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Kinetic Theory of Gases flash cards

Master Kinetic Theory of Gases through 93 JEE Advanced-level recall cards, systematically structured one idea at a time. Revise concept-wise, identify the areas where you need improvement, and focus your preparation with greater precision.

Kinetic Theory of Gases, question and answer

19 of this chapter's 93 cards, laid out open so you can read straight through. The remaining 74 are in the interactive deck, where the answer stays hidden until you commit to one.

  1. 1.State the basic assumption of kinetic theory about the size of gas molecules.

    A gas consists of a very large number of identical molecules whose actual volume is negligible compared to the total volume of the container. Molecules are treated as point particles.

    Hint: Molecular size vs container size.

  2. 2.According to kinetic theory, how do molecules of an ideal gas interact?

    Molecules exert no force on each other except during collisions. There is no intermolecular potential energy, so the total internal energy is purely kinetic.

    Hint: No forces between collisions.

  3. 3.What is assumed about collisions of gas molecules in kinetic theory?

    Collisions (molecule–molecule and molecule–wall) are perfectly elastic and of negligible duration compared with the time between collisions. Kinetic energy and momentum are conserved.

    Hint: Elastic, instantaneous.

  4. 4.How do molecules move between collisions according to kinetic theory?

    Between collisions molecules move in straight lines with constant velocity (no external force, gravity neglected). Directions are random and uniformly distributed.

    Hint: Straight-line free flight.

  5. 5.What does 'molecular chaos' / random motion assumption mean?

    At any instant molecular velocities are distributed randomly in all directions; there is no preferred direction, so the average velocity vector is zero even though the average speed is not.

    Hint: v=0\langle \vec v\rangle = 0, v0\langle v\rangle \neq 0.

  6. 6.Why is vx2=vy2=vz2\langle v_x^2\rangle = \langle v_y^2\rangle = \langle v_z^2\rangle for a gas?

    By isotropy (no preferred direction), each component contributes equally. Since v2=vx2+vy2+vz2\langle v^2\rangle = \langle v_x^2\rangle + \langle v_y^2\rangle + \langle v_z^2\rangle, each equals 13v2\frac13\langle v^2\rangle.

    Hint: Equal sharing among 3 axes.

  7. 7.Write the kinetic theory expression for pressure of an ideal gas in terms of density.

    P=13ρv2P = \dfrac13 \rho\, \overline{v^2}, where ρ\rho is the gas density and v2\overline{v^2} is the mean square speed of the molecules.

    Hint: One-third rho v-squared.

  8. 8.Write the pressure expression in terms of number of molecules NN, mass mm, and volume VV.

    P=13NmVv2=13nmv2P = \dfrac{1}{3}\dfrac{N m}{V}\,\overline{v^2} = \dfrac13\, n\, m\, \overline{v^2}, where n=N/Vn=N/V is number density.

    Hint: ρ=Nm/V\rho = Nm/V.

  9. 9.In deriving P=13ρv2P=\frac13\rho\overline{v^2}, what is the change in momentum when one molecule hits a wall elastically?

    For a wall perpendicular to xx, momentum change per collision is Δp=2mvx\Delta p = 2 m v_x (the xx-component reverses; y,zy,z unchanged).

    Hint: Reverses vxv_x.

  10. 10.Why does the factor 13\frac13 appear in the pressure formula?

    Only the velocity component perpendicular to the wall causes pressure. Because vx2=13v2\overline{v_x^2}=\frac13\overline{v^2} by isotropy, the 13\frac13 enters the final expression.

    Hint: One of three components hits the wall.

  11. 11.Relate pressure to the average translational kinetic energy per unit volume.

    P=23(NV)EP = \dfrac23\left(\dfrac{N}{V}\right)\overline{E} where E=12mv2\overline{E}=\frac12 m\overline{v^2}. So P=23×P=\frac23 \times (translational KE per unit volume).

    Hint: P=23nEP=\frac23 n\overline E.

  12. 12.State the ideal gas equation in terms of moles.

    PV=nRTPV = nRT, where nn is number of moles, R=8.314J mol1K1R=8.314\,\text{J mol}^{-1}\text{K}^{-1} is the universal gas constant, and TT is absolute temperature.

    Hint: Moles form.

  13. 13.State the ideal gas equation in terms of number of molecules.

    PV=NkBTPV = N k_B T, where NN is the number of molecules and kBk_B is the Boltzmann constant.

    Hint: Molecule form uses kBk_B.

  14. 14.How are RR, kBk_B and Avogadro number NAN_A related?

    kB=RNAk_B = \dfrac{R}{N_A}, so kB=8.3146.022×10231.38×1023J K1k_B = \dfrac{8.314}{6.022\times10^{23}} \approx 1.38\times10^{-23}\,\text{J K}^{-1}.

    Hint: Gas constant per molecule.

  15. 15.What is the physical meaning of the Boltzmann constant kBk_B?

    kBk_B is the gas constant per molecule; it links the average thermal energy of a particle to temperature: energy per degree of freedom =12kBT=\frac12 k_B T.

    Hint: Energy scale of temperature.

  16. 16.By combining P=13NmVv2P=\frac13\frac{Nm}{V}\overline{v^2} with PV=NkBTPV=Nk_BT, derive the kinetic interpretation of temperature.

    13mv2=kBT12mv2=32kBT\frac13 m\overline{v^2} = k_B T \Rightarrow \frac12 m\overline{v^2} = \frac32 k_B T. Average translational KE per molecule =32kBT=\frac32 k_BT.

    Hint: Equate the two expressions for PVPV.

  17. 17.What is the average translational kinetic energy of a gas molecule?

    Etrans=32kBT\overline{E}_{trans} = \dfrac32 k_B T. It depends only on temperature, not on the mass or nature of the gas.

    Hint: Three-halves kBTk_BT.

  18. 18.What is the total translational kinetic energy of one mole of an ideal gas?

    E=32NAkBT=32RTE = \dfrac32 N_A k_B T = \dfrac32 R T per mole (translational only).

    Hint: Multiply per-molecule value by NAN_A.

  19. 19.State the kinetic interpretation of temperature in words.

    Absolute temperature is a direct measure of the average translational kinetic energy of the molecules of a gas. Higher TT means faster mean-square molecular motion.

    Hint: TEtransT \propto \overline{E}_{trans}.

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