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MHT-CET Physics · Thermal Properties of Matter

Temperature Scales and Thermal Expansion

A solid grows in every dimension when heated: its length by αLΔT, its area by 2αAΔT and its volume by 3αVΔT, where α is the coefficient of linear expansion; the Celsius, Fahrenheit and Kelvin scales are linear relabellings of one another.

Why this matters

19 PYQs, 2 of them HARD. Two convert between temperature scales. Eleven are linear expansion — the gap left between rails, a rod's α from its growth, and the favourite: two rods whose difference in length stays the same at every temperature. Six are area and volume expansion, including a thermometer's mercury column. Three cards.

Concept 1 of 3: Converting Between Temperature Scales

Every temperature scale is a straight line through two fixed points. Celsius puts ice at 0 and steam at 100; Fahrenheit puts them at 32 and 212; Kelvin is Celsius shifted by 273. So C/5 = (F − 32)/9 and K = C + 273. A question that asks where two scales read the same number sets them equal and solves: C = F at −40, and a body reads the same number in Kelvin and Fahrenheit at about 574.

Definition

  • C5=F−329\dfrac{C}{5} = \dfrac{F - 32}{9}, K=C+273K = C + 273.
  • 140 °F = 60 °C; C = F at −40; K = F at ≈ 574.

Scale conversion

C5=F−329=K−2735\frac{C}{5} = \frac{F - 32}{9} = \frac{K - 273}{5}

Worked example

A room is at 25 °C. What is that in Fahrenheit and in kelvin?
Practice this conceptself-check · 1 quick reps

The same idea in a real exam question:

MHT-CET · 2025 · 22 April Shift I · Q14Moderate

Example 1 · Thermal Properties of Matter · Thermal Expansion — Linear, Surface, Volumetric

The temperature of a body on Kelvin scale is ' xx ' K. When it is measured by a Fahrenheit thermometer, it is found to be ' x '  ∘F\ ^{\circ}F. The value of ' xx ' is (nearly)

Forgetting the 32 in Fahrenheit

Fahrenheit is not a scaled Celsius: it starts at 32. Subtract 32 before multiplying by 5/9, not after.

Concept 2 of 3: Linear Expansion and Rods That Keep Their Difference

A rod of length L heated through ΔT grows by ΔL = αLΔT. A rail laid with a gap needs that gap to equal the growth between the laying temperature and the hottest day. Two rods of different materials keep a constant difference in length only if they grow by the same amount, αₐLₐ = α_bL_b, so the longer rod must be made of the material that expands less. Once that ratio is fixed, the given difference fixes each length.

Definition

  • ΔL=αLΔT\Delta L = \alpha L \Delta T; α=ΔLL ΔT\alpha = \dfrac{\Delta L}{L\,\Delta T} (2 m, 1.6 mm over 60 °C ⇒ 1.33×10−51.33\times10^{-5}/°C).
  • Rail gap: 10 m, α=1.3×10−5\alpha = 1.3\times10^{-5}, 17 → 45 °C ⇒ 3.64 mm.
  • Constant difference: αALA=αBLB\alpha_A L_A = \alpha_B L_B, LALB=αBαA\dfrac{L_A}{L_B} = \dfrac{\alpha_B}{\alpha_A}.
  • Two rods joined, equal growth: L1L1+L2=α2α1+α2\dfrac{L_1}{L_1 + L_2} = \dfrac{\alpha_2}{\alpha_1 + \alpha_2}.

Linear expansion

ΔL=αLΔT\Delta L = \alpha L \Delta T

Worked example

A 0.5 m brass rod (α = 2 × 10⁻⁵ /°C) is heated from 20 °C to 120 °C. Increase in length?
Practice this conceptself-check · 2 quick reps

The same idea in a real exam question:

MHT-CET · 2025 · 26 April Shift I · Q28Hard

Example 2 · Thermal Properties of Matter · Thermal Expansion — Linear, Surface, Volumetric

The difference in length between two rods A and B is 60 cm at all temperatures. If αA=18×10−6/ ∘C\alpha_{A}= 18 \times10^{- 6}/\ ^{\circ}C and αB=27×10−6/ ∘C\alpha_{B}= 27 \times10^{- 6}/\ ^{\circ}C, then the length of rodArodA and rodBrodB at 0∘C0^{\circ}C is respectively

Pairing the longer rod with the larger α

Equal growth needs αL equal, so the longer rod has the SMALLER coefficient: L_A/L_B = α_B/α_A, not α_A/α_B.

Using the final length in ΔL = αLΔT

L is the original length. For the small changes asked here the difference is negligible, but a question that gives length 'at 0 °C' means use that one.

Concept 3 of 3: Area and Volume Expansion

Each dimension grows by the same fraction αΔT, so an area grows by twice that fraction and a volume by three times: β = 2α and γ = 3α. A percentage increase in volume over a temperature rise gives γ directly; divide by 3 for α. Two rods of the same material heated equally grow in volume in proportion to their volumes. A liquid-in-glass thermometer works because the liquid's volume grows by γVΔT and has nowhere to go but up a thin stem, so the column rises by that volume divided by the stem's cross-section.

Definition

  • ΔA=2αAΔT\Delta A = 2\alpha A\Delta T, ΔV=3αVΔT\Delta V = 3\alpha V\Delta T (β = 2α, γ = 3α).
  • From a percentage: γ=ΔV/VΔT\gamma = \dfrac{\Delta V / V}{\Delta T} (0.225% over 30 °C ⇒ α=2.5×10−5\alpha = 2.5\times10^{-5}).
  • Cube of side 1 m, α = 18 × 10⁻⁶, 100 °C: ΔV=54×10−4\Delta V = 54\times10^{-4} m³.
  • Thermometer column: h=γVΔTAstemh = \dfrac{\gamma V \Delta T}{A_{\text{stem}}}.

Area and volume

ΔA=2αA ΔT,ΔV=3αV ΔT\Delta A = 2\alpha A\,\Delta T, \qquad \Delta V = 3\alpha V\,\Delta T

Worked example

A steel plate 20 cm × 10 cm (α = 1.2 × 10⁻⁵ /°C) is heated by 50 °C. Increase in area?
Practice this conceptself-check · 1 quick reps

The same idea in a real exam question:

MHT-CET · 2025 · 25 April Shift II · Q28Easy

Example 3 · Thermal Properties of Matter · Thermal Expansion — Linear, Surface, Volumetric

The volume of a metal sphere increases by 0.33%0.33\% when its temperature is raised by 50∘C50^{\circ}C. The coefficient of linear expansion of the metal is

Using α for a volume

A volume grows by 3αVΔT. A percentage change in VOLUME gives γ; dividing by 3 gives α, and the options include γ itself.

Summary — formulas & gotchas at a glance

A revision cheat-sheet for the formulas and gotchas above. Click any concept name to jump back to its full explanation.

Formulas (3)

Watch out for (4)

Test yourself on Thermal Properties of Matter

20 past MHT-CET questions from this chapter, timed at 18 minutes and marked the way the exam marks it. You see your score and every answer the moment you finish. Free to start.