Q.Estimate the mean free path and collision frequency of a nitrogen molecule in a cylinder containing nitrogen at 2.0 atm and temperature 17 ∘C. Take the radius of a nitrogen molecule to be roughly 1.0 A˚. Compare the collision time with the time the molecule moves freely between two successive collisions (Molecular mass of N2=28.0 u).
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Kinetic Theory of Gases
Imagine you're sitting in a quiet room. The air around you feels still — but it isn't. Every second, billions of tiny particles (molecules of nitrogen, oxygen, and others) are zipping past you at hundreds of metres per second. They're constantly crashing into each other and into the walls, your skin, the furniture. You don't feel each individual hit because the molecules are so small and the collisions happen so fast. But collectively, those countless tiny impacts produce something you do feel: pressure.
That's the core intuition behind the kinetic theory of gases. It says: all the macroscopic properties of a gas — pressure, temperature, volume — can be explained by the motion of its molecules.
The Big Idea
Instead of treating a gas as a continuous, smooth substance (like a fluid), the kinetic theory treats it as a swarm of tiny, hard, perfectly elastic balls in constant, random motion. "Perfectly elastic" means that when two molecules collide, no kinetic energy is lost — they bounce off each other like ideal billiard balls, not like sticky clay.
From this simple picture, we can derive the gas laws (Boyle's, Charles's, Avogadro's) and even calculate things like the speed of sound in a gas.
The Five Assumptions (The Precise Statement)
For a gas to behave according to the kinetic theory in its simplest form, we make these assumptions:
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A gas consists of a very large number of molecules.
The number is so huge that we can use statistics — individual molecules don't matter, only averages do.
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The molecules are in constant, random motion.
They move in straight lines until they hit something (another molecule or a wall). There's no preferred direction.
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The molecules are point masses.
Their actual size is negligible compared to the distance between them. In other words, the volume of the molecules themselves is tiny compared to the volume of the container.
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Collisions are perfectly elastic.
No kinetic energy is lost when molecules collide with each other or with the walls. Total energy of the system stays constant.
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There are no intermolecular forces.
The molecules don't attract or repel each other except during collisions. Between collisions, they move freely.
These assumptions define an ideal gas. Real gases deviate from this behaviour at high pressure or low temperature, but the kinetic theory gives an excellent approximation for most everyday conditions.
How It Explains Pressure
Pressure is the force per unit area exerted by the gas on the walls of its container. In the kinetic picture:
- A molecule moving toward a wall hits it and bounces back.
- During the collision, the wall exerts a force on the molecule to reverse its momentum.
- By Newton's third law, the molecule exerts an equal and opposite force on the wall.
- Multiply that by the billions of collisions happening every second, and you get a steady, measurable pressure.
If you heat the gas, the molecules move faster. They hit the walls harder and more often — pressure increases. If you compress the gas into a smaller volume, molecules hit the walls more frequently — pressure increases again.
The Key Result: The Kinetic Equation
From these assumptions, we can derive a relationship between pressure P, volume V, and the average kinetic energy of the molecules. The result is:
PV=31Nmv2
Where:
- N = number of molecules
- m = mass of one molecule
- v2 = mean square speed of the molecules (average of the squares of their speeds)
Since the average kinetic energy of a molecule is K=21mv2, we can rewrite this as:
PV=32NK …
Concept: Molecular Volume Fraction — the mean free path λ depends on the number density n and collision cross-section σ=πd2, while collision frequency f=vrms/λ.
Step 1: Number density
T=17∘C=290 K, P=2.0 atm=2.026×105 Pa.
Using P=nkBT:
n=kBTP=(1.38×10−23)(290)2.026×105≈5.06×1025 m−3
Step 2: Mean free path
Molecular diameter d=2r=2.0 A˚=2.0×10−10 m.
