Close the Notes. Start the Clock.

Sections 1 to 12 taught you this chapter: the atomic hypothesis, the ideal gas equation in all four of its forms, Boyle's law and Charles' law and the pressure law, the assumptions of kinetic theory and the pressure derivation built on them, what temperature actually is, the three molecular speeds and the distribution they come from, degrees of freedom, equipartition, the molar specific heats, the mean free path, and an advanced toolkit on top of all of it.

This section asks one different question: can you use any of it with a timer running?

There is no new theory below. There are 30 single-correct questions built to the exam pattern, and a marking scheme designed to punish the four habits this chapter rewards most cruelly: leaving a molar mass in grams per mole inside a speed formula, reaching for vˉ\bar{v} where vrmsv_{rms} belongs, dropping the 2\sqrt{2} out of the mean free path, and squaring a radius that the question meant you to double first.

The rules of engagement

Key Point: This is not a reading exercise. Blank sheet, pen, timer. Attempt all 30 questions in one unbroken sitting, and do not open a single explanation until the last answer is written.

Topic spread of the thirty questions, the marking scheme and guessing odds

The setup What it is
Number of questions 30, single correct option
Marking scheme +4+4 correct, 1-1 incorrect, 00 unattempted
Maximum score 30×4=12030 \times 4 = 120 marks
Minimum possible score 30×(1)=3030 \times \left(-1\right) = -30 marks
Suggested time limit 50 minutes (a shade over a minute and a half per question)
Take 0°C0°C as 273 K throughout
Allowed rough sheet, your own head
Not allowed calculator, formula sheet, a glance back at the earlier sections

Everything in this drill sits inside the JEE Main syllabus for kinetic theory; the two or three items marked Advanced in their tags go a step past it and are there to stretch you, not to scare you.

Notation

Several of the traps below turn on it.

Key Point: In kinetic theory nn is the number density - molecules per cubic metre, n=NVn = \frac{N}{V} - and μ\mu is the number of moles. The previous chapter used nn for moles; this is the reverse, and it is the convention every formula here follows. So the gas equation is PV=μRTPV = \mu RT and P=nkBTP = nk_BT, and the heat at constant volume is ΔQ=μCvΔT\Delta Q = \mu C_v \Delta T.

The rest of the alphabet, fixed for all 30 questions:

  • NN is the number of molecules and NAN_A the Avogadro number, so μ=NNA=MM0\mu = \frac{N}{N_A} = \frac{M}{M_0}. The one exception is the 3N3N degrees-of-freedom rule, where NN counts the atoms inside one molecule; the rule itself always says so.
  • M0M_0 is the molar mass in kilograms per mole, m=M0NAm = \frac{M_0}{N_A} is the mass of one molecule in kilograms, and MM is the total mass of the sample. Three symbols, three different things.
  • TT is always an absolute temperature in kelvin. A Celsius value is written tt or tCt_C.
  • ff is the number of quadratic terms per molecule (loosely, degrees of freedom). Where a collision frequency turns up in the same question it is called ν\nu, never ff.
  • CpC_p and CvC_v are molar specific heats in J/(mol K); lower-case cpc_p and cvc_v are per kilogram. γ=CpCv=1+2f\gamma = \frac{C_p}{C_v} = 1 + \frac{2}{f}.
  • EE is the translational kinetic energy only; UU is the whole internal energy. They agree for a monatomic gas and for nothing else.
  • v2\overline{v^2} is the mean of the squares and vˉ\bar{v} the mean speed. v2\overline{v^2} is not (vˉ)2\left(\bar{v}\right)^2.

The constants sheet

Every question that needs a number uses these and no others. Copy them to the top of your sheet before you start.

Quantity Value
Universal gas constant RR 8.3148.314 J/(mol K)
Boltzmann constant kBk_B 1.38×10231.38 \times 10^{-23} J/K
Avogadro number NAN_A 6.022×10236.022 \times 10^{23} per mol
1 atm 1.013×1051.013 \times 10^{5} Pa
Molar volume at STP 22.4 L
CvC_v, monatomic 32R=12.47\frac{3}{2}R = 12.47 J/(mol K)
CvC_v, rigid diatomic 52R=20.79\frac{5}{2}R = 20.79 J/(mol K)
CvC_v, rigid non-linear polyatomic 3R=24.943R = 24.94 J/(mol K)
γ\gamma: monatomic, rigid diatomic, rigid non-linear polyatomic 53\frac{5}{3}, 75\frac{7}{5}, 43\frac{4}{3}
Molar masses (g/mol) H2_2 2, He 4, N2_2 28, O2_2 32, Ar 40, CO2_2 44
Useful roots 2=1.414\sqrt{2} = 1.414, 3=1.732\sqrt{3} = 1.732, 10=3.162\sqrt{10} = 3.162, 8π=1.596\sqrt{\frac{8}{\pi}} = 1.596

The constants used throughout this drill. Nothing else is needed.

