IB Chemistry HL Topic 4 — Entropy & Spontaneity Paper 1 & 2 Core idea ~11 min read

Entropy

Cold packs get cold. Ice melts on a warm day. Ammonium nitrate soaks up heat and still dissolves happily. If reactions only ever went downhill in energy, none of that should happen. So something else must be pushing, and that something is entropy.

📚 What you need to know

Why enthalpy on its own is not enough

At SL you learned that exothermic reactions give heat out and are the ones that usually “want” to happen. That rule takes you a long way, and then it breaks. Sports cold packs work because ammonium nitrate dissolving in water is endothermic — it pulls heat from your skin. Nobody has to force it. Tear the pack, and it happens on its own.

So the energy going downhill cannot be the whole story. There is a second thing nature keeps score of, and it has nothing to do with heat given out. It is about how spread out things end up.

Think of it as two questions a reaction has to answer, not one. “Do I release energy?” and “Do I spread things out?” A yes to either one can carry the reaction. This page is all about the second question.

What entropy actually measures

Entropy is a counting idea. Take a system and ask: in how many different ways could I arrange these particles and share out their energy, and still have the same overall thing? Lots of ways means high entropy. Very few ways means low entropy.

Entropy in one line S = a measure of how many ways the particles
and their energy can be arranged

Here is the everyday version. There is exactly one way for your books to be stacked neatly in the right order on the shelf. There are thousands of ways for them to be scattered across your bedroom floor. Both are possible, but “scattered” has far more versions of itself, so if things get shuffled at random you end up scattered nearly every time. That is entropy: spread-out states are more likely simply because there are more of them.

Energy behaves the same way. Heat never gathers itself back into one hot spot in a cold room, because there are vastly more ways for that energy to be shared among all the particles than to be piled into a few.

Same substance, three states: how spread out are the particles? More freedom to move means more ways to arrange things, so more entropy SOLID LIQUID GAS locked in place close, sliding past far apart, fast entropy increases
The particles are identical in all three boxes. What changes is how many different positions and speeds they are allowed to have — and that is what entropy counts.

Solid, liquid, gas: look at the real numbers

You do not have to take this on trust. The data booklet lists a standard molar entropy, S°, for hundreds of substances: the entropy of one mole in its standard state at 298 K and 100 kPa. Line up the same substance in different states and the pattern jumps out.

Standard entropy: the jump on boiling is the big one Values in J K⁻¹ mol⁻¹ at 298 K, taken from the data booklet S / J K⁻¹ mol⁻¹ 48 70 189 116 261 H₂O(s) H₂O(l) H₂O(g) I₂(s) I₂(g) water iodine Melting frees the particles a little. Boiling frees them completely. So any reaction that makes a gas is a very good bet for a positive entropy change.
Ice to water adds 22 units. Water to steam adds 119. That gap is why the gases in an equation matter more than anything else when you are judging the sign of ΔS.
Why is boiling such a big deal? In a liquid the particles are still touching, so they are stuck with their neighbours. In a gas each particle can be almost anywhere in the container, moving at almost any speed. The number of possible arrangements explodes, and so does S.

What pushes entropy up

You will be asked to predict the sign of ΔS without a calculator, so learn the things that move it. In order of how much they matter:

Run those in reverse and entropy falls: gases being used up, gases turning into liquids, many particles joining into few.

🧩 How to predict the sign of ΔS in ten seconds

  1. Count moles of gas on the left using the balancing numbers.
  2. Count moles of gas on the right the same way.
  3. More gas on the right? ΔS is positive. Less gas on the right? Negative.
  4. Same gas count on both sides? Now look at solids melting or dissolving, and at the total number of particles.
  5. Still tied? Then ΔS is small — say so, and say why. That is worth the mark.
The fastest check: count the moles of gas on each side Gas is where nearly all of the entropy sits, so the gas count usually decides the sign MgCO₃(s) → MgO(s) + CO₂(g) 2H₂(g) + O₂(g) → 2H₂O(l) H₂(g) + Cl₂(g) → 2HCl(g) gas: 0 → 1 mol gas: 3 → 0 mol gas: 2 → 2 mol ΔS positive ΔS negative ΔS near zero More gas moles on the right means far more ways to arrange things. Gas count tied? Then compare particle numbers and molecule sizes instead.
Notice the third row. Two moles of gas become two moles of gas, so nothing dramatic happens — the small positive value comes from turning two identical molecules into two different ones.

Common changes and their entropy sign

ChangeWhat happens to the particlesSign of ΔS
Ice meltingFixed lattice becomes a liquid that can flowPositive
Water boilingTouching particles become free and far apartPositive, and large
Salt dissolving in waterLattice breaks up, ions spread through the solutionPositive
A carbonate decomposingSolid gives off a gasPositive
Steam condensingFree gas particles get trapped in a liquidNegative
Ammonia being made from N2 and H24 mol of gas becomes 2 mol of gasNegative
H2 and Cl2 making HCl2 mol of gas becomes 2 mol of gasNear zero

Worked examples

WORKED EXAMPLE

Predict, with a reason, whether ΔS is positive or negative for N2(g) + 3H2(g) → 2NH3(g).

Count the gas on the left 1 mol N2 + 3 mol H2 = 4 mol of gas Count the gas on the right 2 mol of gas Compare 4 mol of gas becomes 2 mol, so the particles have fewer ways to be arranged. ΔS is negative The mark is for the reason, not the word. Write “the number of moles of gas falls from 4 to 2”.
WORKED EXAMPLE

Ammonium nitrate dissolving in water takes heat in from its surroundings. Explain why it dissolves anyway.

What the enthalpy says ΔH is positive, so on energy grounds alone this change looks unfavourable. What happens to the arrangement An ordered ionic lattice breaks apart and the NH4+ and NO3− ions spread right through the water. So the entropy change is Strongly positive — a huge gain in ways to arrange the ions. The entropy gain outweighs the energy cost This is the whole reason the next three pages exist. Two competing effects need one number to settle them, and that number is ΔG.
WORKED EXAMPLE

Put these in order of increasing entropy, all at 298 K: 1 mol of CO2(g), 1 mol of H2O(l), 1 mol of NaCl(s).

Sort by state first Solid is lowest, then liquid, then gas — state beats everything else here. Put them in line NaCl(s) < H₂O(l) < CO₂(g) Check against the booklet 72, then 70… careful. Those two are almost the same, so quote the values: NaCl(s) 72 and H2O(l) 70 J K−1 mol−1. H₂O(l) ≈ NaCl(s), both well below CO₂(g) at 214 A useful reminder: solid < liquid < gas is a rule for the same substance. Across different substances you need the real numbers.

💡 Exam tip

⚠ Common mix-up

You can now say whether entropy goes up or down. Next you will put a number on it, straight from the data booklet. Up next: Calculating Standard Entropy Changes.

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