NCERT Solutions for Class 11 Physics Chapter 12 – Kinetic Theory

Kinetic Theory is a conceptual and scoring chapter in Class 11 Physics that explains the microscopic behavior of gases. This chapter covers important topics such as kinetic theory of gases, assumptions of the model, pressure of a gas, kinetic energy of molecules, degrees of freedom, law of equipartition of energy, specific heat capacities, and mean free path, which are frequently tested in school exams and competitive exams like JEE and NEET.

NCERT Solutions for Class 11 Physics Chapter 12 – Kinetic Theory are prepared strictly according to the latest CBSE syllabus and exam pattern. The solutions are written in simple, step-by-step language with clear derivations, graphs, and solved numericals, helping students develop strong conceptual clarity and score well in Class 11 examinations.

NCERT Solutions for Class 11 Physics Chapter 12 – Kinetic Theory

NCERT Solutions for Class 11 Physics Chapter 12 – Kinetic Theory

1) Q. Estimate the fraction of molecular volume to the actual volume occupied by oxygen gas at STP. Take the diameter of an oxygen molecule to be 3 Å.

Answer:
Diameter

d=3 A˚r=1.5×1010 md = 3\ \text{Å} \Rightarrow r = 1.5\times10^{-10}\ \text{m}


Volume of one molecule:

v=43πr3v=\frac{4}{3}\pi r^3

Volume per molecule at STP:

Vper=22.4×103NAV_\text{per}=\frac{22.4\times10^{-3}}{N_A}

Fraction:

vVper3.8×104\frac{v}{V_\text{per}} \approx 3.8\times10^{-4}


2) Q. Molar volume is the volume occupied by 1 mol of any (ideal) gas at STP. Show that it is 22.4 litres.

Answer:
At STP:

P=1.013×105 Pa, T=273 K, n=1P=1.013\times10^5\ \text{Pa},\ T=273\ \text{K},\ n=1

PV=nRTV=RTPPV=nRT \Rightarrow V=\frac{RT}{P}

V=8.31×2731.013×1052.24×102 m3=22.4 LV=\frac{8.31\times273}{1.013\times10^5}\approx 2.24\times10^{-2}\ \text{m}^3 = 22.4\ \text{L}


3) Q. Figure 13.8 shows plot of PV/T versus P for 1.00×1031.00\times10^{-3}

 

kg of oxygen gas at two different temperatures.

(a) What does the dotted plot signify?
Answer: The dotted line represents ideal gas behaviour where

PV/TPV/T

is constant (independent of

PP

).

(b) Which is true:

T1>T2T_1>T_2

or

T1<T2T_1<T_2

?
Answer: The curve closer to the dotted (ideal) line corresponds to the higher temperature. Hence,

T1>T2T_1>T_2

if curve

T1T_1

is nearer to ideal behaviour.

(c) What is the value of

PV/TPV/T

where the curves meet on the y-axis?
Answer: At very low pressure, gas is ideal:

PVT=nR\frac{PV}{T}=nR

For oxygen:

m=103 kg, M=0.032 kg mol1n=0.03125 molm=10^{-3}\ \text{kg},\ M=0.032\ \text{kg mol}^{-1}\Rightarrow n=0.03125\ \text{mol}

PVT=nR=0.03125×8.310.26 J K1\frac{PV}{T}=nR=0.03125\times 8.31 \approx 0.26\ \text{J K}^{-1}

(d) For

1.00×1031.00\times10^{-3}

kg hydrogen, will we get same

PV/TPV/T

at y-axis? If not, what mass of H

2_2

gives same

PV/TPV/T

?
Answer: No, because

PV/T=nRPV/T=nR

depends on number of moles.
To match oxygen’s

n=0.03125n=0.03125

mol:

mH2=nMH2=0.03125×0.002026.3×105 kgm_{H_2}=nM_{H_2}=0.03125\times0.00202 \approx 6.3\times10^{-5}\ \text{kg}

mH20.063 gm_{H_2}\approx 0.063\ \text{g}


4) Q. An oxygen cylinder of volume 30 litres has initial gauge pressure 15 atm at 27°C. After some oxygen is withdrawn, gauge pressure becomes 11 atm and temperature 17°C. Estimate mass of oxygen taken out.