λ=2πd2n1=1.414×π×(2.0×10−10)2×5.06×10251≈1.11×10−7 m
Step 3: Collision frequency
RMS speed: vrms=M3RT=0.0283×8.314×290≈508 m/s
f=λvrms≈1.11×10−7508≈4.58×109 s−1
Step 4: Time comparison …
At 2.0 atm and 290 K the mean free path is λ≈1.1×10−7 m and the collision frequency is ν≈4.6×109 s−1. A collision lasts about 500 times less than the free-flight time between collisions.
Set-up
We need the number density n, then the mean free path λ, the molecular speed, the collision frequency ν=v/λ, and finally the ratio of collision time to free-flight time.
λ=2πd2n1,ν=λvrms
Data (SI)
- P=2.0 atm=2.026×105 Pa
- T=17 ∘C=290 K
- r=1.0 A=1.0×10−10 m ⇒ d=2.0×10−10 m
- m=28.0×1.66×10−27=4.65×10−26 kg
Step 1 - Number density
n=kTP=(1.38×10−23)(290)2.026×105≈5.06×1025 m−3
Step 2 - Mean free path
λ=2π(2.0×10−10)2(5.06×1025)1≈1.11×10−7 m
Step 3 - Molecular speed
vrms=m3kT=4.65×10−263(1.38×10−23)(290)≈5.1×102 m s−1
Step 4 - Collision frequency
ν=λvrms=1.11×10−7508≈4.6×109 s−1
Step 5 - Collision time vs free-flight time
A collision lasts roughly the time to cross one molecular diameter: …
Sanity-check via a known benchmark. A useful reference point: for a typical diatomic gas at 1 atm, 300 K, the mean free path is of order 10−7 m (a few hundred molecular diameters). Since λ∝1/(nP)∝1/P at fixed T, doubling the pressure to 2.0 atm should roughly halve that benchmark — consistent with the computed 1.11×10−7 m. The deeper physical point here is the ratio τ/τc∼550: a molecule spends the overwhelming majori …
- KCET 2025Set D-41 markMCQQ.At 27∘C temperature, the mean kinetic energy of the atoms of an ideal gas is E1. If the temperature is increased to 327∘C, then the mean kinetic energy of the atoms will be (A) 2E1 (B) 2E1 (C) 2E1 (D) 2E1
›Reveal solutionSolution
Mean kinetic energy is 23kBT, i.e. directly proportional to the absolute (kelvin) temperature — and 27∘C → 327∘C is 300 K → 600 K, an exact doubling.
Step 1 — The concept: kinetic interpretation of temperature
From the kinetic theory of gases, the average translational kinetic energy of a single molecule of an ideal gas is
E=23kBT
where kB is Boltzmann's constant and T is the absolute temperature in kelvin.
This is the deepest statement in the chapter: temperature is a measure of the mean molecular kinetic energy. Note what the formula does not contain — no mass, no pressure, no volume, no gas identity. The mean KE depends on temperature alone.
Since 23kB is a constant:
E∝T⟹E1E2=T1T2
Step 2 — ⚠️ Convert to KELVIN (this is the whole trap)
The proportionality holds for absolute temperature only. Using Celsius here would be a serious error, so convert first:
T(K)=t(∘C)+273
T1=27+273=300 K
T2=327+273=600 K
Step 3 — Take the ratio
E1E2=T1T2=300600=2
E2=2E1
Step 4 — Why the distractors are there …
- COMEDK 2025Set 2025-E1 markMCQQ.The rms velocity of the gas molecule at 327∘C is same as the rms velocity of the oxygen molecules at 27∘C. If the molecular weight of oxygen is 32 then the molecular weight of the given gas molecule is: (A) 32 (B) 64 (C) 96 (D) 128
›Reveal solutionSolution
The rms speed depends only on temperature and molecular mass; equating the rms speeds for two gases gives a direct ratio of masses. The molecular weight of the unknown gas is 64, so the correct option is (B).
Concept & Intuition
The root-mean-square (rms) speed of gas molecules is given by vrms=M3RT, where T is the absolute temperature (in Kelvin) and M is the molar mass. If two different gases have the same rms speed, then their MT ratios must be equal. This lets us solve for the unknown molar mass without needing any other gas properties.
