This MCQ module is based on: Molecular Behaviour Gas Laws
Molecular Behaviour Gas Laws
This assessment will be based on: Molecular Behaviour Gas Laws
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Molecular Behaviour Gas Laws
12.1 Introduction — From Macroscopic to Microscopic
In Chapter 11 we treated thermodynamics in purely macroscopic terms — pressure, volume, temperature, internal energy. Kinetic theory takes a complementary view: it explains all those macroscopic observations starting from the assumption that a gas is a swarm of tiny molecules in incessant random motion. Robert Boyle (1661), and later Maxwell and Boltzmann in the 19th century, built this picture into one of the most successful theories of physics.
12.2 Molecular Nature of Matter
Richard Feynman remarked that the discovery "matter is made of atoms" is among the most significant in the history of science. The modern atomic theory is credited to John Dalton (~1808), who used it to explain the laws of definite and multiple proportions. Avogadro then sharpened the picture with his hypothesis: equal volumes of all gases at the same temperature and pressure contain the same number of molecules.
A typical molecule has size ~ 10⁻¹⁰ m (an Angstrom). At standard temperature and pressure (STP), 1 mole of any gas (6.022 × 10²³ molecules) occupies about 22.4 litres. The mean separation between molecules in a gas at STP is roughly 10 times the molecular diameter — gases are mostly empty space.
Inter-molecular forces are short-range and important in solids and liquids; in gases the molecules are so far apart that we can treat them as non-interacting except during instantaneous collisions. This single simplification is what makes gas behaviour so much easier to describe than that of solids and liquids.
12.3 Behaviour of Gases — The Gas Laws
Long before kinetic theory, careful experiments produced three empirical gas laws. They are what kinetic theory must reproduce.
12.3.1 Boyle's Law (T constant)
12.3.2 Charles' Law (P constant)
12.3.3 Avogadro's Hypothesis
Combining these three relations gives the ideal gas equation:
Equivalently in terms of total molecules N and the Boltzmann constant k_B = R/N_A = 1.38 × 10⁻²³ J/K:
12.3.4 Dalton's Law of Partial Pressures
For a mixture of non-reacting ideal gases, each gas acts independently. The total pressure equals the sum of the partial pressures each gas would exert if it occupied the volume alone:
| Constant | Symbol | Value (SI) |
|---|---|---|
| Universal gas constant | R | 8.314 J·mol⁻¹·K⁻¹ |
| Boltzmann constant | k_B | 1.381 × 10⁻²³ J·K⁻¹ |
| Avogadro number | N_A | 6.022 × 10²³ mol⁻¹ |
| Molar volume at STP (273.15 K, 1 atm) | V_m | 22.4 × 10⁻³ m³ |
| Atmospheric pressure | P_atm | 1.013 × 10⁵ Pa |
Worked Examples
Example 12.1: Number of molecules at STP
How many molecules of an ideal gas are present in 1 cm³ at STP (T = 273 K, P = 1.013 × 10⁵ Pa)?
= 0.1013 / (3.77 × 10⁻²¹) ≈ 2.69 × 10¹⁹ molecules.
This is the Loschmidt number n₀ — the molecular density of an ideal gas at STP.
Example 12.2: Boyle's law compression
A bubble of air rises from the bottom of a lake (10.3 m deep, T constant). At the bottom its volume is 1.0 cm³. Atmospheric pressure = 1.013 × 10⁵ Pa, ρ_water = 10³ kg/m³, g = 9.8 m/s². Find its volume when it reaches the surface.
P_top = P_atm = 1.013 × 10⁵ Pa.
By Boyle's law (constant T): P₁V₁ = P₂V₂. So V₂ = (P₁/P₂)V₁ = (2.02/1.013) × 1.0 ≈ 2.0 cm³ — the bubble doubles in size.
Example 12.3: Heating a sealed tyre
A tyre is inflated to 2.5 × 10⁵ Pa at 27 °C. After driving on a hot road its temperature rises to 57 °C. Assuming volume is unchanged, find the new pressure.
Interactive: Ideal Gas Law Calculator L3 Apply
Set the moles n, temperature T and volume V; the applet computes the pressure P from PV = nRT.
- Take a 10-mL plastic syringe; pull plunger to 10 mL with the tip open. Now seal the tip with your finger.
- Push the plunger from 10 mL to 5 mL (volume halves) at room temperature.
- Note the resistance you feel — that resistance is the increased pressure pushing back on the plunger.
- Release; observe the plunger spring back to nearly its original position.
Competency-Based Questions
Q1. L1 Remember State Avogadro's hypothesis.
Q2. L2 Understand Why is the ideal gas law more accurate at low pressures and high temperatures?
Q3. L3 Apply Find the new volume of the balloon in the storage room.
Q4. L4 Analyse A mixture of 0.10 mol N₂ and 0.20 mol O₂ is placed in a 5.0 L vessel at 300 K. Find the partial pressure of O₂ and the total pressure. (R = 8.314 J/mol·K)
Q5. L5 Evaluate A student claims a real gas at very high pressure can have PV/(nT) less than R. Is this consistent with experiments? Justify.
Assertion-Reason Questions
Assertion (A): The ideal gas law is universal — at given P, T, V, all gases contain the same number of moles.
Reason (R): The constant R has the same numerical value for every ideal gas.
Assertion (A): Boyle's law fails for a real gas near its liquefaction temperature.
Reason (R): Inter-molecular forces become non-negligible near liquefaction.
Assertion (A): At STP, one mole of any ideal gas occupies 22.4 L.
Reason (R): The Boltzmann constant equals R/N_A.