Chem notesPhysicalGases & Liquids

Independent topic page

Gaseous & Liquid States

Identify ideal, mixture, kinetic-theory or real-gas mode in 12 seconds; then one state equation plus a physical limit check controls the stem.

Portion PhysicalFocus High-return numericals when state equations, partial pressures and molecular speeds stay separatedTarget 45–75sPortion share 49.8%Trend Falling share
The paper mixes macroscopic P–V–T data with molecular speeds and non-ideality. Never splice formulas from different models without checking whether pressure is total or partial and whether the same T and molar mass apply. Name the speed type before opening a formula sheet — most kinetic-theory errors are label errors, not algebra errors.

How Advanced asks this

  • Gas collected over water or reacting gas mixture
  • Density/molar-mass determination under non-STP conditions
  • Compare v_mp, v_avg, v_rms, kinetic energy or effusion rates
  • van der Waals constants, compressibility factor and limiting behaviour
  • Intermolecular-force effects on vapour pressure, boiling point, viscosity and surface tension

Traps that leak marks

  • Using total pressure for gas collected over water
  • Putting molar mass in g mol⁻¹ into SI speed formula
  • Assuming equal speeds because kinetic energies are equal
  • Calling every Z<1 gas ideal-like
  • Including condensed water in Dalton's gas total
  • Using wet-gas total pressure as dry P
  • Putting M in g mol⁻¹ into SI speed formulas
  • Assuming equal speeds because mean KE is equal

01. PV=nRT is a model whose strongest domain is low pressure and high temperature; van der Waals corrections explain finite molecular size (b) and attractions (a).

02. Dalton works with gas-phase partial pressures. Vapour collected over liquid requires subtracting that liquid's equilibrium vapour pressure.

03. Speed order is v_mp < v_avg < v_rms for one gas at one temperature; every characteristic speed scales as √(T/M). Diffusion/effusion follows Graham’s square-root mass law.

04. Official syllabus also tests intermolecular interactions: type, distance dependence, and effect on properties. Stronger cohesion generally lowers vapour pressure and raises boiling point, viscosity and surface tension.

05. Pick one model and stay inside it: ideal P–V–T, Dalton partial pressures, kinetic speeds, or van der Waals — hybrid formulas without matching assumptions lose marks.

06. Gas collected over water is never total pressure of the dry gas; subtract the liquid’s vapour pressure before using PV=nRT.

07. Liquid-property trends are intermolecular-force stories: stronger cohesion lowers vapour pressure and raises boiling point, viscosity and surface tension.

Official · 2026

Syllabus for this topic

Official syllabus points for Gaseous & Liquid States only — not the full Physical portion map. Portion hub: Physical · Physical analysis.

Syllabus on this page is topic-scoped: States of Matter: Gases and Liquids. The parent portion (Physical) also covers other topics — use the portion hub for the full map.

Must cover (this topic)

  • Zero/first order kinetics + Arrhenius

Gaps / watch-outs

No topic-specific exclusions flagged — finish the unit points below for Gases & Liquids.

Source: https://jeeadv.ac.in/documents/jee-advanced-2026-syllabus.pdf

Unit 01

States of Matter: Gases and Liquids

medium

Exam focusvan der Waals, rms velocities, vapour pressure/viscosity ideas.

Syllabus points

  • Gas laws; ideal gas; absolute temperature; van der Waals; kinetic theory velocities
  • Partial pressures; diffusion
  • Intermolecular interactions; liquids: vapour pressure, surface tension, viscosity

Do / check

  • Relate <v>, v_rms, v_mp to T before plugging numbers

Full Chemistry syllabus →

Cross-topic stems

Mixed joins for this topic

Advanced rarely asks a chapter in isolation. These are tagged multi-idea Chemistry stems that touch Gaseous & Liquid States — practise the knowledge bridge, not only the single-chapter drill.

Chemistry2026 · Paper 2 · Q15–Q16linked-numerical

Ideal solution molar volumes + vapour mole fraction

Solutions – colligative / ideal+Raoult’s law+Vapour–liquid composition

Knowledge bridge

Step 1: from the linked ideal-solution data, compute the vapour-to-liquid molar volume ratio for pure B. Step 2: find liquid mole fractions (e.g. from molality). Step 3: apply Raoult to get y_B in the vapour (numerical ~0.16 style).

Why it feels hard

Two numericals share solution data; unit slips (molality vs mole fraction) are common.

What to practise

Convert every molality stem to x_i before touching vapour pressures.