The three formulas that decide the most marks

vmp=2RTM0  <  vˉ=8RTπM0  <  vrms=3RTM0v_{mp} = \sqrt{\frac{2RT}{M_0}} \; < \; \bar{v} = \sqrt{\frac{8RT}{\pi M_0}} \; < \; v_{rms} = \sqrt{\frac{3RT}{M_0}}

l=12nπd2=kBT2πd2P,ν=vˉll = \frac{1}{\sqrt{2}\,n\pi d^2} = \frac{k_BT}{\sqrt{2}\,\pi d^2 P}, \qquad \nu = \frac{\bar{v}}{l}

Cv=f2R,Cp=Cv+R,γ=1+2fC_v = \frac{f}{2}R, \qquad C_p = C_v + R, \qquad \gamma = 1 + \frac{2}{f}

In the first line M0M_0 is in kilograms per mole. In the second, dd is the molecular diameter, and the 2\sqrt{2} is not optional. In the third, ff counts quadratic terms, so a vibrational mode contributes 2 and a rotational degree of freedom only 1.

What this set covers

Topic Questions How many
The ideal gas equation, its four forms and Dalton's law Q1 to Q5 5
The pressure derivation and its consequences Q6 to Q8 3
Temperature, kinetic energy and vrmsv_{rms} Q9 to Q12 4
The Maxwell distribution and the three speeds Q13 to Q16 4
Degrees of freedom, linear against non-linear Q17 to Q19 3
Equipartition and internal energy Q20 to Q21 2
CvC_v, CpC_p and γ\gamma Q22 to Q24 3
Gas mixtures Q25 to Q26 2
Mean free path and collision frequency Q27 to Q29 3
Graham's law of diffusion Q30 1

That spread mirrors how the paper actually samples this chapter. Speeds, specific heats and the mean free path together carry 19 of the 30, because those are the blocks that carry the multi-step questions, and therefore the marks.

The difficulty mix is roughly 25% easy, 45% medium and 30% hard. A handful will feel brutal. They are meant to.

[Exam Tip] That 1-1 changes the arithmetic of guessing. A blind guess among four options returns 443×14=+0.25\frac{4}{4} - \frac{3 \times 1}{4} = +0.25 marks on average, barely worth the minute it costs. A question narrowed to two options returns 412=+1.50\frac{4 - 1}{2} = +1.50 marks on average, six times as much. Narrow first, then commit. Leave blank only what you could not narrow at all.

[Exam Tip] Before you start, write five lines at the top of your sheet: kelvin, not Celsius?, is M0M_0 in kg/mol?, which of the three speeds does this want?, diameter or radius?, did I keep the 2\sqrt{2}? Those five questions catch the overwhelming majority of the marks lost in this chapter.

Scoring Yourself Honestly

Mark your sheet with the real scheme, +4+4 and 1-1 and 00, and total it. No half marks for "I knew that one really". The number you get is the number that matters.

Four score bands beside the five standing traps and the damage each does

The bands

Your score (out of 120) Verdict What to do next
96 to 120 Exam ready. 80% or more on a hard set, inside the time. Move on. This chapter will not cost you marks. Revisit only the specific items you missed.
72 to 95 Solid, but leaking marks. Almost always slips rather than gaps: a molar mass left in grams, a mean speed where an rms speed belonged, a radius squared without being doubled. Redo every wrong question without the explanation first.
42 to 71 Shaky. The ideas are there; the execution is not. For each wrong answer go back to the section that owns it (use the topic table above) and rework its solved examples before re-attempting.
Below 42 Start again. Work Sections 1 to 10 properly, then Section 11's worked problems, then Section 12. Re-attempting this set now teaches you nothing but the answer key.

Read your own answer sheet

Before you touch a single explanation, sort your mistakes into three piles. This is the most valuable ten minutes in the whole section.

