type: metals (copper, nichrome) increase with temperature; semiconductors (germanium) decrease with temperature; insulators are not temperature-independent — like semiconductors, their resistivity falls with rising temperature as more carriers become available.
Step-by-Step Solution
- (A) Copper is a metal: resistivity increases with temperature — correct.
- (B) Germanium is a semiconductor: resistivity decreases with temperature — correct.
- (C) Semiconductors have higher resistivity than conductors — correct.
- (D) Nichrome (alloy) has a weak temperature dependence — correct. …
- KEAM 2022Set eng-2022-P1-A14 marksMCQQ.Material that is widely used to make wire bound standard resistors is (A) manganin (B) iron (C) copper (D) tungsten (E) germanium
›Reveal solutionSolution
Standard wire-wound resistors are made of manganin because of its very low temperature coefficient of resistance.
Concept and Intuition
A standard resistor must keep its resistance essentially constant with temperature and time. Manganin (Cu–Mn–Ni alloy) has an extremely small temperature coefficient of resistivity, making its resistance stable — ideal for precision standard resistors. Copper, iron and tungsten have significant temperature coefficients; germanium is a semiconductor.
Step-by-Step Solution
- Requirement: near-zero temperature coefficient for a stable standard. …
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