Chemistry2020 · Paper 1 · Q16–Q17numerical

Physical mixed numerical pair

Physical – Mixed+Mole / gas / thermo blend+Numerical

Knowledge bridge

Step 1: parse which Physical sub-ideas are fused (mole + thermo, gas + equilibrium, etc.). Step 2: write governing equations for each piece. Step 3: combine numerically without dropping stoichiometric factors.

Why it feels hard

‘Mixed’ Physical tags mean the stem will not stay in one textbook chapter.

What to practise

Practise deliberately cross-chapter Physical sets (thermo×gases×equilibrium).

All mixed joins →

Why methods matter

Common methods that change your score

Gas and liquid questions are bookkeeping problems once partial pressure, molar volume and phase composition are separated.

01

Partial-pressure inventory

Dalton applies to what remains in the gas phase, not blindly to initial labels.

Do thisConvert each gas to moles, remove reacted/condensed species, then calculate p_i.

Why it works

Dalton applies to what remains in the gas phase, not blindly to initial labels.

See it once

Wet gas: P_dry=P_total−P_H₂O before using PV=nRT for dry-gas moles.

02

Ratio before constants

Cancels units and exposes √T/M scaling directly.

Do thisDivide two gas-state or speed equations before substituting R.

Why it works

Cancels units and exposes √T/M scaling directly.

See it once

v_rms(A)/v_rms(B)=√(T_A M_B/(T_B M_A)).

03

Z-sign diagnosis

Attraction lowers observed P (Z<1); hard-core repulsion dominates high P (Z>1).

Do thisAt moderate P ask whether attraction or excluded volume dominates.

Why it works

Attraction lowers observed P (Z<1); hard-core repulsion dominates high P (Z>1).

See it once

A negative deviation cannot be explained by b alone; it signals net attractive correction.

04

Property-force map

One causal map replaces disconnected memorisation.

Do thisTranslate liquid trend to intermolecular forces before ranking.

Why it works

One causal map replaces disconnected memorisation.

See it once

Stronger cohesion generally lowers vapour pressure and raises boiling point, viscosity and surface tension.

Processed examples

Sample questions · full working

Read the impact line first. Then notice which family/model was chosen. The solution is written the way your rough sheet should look in the hall.

01

bankFamily · Gas mixture and partial pressure

Sample question

2 mol N₂ and 3 mol H₂ occupy a vessel at total pressure 10 bar. Find p(H₂).

This stem rewards early recognition of the gas mixture and partial pressure model.

Model chosenApply Dalton’s law.

Processed solution

  1. Total moles=5.
  2. x(H₂)=3/5.
  3. p(H₂)=xP=6 bar.

Answer6 bar

Takeaway: Partial pressure follows mole fraction.

02

standardFamily · Kinetic theory and effusion

Sample question

Find r(H₂)/r(O₂) when H₂ is at 300 K and O₂ at 1200 K.

This stem rewards early recognition of the kinetic theory and effusion model.

Model chosenUse r∝√(T/M).

Processed solution

  1. Form the ratio √[(300/2)/(1200/32)].
  2. The quantity inside the root is 4.
  3. Therefore the rate ratio is 2.

Answer2

Takeaway: Temperature and molar mass enter under one square root.

03

twistFamily · Real-gas equation

Sample question

One mole of a van der Waals gas is at its critical point. Express Zc using the van der Waals critical constants.

This Advanced-level variation couples hidden constraints with the real-gas equation model.

Model chosenInsert Pc, Vc and Tc into Z=PV/RT.

Processed solution

  1. For a van der Waals gas, Vc=3b.
  2. Pc=a/(27b²) and Tc=8a/(27Rb).
  3. Zc=PcVc/(RTc).
  4. Substitution gives [a/(27b²)](3b)/[8a/(27b)].
  5. Hence Zc=3/8.

Answer3/8

Takeaway: Critical constants collapse dimensionless expressions.

Reusable models

Common question families

Advanced stems cluster. Name the family in 10–15s, write the fast model, then run the same path. Do not invent a new plan each time.

01

Gas mixture and partial pressure

Looks likeSeveral gases mixed, collected over water or selectively removed

Fast modelUse mole bookkeeping with Dalton’s law.

Same solve path

  1. Find each gas mole count.
  2. Subtract reacted or absorbed gas.
  3. Compute total moles.
  4. Use pᵢ=xᵢP.

Rough skeleton

  • mole table
  • xᵢ
  • pᵢ

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

02

Real-gas equation

Looks likevan der Waals constants, compression factor or critical data

Fast modelInsert molar volume consistently before interpreting deviation.

