B.3.2—Amount of substance
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- SL
Amount of substance
The amount of substance n counts how many groups of NA particles are present:
n=NAN
where N is the number of particles and NA is the Avogadro constant.
Connect mass to moles
If molar mass is M, then
n=Mm
Use matching units for m and M. Once n is known, the number of particles is N=nNA.
Use ratios efficiently
For equal numbers of particles, the samples contain equal amounts in moles even if their masses differ. For isotope or element comparisons, calculate moles before comparing particle counts.
Worked comparison from local Question Bank row 28984
For 40g of argon-40, nAr=40/40=1.0mol. For 8g of helium-4, nHe=8/4=2.0mol. Since N=nNA,
NHeNAr=2.0NA1.0NA=21
The larger argon mass does not mean more atoms; its molar mass is also larger.
Common trap
Do not confuse N (number of particles) with NA (particles per mole) or n (amount in moles).
The evidence uses particle-number ratios for different isotopes and a calculation of the mass of one copper atom from molar mass and Avogadro’s constant.
Calculate / Determine
Use n=N/N_A for particle counts and n=m/M for mass-to-moles conversions. Compare moles before comparing numbers of atoms or molecules, and keep mass units consistent with molar mass.
Comparing sample masses directly without accounting for molar mass, or confusing N with n.
Representative question
What is the number of atoms in 40 g of Krypton- 80 number of atoms in 20 g of Neon- 20 ?
41
21
2
4
C
Macroscopic equations
Pressure is P=F⊥/A. For a fixed amount of gas, empirical laws combine to PV/T=constant, and the ideal-gas equations are PV=nRT=NkBT.
Microscopic model
Particles move randomly and collide elastically with walls. Momentum transfer produces pressure, with P=31ρv2. For a monatomic ideal gas, U=23NkBT=23nRT.
Bridge the descriptions
Use n=N/NA to move between moles and particles. Choose the equation from the data provided, convert temperature to kelvin, and keep SI units consistent.
Model boundary
The ideal approximation works best at high temperature and low pressure or density. At high density, high pressure or near condensation, finite particle size and intermolecular forces matter.