Purification of organic compounds

No organic compound comes out of a reaction flask or a plant extract pure. It arrives tangled with unreacted starting material, by-products, solvent traces, or other impurities, and a chemist cannot trust a melting point, a spectrum, or a formula determined from a dirty sample. Purification is the answer: a toolkit of physical separation techniques, each built on exploiting one physical property in which the desired compound and its impurities differ. This section covers the ISC Class 11 principle-level toolkit — crystallisation, sublimation, the four flavours of distillation, differential extraction, and chromatography — with the emphasis on recognising which property is exploited and choosing the right technique for given data, exactly as the syllabus and board papers expect.

The core insight

Every purification technique separates a compound from impurities by exploiting one physical property difference between them — solubility for crystallisation, volatility for sublimation and distillation, or rate of adsorption and partition for chromatography — so choosing the right method is really an exercise in identifying which property differs and by how much.

The core idea

Purification methods are not a random list to memorise; they fall out of asking one question about a mixture: which physical property separates the compound from its impurities, and how cleanly?

  • Crystallisation — solubility. The impure solid is dissolved in the minimum volume of a hot solvent, filtered hot to remove insoluble matter, then cooled slowly. Because most solids are less soluble in cold solvent than in hot, the desired compound crystallises out first while soluble impurities remain dissolved in the mother liquor. It works best when the compound's solubility changes sharply with temperature and the impurity's does not.
  • Sublimation — direct solid-to-vapour transition. A few solids (naphthalene, camphor, benzoic acid, iodine) pass straight from solid to vapour on gentle heating, without an intervening liquid phase, and resolidify on a cool surface. Non-sublimable impurities are simply left behind.
  • Distillation — boiling point (volatility). All four variants exploit the same property but handle different constraints:
  • Simple distillation separates a volatile liquid from a non-volatile or much-higher-boiling impurity, generally when the boiling-point gap exceeds about 25 K25\ \text{K}.
  • Fractional distillation separates two miscible liquids whose boiling points are close, using a fractionating column that behaves like many simple distillations stacked in series.
  • Steam distillation suits a compound that is steam-volatile, insoluble in water, and thermally sensitive — it distils over below 373 K373\ \text{K}, well under its own boiling point.
  • Vacuum distillation lowers the external pressure so a high-boiling liquid reaches its (now lower) boiling point at a much lower temperature, again protecting a thermally unstable compound.
  • Differential extraction — relative solubility in two immiscible solvents. Shaking the mixture with a solvent such as ether in a separating funnel pulls the organic solute preferentially into the organic layer, which is drawn off from the aqueous layer.
  • Chromatography — rate of adsorption or partition. A mobile phase carries the mixture over a stationary phase (alumina in a column, or paper/a thin adsorbent layer); components that adsorb more weakly or partition more into the mobile phase travel farther/faster, spreading the mixture into separated spots or bands.

The one technique in this list with a genuine quantitative handle at this level is steam distillation, because "why does it boil below 373 K373\ \text{K}" has a precise answer in Dalton's law of partial pressures — worked out below.

Figure
Six purification techniques mapped to the single physical property each one exploits
Technique versus the property it exploits Crystallisation Solubility change with temperature Sublimation Solid to vapour without melting Simple / fractional distillation Boiling point gap between liquids Steam / vacuum distillation Lowering effective boiling temperature Differential extraction Solubility split between two solvents Chromatography Rate of adsorption / partition

Why it works — steam distillation and Dalton's law

The claim that a steam-volatile liquid distils over "below 373 K373\ \text{K}" is not a rule to accept on faith; it follows directly from how the total vapour pressure of two immiscible, mutually insoluble liquids adds up, and working through it explains why steam distillation protects a thermally sensitive compound that simple distillation would decompose.

Step 1. Two liquids that do not dissolve in each other, such as water and most organic liquids used in steam distillation, each generate their own vapour pressure at a given temperature independently of the other — neither liquid's presence lowers or raises the other's individual vapour pressure, because they are not in solution together.

Step 2. By Dalton's law of partial pressures applied to this pair, the total vapour pressure above the mixture is simply the sum of the two individual (pure-liquid) vapour pressures at that temperature:

Ptotal=pwater+porganic.(1)P_{\text{total}} = p_{\text{water}} + p_{\text{organic}}. \qquad (1)

where: PtotalP_{\text{total}} is the combined vapour pressure of the boiling mixture, pwaterp_{\text{water}} is the vapour pressure pure water would have alone at that temperature, and porganicp_{\text{organic}} is the vapour pressure the pure organic liquid would have alone at that same temperature.

Step 3. A liquid (or liquid mixture) boils at the temperature where its total vapour pressure equals the surrounding atmospheric pressure, Ptotal=Patm≈101.3 kPaP_{\text{total}} = P_{\text{atm}} \approx 101.3\ \text{kPa}. Because two vapour pressures are now adding up rather than one, the mixture reaches 101.3 kPa101.3\ \text{kPa} at a temperature lower than either pure liquid's own boiling point — in particular lower than 373 K373\ \text{K} (water's own boiling point) and far lower than a high-boiling organic liquid's own boiling point.

Step 4. Concretely: at any temperature below 373 K373\ \text{K}, pure water alone has pwater<101.3 kPap_{\text{water}} < 101.3\ \text{kPa} (it has not yet reached its own boiling point), so it cannot boil by itself. But if the organic liquid contributes even a modest extra porganicp_{\text{organic}} at that same temperature, the sum can reach 101.3 kPa101.3\ \text{kPa} well before water would have boiled on its own — and long before the organic liquid, heated alone, would have reached its own (much higher) boiling point.