Answer:
Use absolute pressure:

Pabs=Pgauge+1P_\text{abs}=P_\text{gauge}+1

P1=16 atm, T1=300 KP_1=16\ \text{atm},\ T_1=300\ \text{K}

P2=12 atm, T2=290 KP_2=12\ \text{atm},\ T_2=290\ \text{K}

V=30 L=0.03 m3V=30\ \text{L}=0.03\ \text{m}^3

n=PVRTn=\frac{PV}{RT}

n119.50,n215.13Δn4.37 moln_1\approx 19.50,\quad n_2\approx 15.13 \Rightarrow \Delta n \approx 4.37\ \text{mol}

Mass removed:

m=Δn×0.0320.14 kg140 gm=\Delta n \times 0.032 \approx 0.14\ \text{kg}\approx 140\ \text{g}


5) Q. An air bubble of volume 1.0 cm³ rises from bottom of a lake 40 m deep at 12°C. To what volume does it grow at surface at 35°C?

Answer:
Bottom pressure:

P1=P0+ρghP_1=P_0+\rho gh

P1=1.013×105+1000×9.8×404.93×105 PaP_1=1.013\times10^5+1000\times9.8\times40 \approx 4.93\times10^5\ \text{Pa}

Surface:

P2=P0P_2=P_0

T1=285 K, T2=308 KT_1=285\ \text{K},\ T_2=308\ \text{K}

P1V1T1=P2V2T2V2=V1P1P2T2T1\frac{P_1V_1}{T_1}=\frac{P_2V_2}{T_2} \Rightarrow V_2=V_1\frac{P_1}{P_2}\frac{T_2}{T_1}

V25.26 cm3V_2 \approx 5.26\ \text{cm}^3


6) Q. Estimate total number of air molecules in a room of capacity 25.0 m³ at 27°C and 1 atm.

Answer:

n=PVRT=(1.013×105)×258.31×3001.02×103 moln=\frac{PV}{RT}=\frac{(1.013\times10^5)\times25}{8.31\times300}\approx 1.02\times10^3\ \text{mol}

N=nNA(1.02×103)(6.022×1023)6.1×1026 moleculesN=nN_A\approx (1.02\times10^3)(6.022\times10^{23}) \approx 6.1\times10^{26}\ \text{molecules}


7) Q. Estimate average thermal energy of a helium atom at (i) 27°C (ii) 6000 K (iii) 10 million K.

Answer: (per atom)

E=32kT\langle E\rangle=\frac{3}{2}kT

(i)

T=300 KE6.2×1021 JT=300\ \text{K}\Rightarrow E\approx 6.2\times10^{-21}\ \text{J}


(ii)

T=6000 KE1.24×1019 JT=6000\ \text{K}\Rightarrow E\approx 1.24\times10^{-19}\ \text{J}


(iii)

T=107 KE2.07×1016 JT=10^7\ \text{K}\Rightarrow E\approx 2.07\times10^{-16}\ \text{J}


8) Q. Three vessels of equal capacity have gases at same T and P: neon, chlorine, uranium hexafluoride. Do they contain equal number of molecules? Is vrmsv_{rms}

 

same? If not, where is it largest?

Answer:

  • Yes, they contain equal number of molecules (Avogadro’s law: same

    P,V,TP,V,T\Rightarrow same

    nn).

  • vrmsv_{rms} is not same:

vrms=3RTMv_{rms}=\sqrt{\frac{3RT}{M}}

  • Largest

    vrmsv_{rms} for smallest molar massNeon.


9) Q. At what temperature is rms speed of argon equal to rms speed of helium at –20°C?

Answer:

TArMAr=THeMHeTAr=THeMArMHe\sqrt{\frac{T_{Ar}}{M_{Ar}}}=\sqrt{\frac{T_{He}}{M_{He}}} \Rightarrow T_{Ar}=T_{He}\frac{M_{Ar}}{M_{He}}

THe=253 K, MAr=39.9, MHe=4.0T_{He}=253\ \text{K},\ M_{Ar}=39.9,\ M_{He}=4.0

TAr253×39.94.02.52×103 KT_{Ar}\approx 253\times\frac{39.9}{4.0}\approx 2.52\times10^3\ \text{K}


10) Q. Estimate mean free path and collision frequency of N₂ at 2.0 atm and 17°C. Radius ≈ 1 Å. Compare collision time with free-flight time.

