Theme B — The Particulate Nature of Matter
B.3.4 Ideal Gas Equation — IB Physics HL Revision Notes & Topical Questions
5 min read 10 parts Lesson 28 of 53 1 quiz
Curriculum Equation Key قوانين الرقم الهيدروجيني والاتزان الأيوني - pH & Acid-Base Equilibrium FormulasFast Exam Solution
pH = -log[H⁺] | pOH = -log[OH⁻] | pH + pOH = 14 | [H⁺][OH⁻] = 10⁻¹⁴
Word Equation & Conditions: الرقم الهيدروجيني = -لوغاريتم تركيز أيون الهيدروجين | pH + pOH = 14
Location & Specifications: الاتزان الأيوني، كيمياء 3 ثانوي، التحصيلي، و AP Chemistry.
Lesson summary
B.3.4 Ideal Gas Equation — IB PHYSICS SL notes: Use pV = nRT and pV = NkBT to solve gas problems, and explain when a real gas behaves ideally.Combining the laws — Boyle's, Charles's and the pressure law give one constant for a fixed amount of gas, which is proportional to the amo…
- Equation of state
- What the symbols mean
- Definition
- Gas constant R
- Boltzmann constant kB
- Constants in the data booklet
Section 1 of 10The ideal gas equation
Combining the laws
- Boyle's, Charles's and the pressure law give one constant for a fixed amount of gas, which is proportional to the amount.
Equation of state
- Equation of state pV = nRT.What the symbols mean: p = pressure (Pa) · V = volume (m3) · n = amount of gas (mol) · R = 8.31 J mol−1 K−1 · T = temperature (K = °C + 273)
- p is the absolute pressure in Pa.
- V is the volume in m3 (1 dm3 = 10−3 m3).
- n is the amount of gas in mol.
- R = 8.31 J K−1 mol−1 is the ideal gas constant.
- T is the temperature in K.
Units
- Units pV has the dimensions of energy, so the units of R follow, and all quantities must be in SI.
Definition
- Definition an ideal gas obeys the ideal gas equation at all pressures, volumes and temperatures.
Section 2 of 10Constants
1Gas constant R
- Gas constant R the macroscopic constant, linked to volume and temperature.
2Boltzmann constant kB
- Boltzmann constant kB the microscopic constant, linked to the thermal energy of particles.
3Relation
- Relation kB = R/NA = 1.38 × 10−23 J K−1.
4Constants in the data booklet
- R, NA and kB are all given.
Section 3 of 10Molecular form
Equation
- Equation pV = NkBT, using N = nNA.
When to use
- When to use when the number of molecules, a number density N/V or a molecular mass is given.
Rearranged
- Rearranged p = (N/V)kBT, so at constant temperature the pressure is proportional to the number of molecules per unit volume.
Link
- Link the two forms are connected by nR = NkB.
Section 4 of 10Assumptions of the ideal gas
Small molecules
- Small molecules their volume is negligible compared with their separation.
No intermolecular forces
- No intermolecular forces except in collisions, so there is no potential energy.
Elastic collisions
- Elastic collisions with each other and with the walls.
Random motion
- Random motion the time of a collision is negligible compared with the time between collisions.
Internal energy
- Internal energy all of it is random kinetic energy of the molecules.
Section 5 of 10Real gases
Close to ideal
- Close to ideal at low pressure, low density and a temperature well above the boiling point.
- The molecules are far apart, so their volume is negligible and the forces are small.
High pressure
- High pressure the molecules are close and occupy a significant fraction of the volume, and attractive forces appear.
Low temperature
- Low temperature the attractive forces become important compared with kinetic energy and the gas condenses.
Most ideal
- Most ideal gases of weakly interacting molecules, such as helium.
Air
- Air at normal room temperature and pressure it behaves very nearly like an ideal gas.
pV/nRT graph
- pV/nRT graph it is a horizontal line at 1 for an ideal gas, dips below 1 at moderate pressures for real gases and rises above 1 at very high pressures.
Section 6 of 10Strategy for problems
1
List n or N, p, V and T, and convert to SI units.
2
If the same gas changes state, use pV/T = constant, which avoids R and n.
3
If the amount changes, as when gas leaks or is pumped in, use n = pV/RT at each stage.
4
For a gas under a piston or at depth, find the absolute pressure first.
5
To find the number of particles, use N = nNA.
- Check
- at 273 K and 1.01 × 105 Pa one mole occupies about 22.4 dm3.
Section 7 of 10Density form
Density
- ρ = m/V = pM/RT, where M is the molar mass in kg mol−1.
Fixed pressure
- Fixed pressure density is inversely proportional to absolute temperature, which is why hot air rises.
Fixed temperature
- Fixed temperature density is proportional to molar mass, which is why a helium balloon floats.
Air
- Air with M = 0.029 kg mol−1 at 300 K and 1.01 × 105 Pa, ρ ≈ 1.2 kg m−3.
Section 8 of 10More from the specification
1Kinetic collisions of ideal gas atoms
- Kinetic collisions of ideal gas atoms ideal gas laws assume negligible intermolecular attractive forces between rapidly colliding gaseous molecules or atoms.
2Ideal Gas Equation of State
- The equation of state for an ideal gas is p·V = n·R·T = N·kB·T, relating pressure p, volume V, temperature T in kelvin,
- and quantity of substance in moles n confined within a rigid container.
- (or number of molecules N)
3Kinetic Theory of Gases and Pressure
- Kinetic theory models gas molecules in continuous random motion;
- pressure results from elastic collisions with container walls where molecules rebound with equal speed, imparting momentum changes Δp = 2·m·v per collision.
4Molecular Speed Distribution and Temperature
- The average translational kinetic energy of gas molecules is directly proportional to absolute temperature (½·m·(crms)² = 3/2·kB·T);
- this means higher temperatures result in a higher root-mean-square speed of particles.
5Theory
- A well-tested, wide-ranging explanation supported by evidence.
6Momentum
- P = mv, a vector.
7Kinetic theory
- Particles in constant random motion.
8Avogadro constant
- The number of particles per mole, 6.02 × 10²³ mol⁻¹
9Average speed
- Total distance divided by total time.
10Thermodynamic temperature
- The absolute temperature in kelvin.
Section 9 of 10Key terms
| Term | Meaning |
|---|---|
| Ideal gas | A gas that obeys the ideal gas equation at all pressures, volumes and temperatures |
| Ideal gas constant (R) | R = 8.31 J K−1 mol−1 |
| Boltzmann constant (kB) | kB = R/NA = 1.38 × 10−23 J K−1 |
| Equation of state | Relation pV = nRT linking pressure, volume, amount and temperature |
| Real gas | A gas that deviates from ideal behaviour at high pressure and low temperature |
| Number density | Number of molecules per unit volume, N/V |
Section 10 of 10Exam technique
1
Using °C or litres directly in the equation — use kelvin and m3.
2
Mixing R with kB — use R with n and kB with N.
3
Using gauge pressure — use absolute pressure.
4
Using pV = nRT when the amount changes between states — apply it to each state.
5
Expecting ideal behaviour at high pressure and low temperature — real gases deviate there.
Marked practiceQuizzes for this lesson
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