Step-by-step solution
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Convert temperatures to Kelvin
- For the unknown gas: T1=327∘C=327+273=600K
- For oxygen: T2=27∘C=27+273=300K
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Write the rms speed equality
vrms, unknown=vrms, oxygen
M13RT1=M23RT2
- Cancel common factors The 3R cancels from both sides, leaving:
M1T1=M2T2
Squaring both sides:
M1T1=M2T2
- Substitute known values T1=600K, T2=300K, M2=32 (oxygen’s molecular weight):
M1600=32300
- Solve for M1 Cross-multiply: …
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- COMEDK 2024Set 2024-A1 markMCQQ.If pressure of an ideal gas is increased by keeping temperature constant the kinetic energy will (A) Vary quadratically (B) Increase (C) Not change (D) Decrease
›Reveal solutionSolution
For an ideal gas at constant temperature, the average kinetic energy depends only on temperature, so increasing pressure does not change it. The correct option is (C).
The key concept here is the kinetic theory of gases. The average kinetic energy of an ideal gas molecule is directly proportional to the absolute temperature:
KE=23kBT
where kB is Boltzmann’s constant. This means that as long as the temperature stays fixed, the average kinetic energy per molecule remains constant — regardless of changes in pressure or volume.
Pressure is increased by reducing volume (since PV=nRT at constant T), which makes molecules collide with the walls more frequently, but their individual speeds (and thus kinetic energy) do not change. The total internal energy of the gas also stays the same because it depends only on temperature for an ideal gas.
Let’s walk through the reasoning step by step:
-
Recall the definition: Kinetic energy of a single molecule is 21mv2. The average over all molecules is 23kBT for a monatomic ideal gas. This formula shows no dependence on pressure or volume.
-
Apply the ideal gas law: PV=nRT. If temperature T is constant and pressure P increases, then volume V must decrease proportionally. But T is the only factor in the kinetic energy expression.
-
Check the options:
- (A) Vary quadratically — No, because kinetic energy is constant, not varying.
- (B) Increase — No, temperature is fixed.
- (C) Not change — Yes, matches the theory.
- (D) Decrease — No, same reason. …
-
- COMEDK 2024Set 2024-A1 markMCQQ.A cubical box of side 2 m contains helium gas. It was observed that in a time of 1 second, an atom travelling with the root-mean-square speed parallel to one of the edges of the cube, made 250 hits with one of the walls, without any collision with other atoms. The average kinetic energy of the helium gas is Take R=325 J/mol−K and kB=1.38×10−23JK−1 (A) 82.8×10−21 J (B) 3.31×10−21 J (C) 82.8×10−19 J (D) 1×10−21 J
›Reveal solutionSolution
The atom makes 250 round trips of 4 m in 1 s, giving vrms=1000 m/s; the average translational KE 21mvrms2≈3.31×10−21 J.
Speed from wall hits: The atom bounces between opposite walls separated by L=2 m, striking a given wall once per round trip of length 2L=4 m. With 250 hits in 1 s:
d=250×4=1000 m in 1 s ⇒ vrms=1000 m s−1.
Mass of a helium atom (NA=R/kB=(25/3)/1.38×10−23=6.04×1023): …
- COMEDK 2024Set 2024-M1 markMCQQ.A cubical box of side 1 m contains Boron gas at a pressure of 100 Nm−2. During an observation time of 1 second, an atom travelling with the rms speed parallel to one of the edges of the cube, was found to make 500 hits with a particular wall, without any collision with other atoms. The total mass of gas in the box in gram is (A) 30 (B) 0.3 (C) 3 (D) 0.03
›Reveal solutionSolution
The key is to relate the number of wall hits to the rms speed and the box dimensions, then use the ideal gas law to find the total mass. The final answer is 0.3 grams.
We are told a single atom, moving at the rms speed parallel to an edge, hits a particular wall 500 times in 1 second without any collisions with other atoms. This means the atom travels back and forth between opposite walls, bouncing elastically. The distance between the two opposite walls is 1 m (the side of the cube). In one round trip (to the wall and back), the atom travels 2 m. Each time it hits the wall counts as one hit.
