Quick Recap — Concentration Terms

  • Molarity M=mol soluteL solutionM=\dfrac{\text{mol solute}}{\text{L solution}} (temperature-dependent).
  • Molality m=mol solutekg solventm=\dfrac{\text{mol solute}}{\text{kg solvent}}; mole fraction xA=nAnA+nBx_A=\dfrac{n_A}{n_A+n_B} (both temperature-independent).
  • Mass % =mass solutemass solution×100=\dfrac{\text{mass solute}}{\text{mass solution}}\times100; ppm == mg solute per kg solution.
  • Normality == molarity ×\times n-factor. M×V(L)=M\times V(\text{L})= moles.

Beyond-NCERT JEE Formulae

Learn each relation together with when it applies. Unless stated, every colligative formula below assumes a dilute solution of a non-volatile solute.

1. Raoult's law and relative lowering

For a binary mixture of two volatile liquids A and B the total vapour pressure is p=pAxA+pBxBp=p_A^\circ x_A+p_B^\circ x_B, where xAx_A and xBx_B are the mole fractions in the liquid. The vapour is always richer in the more volatile component, with yA=pApy_A=\dfrac{p_A}{p}.

For a non-volatile solute only the solvent evaporates, so the relative lowering of vapour pressure equals the mole fraction of solute: ppp=xsolute\dfrac{p^\circ-p}{p^\circ}=x_{solute} When to use: getting the molar mass of a non-volatile solute from vapour-pressure data. For dilute solutions xsoluten2n1=w2/M2w1/M1x_{solute}\approx\dfrac{n_2}{n_1}=\dfrac{w_2/M_2}{w_1/M_1}.

[JEE Tip] Relative lowering needs no KK constant; it works with mole fraction directly. If the solute dissociates or associates, use in2i\,n_2 in place of n2n_2.

2. Colligative properties (with the van't Hoff factor)

Elevation of boiling point ΔTb=iKbm\Delta T_b=iK_b m, depression of freezing point ΔTf=iKfm\Delta T_f=iK_f m, and osmotic pressure π=iCRT\pi=iCRT with C in mol/L. The molar mass of a non-electrolyte from freezing-point data is M2=Kfw21000ΔTfw1M_2=\dfrac{K_f\,w_2\,1000}{\Delta T_f\,w_1} with the masses in grams. The constants depend only on the solvent: for water Kb=0.52K_b=0.52 and Kf=1.86K_f=1.86 K kg/mol.

[JEE Tip] Osmotic pressure is measurable at very low concentration, so π=iCRT\pi=iCRT gives the most accurate molar masses of proteins and polymers. Two isotonic solutions (equal π\pi) obey i1C1=i2C2i_1C_1=i_2C_2.

3. van't Hoff factor, dissociation and association

The factor compares the real particle count with the formula count: i=observed colligative effectvalue calculated for i=1=normal molar massobserved molar massi=\dfrac{\text{observed colligative effect}}{\text{value calculated for }i=1}=\dfrac{\text{normal molar mass}}{\text{observed molar mass}} For a solute that gives nn particles: dissociation, for example AB to A+ and B- so that n=2n=2, gives α=i1n1\alpha=\dfrac{i-1}{n-1}; association, such as the dimerisation 2A to A2 with n=2n=2, gives α=1i11/n\alpha=\dfrac{1-i}{1-1/n}.

[JEE Tip] Dissociation raises the particle count, so i>1i>1 and the observed molar mass drops below normal; association lowers the count, so i<1i<1 and the observed molar mass rises above normal. Benzoic acid in benzene is the classic dimer, with i0.5i\approx0.5 and an apparent molar mass near 244 g/mol.

4. Henry's law and real solutions

Gas solubility follows p=KHxp=K_H x, where xx is the mole fraction of dissolved gas. A larger KHK_H means a less soluble gas, and KHK_H rises with temperature, so gases are less soluble when hot. For deviations from Raoult's law, a positive deviation (with pp above the Raoult value) comes from weaker solute-solvent forces, as in ethanol and acetone, and gives a minimum-boiling azeotrope; a negative deviation (with pp below the Raoult value) comes from stronger solute-solvent forces, as in acetone and chloroform, and gives a maximum-boiling azeotrope.

[JEE Tip] An ideal solution obeys Raoult's law at every composition with ΔmixH=0\Delta_{mix}H=0 and ΔmixV=0\Delta_{mix}V=0. Azeotropes boil at a fixed temperature and cannot be separated by fractional distillation, a favourite one-mark trap.

Solved Examples — Beyond-NCERT Formulae

Example 1 — Molar mass from freezing-point depression. A 1.00 g sample of a non-volatile, non-electrolyte solute in 50.0 g of benzene lowers the freezing point by 0.40 K, with Kf=5.12K_f=5.12 K kg/mol for benzene. Using M2=Kfw21000ΔTfw1M_2=\dfrac{K_f\,w_2\,1000}{\Delta T_f\,w_1}, M2=5.12×1.00×10000.40×50.0=512020=256M_2=\dfrac{5.12\times1.00\times1000}{0.40\times50.0}=\dfrac{5120}{20}=256 so the molar mass is 256 g/mol.

Example 2 — Molar mass from boiling-point elevation. Dissolving 1.80 g of a non-volatile solute in 100 g of water raises the boiling point by 0.052 K, with Kb=0.52K_b=0.52 K kg/mol for water. Then M2=Kbw21000ΔTbw1=0.52×1.80×10000.052×100=9365.2=180M_2=\dfrac{K_b\,w_2\,1000}{\Delta T_b\,w_1}=\dfrac{0.52\times1.80\times1000}{0.052\times100}=\dfrac{936}{5.2}=180 so the molar mass is 180 g/mol, matching glucose.