Answer:
Diameter

d=2r=2 A˚=2×1010 md=2r=2\ \text{Å}=2\times10^{-10}\ \text{m}


Number density:

n=PkTn=\frac{P}{kT}

Mean free path:

λ=12πd2n1.1×107 m\lambda=\frac{1}{\sqrt{2}\pi d^2 n}\approx 1.1\times10^{-7}\ \text{m}

Mean speed

vˉ4.7×102 m s1\bar v \approx 4.7\times10^2\ \text{m s}^{-1}


Collision frequency:

fvˉλ4.2×109 s1f\approx \frac{\bar v}{\lambda}\approx 4.2\times10^9\ \text{s}^{-1}

Time between collisions:

τ1f2.4×1010 s\tau \approx \frac{1}{f}\approx 2.4\times10^{-10}\ \text{s}

Collision duration is typically much smaller (~

101210^{-12}

s), so collision time

\ll

free-flight time.


11) Q. A 1 m narrow tube (closed at one end) contains a 76 cm mercury thread trapping 15 cm air. What happens if tube is held vertical with open end at bottom?

Answer:
When vertical with open end at bottom, the mercury falls down and some mercury comes out, so the remaining mercury height becomes less than 76 cm. Trapped air expands until equilibrium:

Pair=Patmρgh(in cm Hg: Pair=76h)P_{air}=P_{atm}-\rho g h \quad (\text{in cm Hg: } P_{air}=76-h)

If mercury height becomes

hh

cm, air length becomes

100h100-h

cm, and Boyle’s law gives:

(76h)(100h)=76×15(76-h)(100-h)=76\times15

Solving:

h52.2 cmh\approx 52.2\ \text{cm}

So trapped air length

47.8\approx 47.8

cm and about

7652.223.876-52.2\approx 23.8

cm of mercury flows out.


12) Q. Diffusion rate of H₂ is 28.7 cm³/s. Another gas diffuses at 7.2 cm³/s. Identify the gas.

Answer:
Graham’s law:

R1R2=M2M1\frac{R_1}{R_2}=\sqrt{\frac{M_2}{M_1}}

28.77.23.99(28.77.2)215.9\frac{28.7}{7.2}\approx 3.99 \Rightarrow \left(\frac{28.7}{7.2}\right)^2\approx 15.9

For H₂,

M1=2M231.832M_1=2\Rightarrow M_2\approx 31.8\approx 32


Hence the gas is O₂ (oxygen).


13) Q. Use law of atmospheres to derive sedimentation equilibrium formula.

Answer (outline):
Law of atmospheres:

n2=n1exp[mg(h2h1)kBT]n_2=n_1\exp\left[-\frac{mg(h_2-h_1)}{k_BT}\right]

For a particle in liquid, effective (apparent) weight:

Weff=mg(1ρρ)=mg(ρρ)ρW_{eff}=mg\left(1-\frac{\rho'}{\rho}\right)=mg\frac{(\rho-\rho')}{\rho}

Replace

mm

by molar mass form using

kB=RNAk_B=\frac{R}{N_A}

, giving:

n2=n1exp[mgNA(ρρ)(h2h1)ρRT]n_2=n_1\exp\left[-\frac{mgN_A(\rho-\rho')(h_2-h_1)}{\rho RT}\right]

which is the required expression.


14) Q. Given densities, estimate atomic sizes (tight packing approximation).

Answer (rough estimate):
Volume per atom

MρNA\approx \frac{M}{\rho N_A}

, atomic size

(volume)1/3\sim (\text{volume})^{1/3}

.
Approx atomic sizes (order of Å):

  • Carbon (diamond): ~ 2.1 Å

  • Gold: ~ 2.6 Å

  • Nitrogen (liquid): ~ 2.9 Å

  • Lithium: ~ 2.8 Å

  • Fluorine (liquid): ~ 3.0 Å

So atomic sizes are in the range of a few Å.


FAQs: Class 11 Physics Chapter 12 – Kinetic Theory

Q1. Is Kinetic Theory important for exams?
Yes, it is a high-weightage chapter in thermal physics.

Q2. Which topics are most important in this chapter?
Kinetic theory of gases, equipartition of energy, and degrees of freedom.

Q3. Are numericals asked from this chapter?
Yes, RMS speed, pressure, and energy-based numericals are common.

Q4. Are derivations important here?
Yes, derivations related to pressure of gas and kinetic energy are frequently asked.

Q5. How do NCERT Solutions help?
They provide NCERT-aligned, exam-ready explanations with solved numericals.