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Thermodynamics · reward round

Engine Room

246810100200300400V (dm³)p (kPa)Tₕ 480 KT_c 300 KW = 58 JQₕ inQ_c outCDAB

Engine Room

Two corners, one loop. Drag them to shape a cycle between the hot and cold plates — the area you enclose is the work you get paid for.

Tap the stage to clock in

Drag the two corners of the cycle on the p–V diagram. The shaded area is the work you sell, Qₕ is the heat drawn from the hot plate along the expansion, and η = W/Qₕ chases — but never catches — the Carnot ceiling η_C = 1 − T_c/Tₕ.

Score0best 0 · streak 0×
W = area58JQₕ 212 J from the 480 K plate
η = W / Qₕ27.5%Carnot ceiling 37.5%
Level 1/51· Stoke itwork W ≥ 100 J

Score 0 · level 1/5 · work W ≥ 100 J

How the physics works

Every stroke obeys the first law, Q = ΔU + W, with ΔU = (3/2)Δ(pV) for the monatomic gas. The hot stroke A→B is a straight line in the p–V plane, and because dQ along a straight segment changes direction at most once, the game splits it there and books the heat gross: Qₕ is only what flows in. The two curved flanks are exact adiabats (pV^γ constant, Q = 0), and the return stroke rides the cold plate’s isotherm, rejecting Q_c = nRT_c·ln(V_D/V_C).

The work is the enclosed area: going round the loop, ∮p dV is exactly Qₕ − |Q_c|, which is why the shaded patch and the W read-out can never disagree. Efficiency is η = W/Qₕ — work sold per joule of heat bought.

The drag limits keep the whole loop between the reservoir temperatures, and that is what makes Carnot unbeatable here: heat absorbed at T ≤ Tₕ brings entropy of at least Qₕ/Tₕ, entropy the gas can only shed by paying at least T_c·(Qₕ/Tₕ) to the cold plate. So η ≤ 1 − T_c/Tₕ with equality only for a reversible cycle hugging both isotherms — level 5’s “target” sits above that ceiling, which is why no shape of loop, in this game or in any laboratory, can reach it.

Game 22 · Thermodynamics learning guide

Turn the playthrough into a physics lesson.

Learning objectiveShape a cycle on a pressure–volume diagram to produce useful work while respecting the Carnot efficiency limit.

01

What you will learn

  • The enclosed area of a p–V cycle represents net work.
  • Clockwise and anticlockwise cycles have opposite work signs.
  • No heat engine can exceed the Carnot efficiency for its reservoirs.

02

How to play

  1. Read the reservoir temperatures and the shift target.
  2. Drag the glowing corners to shape a closed cycle on the p–V diagram.
  3. Fire the cycle, inspect its work and efficiency, then refine the shape.

03

Quick classroom check

What geometric feature of a p–V cycle gives the net work done per cycle?

Suitable forUpper-secondary physics · thermodynamics and heat engines

Continue this topic

Move from play to explanation and exam-style practice.

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