Example 3 — Osmotic pressure and molar mass. A 1.0 g sample of a polymer in 100 mL of aqueous solution has an osmotic pressure of 4.926×1034.926\times10^{-3} atm at 300 K, with R=0.0821R=0.0821 L atm/mol/K. From π=wM2VRT\pi=\dfrac{w}{M_2 V}RT, rearrange to M2=wRTπVM_2=\dfrac{wRT}{\pi V}: M2=1.0×0.0821×3004.926×103×0.100=24.634.926×104=5.0×104M_2=\dfrac{1.0\times0.0821\times300}{4.926\times10^{-3}\times0.100}=\dfrac{24.63}{4.926\times10^{-4}}=5.0\times10^{4} The molar mass is 5.0×1045.0\times10^{4} g/mol; the tiny yet measurable osmotic pressure is exactly why osmometry suits macromolecules.

Example 4 — van't Hoff factor and percent dissociation. A 0.10 m aqueous solution of a weak binary electrolyte, which ionises as AB to A+ and B- so that n=2n=2, shows an observed freezing-point depression of 0.279 K, with Kf=1.86K_f=1.86 K kg/mol. First the van't Hoff factor, i=ΔTfKfm=0.2791.86×0.10=1.5i=\dfrac{\Delta T_f}{K_f\,m}=\dfrac{0.279}{1.86\times0.10}=1.5. Then the degree of dissociation from α=i1n1\alpha=\dfrac{i-1}{n-1}, α=1.5121=0.5\alpha=\dfrac{1.5-1}{2-1}=0.5 so the electrolyte is 50 percent dissociated.

Example 5 — Association of a dimer (benzoic acid). 2.44 g of benzoic acid (normal molar mass 122 g/mol) in 50 g of benzene gives an observed freezing-point depression of 1.024 K, with Kf=5.12K_f=5.12 K kg/mol; in benzene the acid dimerises, 2A to A2, so n=2n=2. The moles of acid are 2.44122=0.0200\dfrac{2.44}{122}=0.0200 and the molality is 0.02000.050=0.400\dfrac{0.0200}{0.050}=0.400 mol/kg, so the depression expected without association is ΔTf(calc)=Kfm=5.12×0.400=2.048\Delta T_f(\text{calc})=K_f m=5.12\times0.400=2.048 K. Hence i=ΔTf(obs)ΔTf(calc)=1.0242.048=0.50i=\dfrac{\Delta T_f(\text{obs})}{\Delta T_f(\text{calc})}=\dfrac{1.024}{2.048}=0.50 The degree of association is α=1i11/n=10.5011/2=1.0\alpha=\dfrac{1-i}{1-1/n}=\dfrac{1-0.50}{1-1/2}=1.0, i.e. essentially complete dimerisation, and the apparent molar mass is 1220.50=244\dfrac{122}{0.50}=244 g/mol, twice the monomer value.

Example 6 — Two-component Raoult's law. An ideal solution is made from 2 mol of liquid A (with pA=100p_A^\circ=100 torr) and 3 mol of liquid B (with pB=60p_B^\circ=60 torr) at 300 K. The liquid mole fractions are xA=25=0.40x_A=\dfrac{2}{5}=0.40 and xB=0.60x_B=0.60, so the total vapour pressure is p=pAxA+pBxB=100×0.40+60×0.60=40+36=76p=p_A^\circ x_A+p_B^\circ x_B=100\times0.40+60\times0.60=40+36=76 that is 76 torr. The vapour mole fraction of A is yA=pAp=4076=0.53y_A=\dfrac{p_A}{p}=\dfrac{40}{76}=0.53, confirming the vapour is richer than the liquid in the more volatile component A.

Example 7 — Relative lowering of vapour pressure. At a fixed temperature the vapour pressure of pure water is 25.0 torr and falls to 24.0 torr when 12.5 g of a non-volatile solute is dissolved in 90 g of water. The relative lowering equals the solute mole fraction, x2=ppp=25.024.025.0=0.040x_2=\dfrac{p^\circ-p}{p^\circ}=\dfrac{25.0-24.0}{25.0}=0.040. With water n1=9018=5.00n_1=\dfrac{90}{18}=5.00 mol, and since x2=n2n1+n2x_2=\dfrac{n_2}{n_1+n_2}, rearranging gives n2=n1x21x2=5.00×0.0400.96=0.2083n_2=\dfrac{n_1 x_2}{1-x_2}=\dfrac{5.00\times0.040}{0.96}=0.2083 mol. Hence M2=w2n2=12.50.2083=60M_2=\dfrac{w_2}{n_2}=\dfrac{12.5}{0.2083}=60 so the molar mass is 60 g/mol, matching urea.

Example 8 — Henry's law solubility. For carbon dioxide in water at 298 K the Henry constant is KH=2.0×103K_H=2.0\times10^{3} bar. To find the dissolved amount in 1 kg of water when the partial pressure of carbon dioxide is 4.0 bar, use p=KHxp=K_H x to get x=pKH=4.02.0×103=2.0×103x=\dfrac{p}{K_H}=\dfrac{4.0}{2.0\times10^{3}}=2.0\times10^{-3}. In 1 kg of water there are n1=100018=55.6n_1=\dfrac{1000}{18}=55.6 mol, so the dissolved amount is nxn1=2.0×103×55.6=0.11n\approx x\,n_1=2.0\times10^{-3}\times55.6=0.11 mol, that is 0.11×44=4.90.11\times44=4.9 grams of carbon dioxide per kilogram of water.