Concept and Intuition:
The number of hits per second tells us how fast the atom is moving. If an atom makes 500 hits in 1 second, it covers 500 × 2 m = 1000 m in that second. That distance is exactly the rms speed of the atom. Once we know the rms speed, we can find the temperature from the kinetic theory relation. Then, using the ideal gas law, we can find the number of moles and hence the total mass of the gas.
- Find the rms speed from the hit rate. The atom travels from one wall to the opposite wall (distance 1 m) and back (another 1 m) for each hit. So each hit corresponds to a round trip of 2 m. In 1 second, 500 hits means the atom travels 500×2=1000 m. Therefore, its speed (which is the rms speed, vrms) is
vrms=1000m/s.
- Relate rms speed to temperature. For a monatomic gas like Boron (which is monatomic in gaseous form), the rms speed is given by
vrms=M3RT,
where R=8.314J mol−1K−1 and M is the molar mass in kg/mol.
Boron has atomic mass 10.8 u, so M=10.8×10−3kg/mol.
Squaring both sides:
(1000)2=10.8×10−33×8.314×T.
Solving for T:
106=0.010824.942T⇒T=24.942106×0.0108≈433.0K. …
- KCET 2023Set A-31 markMCQQ.The speed of sound in an ideal gas at a given temperature T is v. The rms speed of gas molecules at that temperature is vrms. The ratio of the velocities v and vrms for helium and oxygen gases are X and X' respectively. Then X′X is equal to (A) 215 (B) 215 (C) 521 (D) 521
›Reveal solutionSolution
The ratio v/vrms=γ/3 depends only on γ, so the answer reduces to γHe/γO2.
Step 1 — The two speeds.
Speed of sound in an ideal gas (Laplace's correction — the compressions are adiabatic, not isothermal):
v=MγRT.
Root-mean-square molecular speed from kinetic theory:
vrms=M3RT.
Step 2 — Form the ratio.
vrmsv=3RT/MγRT/M=3γ.
Beautifully, T, R and the molar mass M all cancel — the ratio depends only on the atomicity of the gas through γ. That is why the question can be answered without any numbers for T or M.
Step 3 — Insert the γ values. …
- COMEDK 2023Set 2023-E1 markMCQQ.The molecules of a given mass of a gas have root mean square speed of 120 m/s at 88∘C and 1 atmospheric pressure. The root mean square speed of the molecules at 127∘C and 2 atmospheric pressure is (A) 105.2 m/s (B) 1.443 m/s (C) 126.3 m/s (D) 88/127 m/s
›Reveal solutionSolution
RMS speed depends only on temperature: vrms∝T. Raising T from 361 K to 400 K gives v2≈126.3 m/s; pressure is irrelevant.
vrms=M3RT∝T, independent of pressure.
T1=88∘C=361 K, T2=127∘C=400 K. …
- COMEDK 2022Set 20221 markMCQQ.The average kinetic energy of a molecule in air at room temperature of 20∘C (A) 6×10−22 J (B) 7.06×10−21 J (C) 6.07×10−21 J (D) 6.70×10−21 J
›Reveal solutionSolution
KE = (3/2)(1.38 x 10^-23)(293) = 1.5 x 1.38 x 293 x 10^-23 = 606.5 x 10^-23 = 6.07 x 10^-21 J
Concept: average translational kinetic energy of a gas molecule = (3/2) k_B T (independent of the molecular mass).
T = 20 C = 293 K, k_B = 1.38 x 10^-23 J/K
KE = (3/2)(1.38 x 10^-23)(293) …
- COMEDK 2021Set 20211 markMCQQ.The collision of the molecules of an ideal gas is taken as (A) elastic (B) inelastic (C) partially elastic (D) partially inelastic
›Reveal solutionSolution
One of the basic assumptions is that collisions between molecules (and with the walls) are perfectly ELASTIC - kinetic energy and momentum are conserved, so the gas does not lose energy and the pressure stays steady.
Concept: postulates of the kinetic theory of an ideal gas. …
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