  1. Method errors. You used vˉ\bar{v} where the physics wanted vrmsv_{rms}, or the other way round. You counted a linear triatomic as though it had 3 rotational degrees of freedom. You applied a formula for one molecule to a whole mole, or a molar specific heat to one molecule. You put a Celsius temperature into a ratio. These are the expensive ones, because the whole solution is wrong from line one.
  2. Execution errors. Right method, wrong arithmetic. The classic four here: 3232 substituted where 0.0320.032 belonged; the 2\sqrt{2} dropped out of the mean free path; a radius squared without being doubled into a diameter first; litres left unconverted inside PV=μRTPV = \mu RT.
  3. Reading errors. The question asked for the most probable speed, not the rms one. For the internal energy, not the translational kinetic energy. For CpC_p, not CvC_v. For the number of molecules, not the number of moles. For the collision time, not the collision frequency. For the gas that diffuses slower, not faster.

Key Point: In this chapter pile 2 is unusually fat, because the chapter's four standing traps are all pure execution: grams for kilograms, mean speed for rms speed, radius for diameter, and the missing 2\sqrt{2}. Two of them wreck the answer so badly you would notice; two of them leave a number that still looks perfectly reasonable. Those two are the ones that cost marks.

How badly each trap hurts

The slip What it does to your answer
nn read as moles instead of molecules per cubic metre out by a factor of 6×10236 \times 10^{23}
M0M_0 left in g/mol inside a speed formula out by 1000=31.6\sqrt{1000} = 31.6
A radius used directly as dd in the mean free path ll comes out 4 times too large
The 2\sqrt{2} dropped from the mean free path ll comes out 1.411.41 times too large
vˉ\bar{v} used where vrmsv_{rms} belongs out by 3π8=1.09\sqrt{\frac{3\pi}{8}} = 1.09

The last two are the dangerous ones. Nobody ships an answer that is 102310^{23} times too big; everybody ships one that is 9% off.

The eight habits this set is drilling

  • Write the molar mass in kg/mol on its own line, every single time. 3232 g/mol becomes 0.0320.032 kg/mol before it goes anywhere near a square root. If your rms speed comes out around 15 m/s instead of 480, this is why.
  • Name the speed before you compute it. Energies and pressures want vrmsv_{rms}. Mean free paths, collision frequencies and effusion want vˉ\bar{v}. The peak of the distribution is vmpv_{mp}. The order never changes: vmp<vˉ<vrmsv_{mp} < \bar{v} < v_{rms}, in the ratio 2:8π:3\sqrt{2} : \sqrt{\frac{8}{\pi}} : \sqrt{3}.
  • Count ff before you write any specific heat. Monatomic 3, rigid diatomic 5, rigid linear polyatomic 5, rigid non-linear polyatomic 6, vibrating diatomic 7. Then Cv=f2RC_v = \frac{f}{2}R and γ=1+2f\gamma = 1 + \frac{2}{f} hand you everything else.
  • Carbon dioxide is linear. It behaves like a diatomic, not like water vapour. Getting this wrong changes γ\gamma from 1.401.40 to 1.331.33 and every downstream number with it.
  • Keep EE and UU apart. E=32μRTE = \frac{3}{2}\mu RT is translational only, whatever the gas. U=f2μRTU = \frac{f}{2}\mu RT is the whole thing. They coincide only when f=3f = 3.
  • In the mean free path, check two things before you divide: is dd a diameter, and is the 2\sqrt{2} still there? l=12nπd2l = \frac{1}{\sqrt{2}\,n\pi d^2}, and nothing else.
  • Scale rather than recompute. lTPl \propto \frac{T}{P}, νPT\nu \propto \frac{P}{\sqrt{T}}, vTM0v \propto \sqrt{\frac{T}{M_0}}. Most of the multi-step questions in this set fall in one line to a proportionality and in five lines to brute force.
  • Sanity-check every speed against room temperature. At 300 K, hydrogen is around 1900 m/s, helium around 1400, nitrogen and oxygen around 500, carbon dioxide around 400. An answer of 15 or of 15000 is a units error, not a discovery.

[Exam Tip] Every explanation below is a full step-by-step solution, so this set doubles as revision. Read the explanation even for the questions you got right - several of these have a two-line route and a two-page route, and it is the two-line route you will need in the hall.