Entropy and irreversibility Explained with Examples
Entropy and irreversibility is a core Mechanical Engineering (ME) concept in Engineering. This guide explains what it is, walks through a fully worked example, and lists the key equations you need — with a short quiz to test yourself.
Key equations and worked example
1 mol of gas at 300 K in a 24.6 L cylinder: P = nRT/V = (1×8.314×300)/0.0246 ≈ 101 kPa. Heat it to 600 K at fixed volume and the pressure doubles to ≈ 202 kPa — the molecules hit the walls twice as hard. Push the temperature slider and watch the particles speed up and redden.
- <code>Ideal gas law: P·V = n·R·T</code>
- <code>First law: ΔU = Q − W</code>
- <code>Carnot efficiency: η = 1 − Tc/Th</code>
- <code>Mean molecular KE: ⟨KE⟩ = 3kT/2</code>
Entropy and irreversibility in detail
Entropy and irreversibility is one of the central ideas in Mechanical Engineering (ME), and it appears in Engineering curricula under Thermodynamics. It is worth learning deeply because it connects to so many other topics in this section.
Temperature measures the average kinetic energy of molecules (½m⟨v²⟩ = 3kT/2). Heating a gas makes molecules move faster, raising pressure at fixed volume. The first law (ΔU = Q − W) tracks energy: heat in minus work done by the gas. No heat engine beats the Carnot limit.
For exams, the pattern is predictable: first a definition or statement of the result, then a direct numerical application of one of the equations above, then a "why" question — why the formula takes that form, or what changes when a variable is doubled or halved. The worked example and quiz below cover exactly that progression.
Quick self-check:
- Q: A gas is heated from 300 K to 600 K at constant volume. What happens to its pressure?<br />A: It doubles — P ∝ T at fixed V (Gay-Lussac's law).
- Q: State the first law of thermodynamics.<br />A: ΔU = Q − W: the change in internal energy equals heat added minus work done by the system.
- Q: Why can no engine be 100% efficient?<br />A: The Carnot limit η = 1 − Tc/Th is always below 1 since Tc > 0 — some heat must be rejected.
Related blogs
- Zeroth, first and second laws of thermodynamics Explained with Examples
- Carnot cycle and thermodynamic temperature scale Explained with Examples
- Rankine cycle and steam power plants Explained with Examples
- Brayton cycle and gas turbines Explained with Examples
- Otto, Diesel and dual cycles Explained with Examples
- Psychrometry: properties of moist air Explained with Examples