Same solve path

  1. Choose ideal or van der Waals model.
  2. Convert to molar volume.
  3. Solve for P, V or Z.
  4. Check units and limiting behavior.

Rough skeleton

  • equation
  • Vₘ
  • Z/result

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

03

Kinetic theory and effusion

Looks likeRMS speed, temperature change or porous-wall escape

Fast modelCompare squared speeds or use Graham’s square-root ratio.

Same solve path

  1. Identify the required speed/rate relation.
  2. Form a ratio to cancel constants.
  3. Insert molar masses and temperatures.
  4. Check lighter gas is faster.

Rough skeleton

  • ratio law
  • substitution
  • sense check

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

04

Liquid vapour and colligative behavior

Looks likeVapour pressure, boiling point or nonvolatile solute

Fast modelWork with mole fraction and relative lowering.

Same solve path

  1. Find liquid-phase mole fractions.
  2. Apply Raoult’s law.
  3. Sum partial pressures if volatile.
  4. Relate to the requested property.

Rough skeleton

  • xᵢ
  • pᵢ=xᵢpᵢ°
  • total/result

Why faster

Recognition fixes the model before arithmetic begins.

Refuse this

Do not start blind expansion or casework before identifying the governing model.

Hall timing

45–75s process

  1. 0–12s
    Classify: ideal state, Dalton mixture, kinetic speed, effusion, real gas, or liquid-property trend.

    Underline data, units, phase/standard-state labels and the exact quantity asked. Reject any formula whose assumptions are already violated.

  2. 12–25s
    Write partial pressures/moles and choose PV=nRT, speed scaling, Graham, or van der Waals—not a hybrid.

    Write the governing relation symbolically before substitution; define one basis, reference state, or extent variable if the stem mixes quantities.

  3. 25–60s
    Solve in absolute temperature with consistent R units; use mole fractions before partial pressures.

    Keep ratios and logarithms exact as long as possible. Carry signs, powers of ten and units on the rough sheet instead of repairing them later.

  4. 60–75s
    Check P,V,T limits, Σp_i=P, speed dimensions, and whether attractions should make Z below or above unity.

    Check dimensions, limiting cases and chemical sense. For multi-correct, test every option independently rather than forcing one common conclusion.

After the model is locked

Quick formula bank

Ideal gas

PV=nRT; ρ=PM/RT

Dilute gas and molar-mass/density stems

Dalton law

P=Σp_i; p_i=x_iP=n_iRT/V

Non-reacting ideal-gas mixtures

Molecular speeds

v_mp=√(2RT/M); v_avg=√(8RT/πM); v_rms=√(3RT/M)

Speed comparison; M in kg mol⁻¹ for SI speed

Mean translational energy

Ē_trans=(3/2)RT per mole; (3/2)k_BT per molecule

Ideal-gas molecular energy at T

Graham law

r₁/r₂=√(M₂/M₁)=√(ρ₂/ρ₁) at same T,P

Effusion/diffusion comparison

van der Waals

(P+a n²/V²)(V−nb)=nRT

Attraction and excluded-volume corrections

Compressibility

Z=PV/(nRT); Z→1 as P→0

Measure and direction of non-ideality

Clausius–Clapeyron

ln(P₂/P₁)=−ΔH_vap/R(1/T₂−1/T₁)

Approximate vapour-pressure change over a modest range

Mental bank

  • Use kelvin only
  • At fixed T,V: P∝n
  • p_i=x_iP
  • v_mp:v_avg:v_rms = √2:√(8/π):√3
  • All ideal gases at same T have same mean translational energy
  • a measures attraction; b measures excluded volume
  • Stronger liquid forces: lower vapour pressure, higher boiling point
  • Always convert T to kelvin
  • p_i = x_i P_total for ideal mixtures
  • v_mp < v_avg < v_rms; all ∝ √(T/M)
  • a tracks attraction; b tracks excluded volume

Make it automatic

Practice · checklist

Daily

  • Two gas-mixture pressure tables and two speed-ratio mental calculations.
  • One statement set on Z, a/b, vapour pressure or viscosity.

Weekly

  • Timed mixed set joining stoichiometry with Dalton and condensation.
  • Plot and explain one qualitative Z–P curve without notes.

100% checklist

  • Temperature converted to kelvin
  • Pressure identified as total, dry or partial
  • Gas-phase species inventoried after reaction
  • Correct R and molar-mass units used
  • Speed type named before formula
  • Real-gas limit checked
  • Liquid trend justified through intermolecular forces
  • Pressure type identified: total, dry or partial
  • Correct R and molar-mass units
  • Model assumptions match the stem