Step 5. This is why the technique protects thermally sensitive compounds: sustained heating near a high boiling point (or above a decomposition threshold) is never required, because co-distillation with steam lets the mixture boil at whichever lower temperature makes the two partial pressures sum to atmospheric pressure — always below 373 K373\ \text{K} for any steam-volatile, water-insoluble organic liquid.

Worked example

Problem. A mixture contains chlorobenzene (own boiling point 405 K405\ \text{K}, insoluble in water, steam-volatile) and a resinous impurity that decomposes above 420 K420\ \text{K}. At the temperature where the mixture actually boils, water's own vapour pressure is about 85 kPa85\ \text{kPa}. (a) Estimate chlorobenzene's contribution to the total vapour pressure at that boiling point. (b) Explain why simple distillation is unsuitable here.

Step 1. The mixture boils when the sum of the two partial pressures equals atmospheric pressure: Ptotal=pwater+pchlorobenzene=101.3 kPaP_{\text{total}} = p_{\text{water}} + p_{\text{chlorobenzene}} = 101.3\ \text{kPa}.

Step 2. Rearranging for the unknown contribution: pchlorobenzene=101.3−85=16.3 kPap_{\text{chlorobenzene}} = 101.3 - 85 = 16.3\ \text{kPa}.

Step 3. This is the vapour pressure chlorobenzene alone would show at that boiling temperature — a modest figure compared with the 101.3 kPa101.3\ \text{kPa} it would need to reach on its own at 405 K405\ \text{K}. Because water is already supplying 85 kPa85\ \text{kPa}, chlorobenzene needs to contribute only the remaining 16.3 kPa16.3\ \text{kPa}, which happens at a temperature well under 373 K373\ \text{K}, not at 405 K405\ \text{K}.

Step 4. Simple distillation, by contrast, would require heating the flask up toward chlorobenzene's own boiling point of 405 K405\ \text{K} to make pchlorobenzenep_{\text{chlorobenzene}} alone reach 101.3 kPa101.3\ \text{kPa} — comfortably past the 420 K420\ \text{K} decomposition threshold's neighbourhood in practice, and certainly with no safety margin. The resinous impurity would decompose before or during that heating.

Conclusion: steam distillation is the correct choice, since Dalton's law guarantees the mixture boils below 373 K373\ \text{K} — safely under the 420 K420\ \text{K} decomposition limit — while simple distillation would demand temperatures close to chlorobenzene's own 405 K405\ \text{K} boiling point.

Competitive stretch

If the resinous impurity instead decomposed above 500 K500\ \text{K} (well clear of 405 K405\ \text{K}) and chlorobenzene needed to be recovered at high purity from a miscible liquid with a boiling point of 415 K415\ \text{K}, the better choice would flip to fractional distillation, since the boiling-point gap (10 K10\ \text{K}) is too small for simple distillation to resolve cleanly, and there is no longer a decomposition risk that steam distillation is needed to avoid.

Common traps

  • Treating simple distillation as good for separating any two liquids — it only resolves mixtures with a substantial boiling-point gap (roughly >25 K> 25\ \text{K}); closer boiling points need fractional distillation instead.
  • Confusing sublimation with ordinary evaporation or boiling — sublimation is a direct solid-to-vapour transition with no liquid phase in between, and only certain solids (naphthalene, camphor, benzoic acid, iodine) show it.
  • Assuming steam distillation and vacuum distillation solve the identical problem because both suit heat-sensitive compounds — steam distillation adds a second, independent vapour pressure (Dalton's law) at fixed atmospheric pressure, while vacuum distillation instead lowers the external pressure the compound's own vapour pressure must match; they are mechanistically different routes to the same goal.
  • Forgetting that steam distillation requires the compound to be insoluble in water as well as steam-volatile — a water-soluble steam-volatile liquid would just dissolve into the aqueous phase instead of distilling over as a separate layer.

Ask the tutor: if you would like to work through a fresh mixture — solubility data, boiling points, or a thermal-stability limit — and decide which purification technique fits, just ask the AI tutor to reason through it with you.

Why does crystallisation sometimes fail to purify a compound completely in one attempt

If the impurity has a solubility curve similar to the desired compound's, or if too much solvent is used, some impurity co-crystallises or the compound itself stays dissolved and is lost in the mother liquor. That is why chemists often recrystallise a solid two or three times, checking the melting point after each round, until it stops rising or the range narrows to a sharp value — a sign of increasing purity.

Is steam distillation the same as just boiling a mixture with extra water added

No. The key requirement is that the compound is steam-volatile and insoluble in water, so it forms a separate immiscible layer whose vapour pressure adds independently to water's by Dalton's law. Simply adding water to a water-soluble organic liquid would not create two independent vapour pressures; the substance would dissolve into the aqueous phase and not distil over as a separate steam-volatile fraction at all.

How is chromatography different in principle from distillation or crystallisation

Distillation and crystallisation both rely on an equilibrium physical property of the pure substance itself — boiling point or solubility. Chromatography instead relies on how strongly each component interacts with a stationary phase relative to how readily it moves with a mobile phase; components with weaker adsorption or greater partition into the mobile phase simply travel faster, so the separation happens dynamically as the mixture migrates rather than at a single fixed equilibrium point.

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Where this leads