Intuition The one core idea
At the same temperature, every gas carries the same average kicking energy per molecule — so a light molecule must move fast and a heavy one must move slow . Because "escaping through a hole" happens at the speed the molecules move, light gases leak and spread faster, and the whole of Graham's law is just this sentence turned into a square root.
This page assumes nothing . Before you can read the parent note's derivation, you need to own every letter and symbol in it. We build them one at a time, each on the picture of the one before.
Everything below lives inside one image: a box of gas with a tiny pinhole in the wall.
Gas ::= a huge swarm of tiny molecules flying in straight lines, bouncing off walls and each other, otherwise mostly empty space .
Pinhole ::= a hole so small that a molecule slips through one at a time without bumping another molecule inside the hole.
Keep this box in your head. Every symbol we define is a number about the molecules in this box .
Definition Two masses, two scales
m ::= the mass of a single molecule (unimaginably tiny, kilograms).
M ::= the molar mass — the mass of one mole (a fixed huge count) of those molecules. In SI it is kilograms per mole (kg/mol); chemists usually quote it in grams per mole (g/mol), which is just 1000 × bigger.
Picture: m is one grain of sand; M is a labelled bag holding a standard count of grains. Same "heaviness" idea, just a convenient bookkeeping size.
Intuition Why the topic needs
M and not m
In a lab you never weigh one molecule — you weigh a mole . So chemists work with M . But the physics (speed) naturally uses m . The whole trick later is a clean swap between them — done carefully so the units match.
M for common gases you'll meet: H 2 = 2 , O 2 = 32 , NH 3 = 17 , HCl = 36.5 (all g/mol). You just add up the atomic masses — that's all a molar mass is.
v ::= the speed of one molecule = how many metres it covers each second (m/s).
The overline / angle brackets ⋅ or ⟨ ⋅ ⟩ ::= "take the average of this over all molecules."
⟨ v ⟩ ::= the mean speed — average the speeds themselves.
v 2 ::= the mean square speed — square every molecule's speed first , then average those squares.
Picture: a crowd of arrows of different lengths (each arrow = one molecule's speed). ⟨ v ⟩ is the average arrow length; v 2 is the average of the lengths squared — a different, slightly larger flavour of "typical speed."
Why bother with two averages? Because energy needs v 2 (next section), but flux through a hole needs ⟨ v ⟩ (Section 7). They are proportional — both ∝ 1/ M — so for Graham's ratio they behave identically, but they are not the same number, and honest physics keeps them distinct.
this formula, and why v 2 (not v )?
Double the speed and a ball hits four times as hard — energy grows with the square of speed, not the speed itself. That single fact, K E ∝ v 2 , is exactly why Graham's law ends up with a square root and not a plain 1/ M . Hold onto it.
Because different molecules move at different speeds, we take the average: K E = 2 1 m v 2 . The overline lands on v 2 — that's why we defined v 2 first.
Definition Temperature and Boltzmann's constant
T ::= absolute temperature in kelvin , a direct measure of average molecular jostling energy. T = 0 means no motion.
k B ::= Boltzmann's constant , a tiny fixed conversion number that turns "degrees of temperature" into "joules of energy per molecule."
Common mistake The word "translational" is not decoration
The 2 3 k B T counts only the energy of the molecule moving through space (its three directions x, y, z — hence the 3 ). A diatomic like O 2 or a polyatomic like NH 3 also stores energy in spinning and vibrating (internal degrees of freedom), and its total energy is larger than 2 3 k B T .
Why we can ignore that here: only translational motion carries a molecule toward the hole , so effusion depends on translational speed alone. The 2 3 k B T is exactly the right piece — but say "translational" so you know what you left out.
The picture above is the whole story: same translational energy budget, so the light molecules must run fast to spend it and the heavy ones crawl.
Setting the two expressions for translational K E equal (Section 3 = Section 4):
2 1 m v 2 = 2 3 k B T ⟹ v 2 = m 3 k B T
Definition What "rms" means — read the name backwards
Root-Mean-Square speed ::= take the square root of the mean of the squares of the speeds.
v r m s = v 2 = m 3 k B T
Why take the root at the end? v 2 has units of (m/s)², which is not a speed. The square root pulls it back to honest metres-per-second — a single number that fairly represents the whole spread of speeds in the Maxwell-Boltzmann Distribution .
v r m s vs the mean speed ⟨ v ⟩
The same distribution also has a mean speed ⟨ v ⟩ = π m 8 k B T . It is a little smaller than v r m s (about 92% of it), because squaring-then-rooting weights the fast molecules more heavily. Both carry the crucial factor 1/ m — that is all Graham's law needs.
See Root Mean Square Speed for the full treatment; here we only need its shape: speed ∝ m 1 at fixed T .
The physics gave us v r m s = 3 k B T / m with molecular mass m in kilograms . Chemistry wants molar mass M . One clean swap fixes it — provided we keep the units straight.
Definition Avogadro's number and the gas constant
N A ::= Avogadro's number = how many molecules make one mole (a fixed count, per mole).
R ::= the universal gas constant , and it is literally k B scaled up by N A :
R = N A k B , M = N A m
Here m is in kg, N A is per mole, so M = N A m comes out in kg/mol — the SI molar mass. That is the version that keeps the equation dimensionally clean.
Common mistake The g/mol trap
If you grab M off the periodic table in g/mol and drop it into 3 R T / M with R in J·mol⁻¹·K⁻¹, your speed comes out 1000 ≈ 32 × too big. Fix: convert to kg/mol first (e.g. O 2 : 32 g/mol = 0.032 kg/mol ). For Graham's ratio the 1000 cancels top and bottom, so g/mol is safe there — but never in an absolute speed. R also appears in Ideal Gas Equation , which is why all gas problems share this same unit hygiene.
Definition Rate and the "proportional to" sign
Rate r ::= how much gas throughput passes through the hole per unit time. Physically it is an amount per time : moles/s or volume/s (both count molecules leaving).
∝ ::= "is proportional to " — grows in step with, up to a fixed multiplier.
A diffusion tube instead reports a distance the gas front has travelled. That is not a throughput — it is really a speed — but since distance-covered scales with molecular speed exactly as throughput does, the same 1/ M ratio governs it. We keep the two ideas labelled so we never call a speed a "rate."
Intuition The collapse to Graham's law
Since n , A , 4 1 are common factors, only ⟨ v ⟩ distinguishes two gases. And ⟨ v ⟩ = 8 k B T / π m ∝ 1/ M at fixed T . Therefore
r ∝ ⟨ v ⟩ ∝ M 1 = M 1
That is Graham's law — every symbol in it is now earned. (The parent note writes r ∝ v r m s ; because ⟨ v ⟩ and v r m s differ only by the same constant factor for every gas, the ratio is identical either way — so both routes give the exact same Graham's law.)
Definition Subscripts and the flip
Subscripts 1, 2 ::= just labels for "gas one" and "gas two." r 1 is gas 1's rate, M 2 is gas 2's mass.
The fraction r 2 r 1 ::= how many times faster gas 1 is than gas 2.
Common mistake Why the masses swap sides
Rate is inverse to M . So when you make a ratio, the mass with subscript 1 must land on the bottom and mass 2 on the top — the labels cross:
r 2 r 1 = 1/ M 2 1/ M 1 = M 1 M 2
Sanity check with a pair you know: H 2 (light) must beat O 2 (heavy), and indeed 32/2 = 4 . ✓
This exact skill — reading a tiny mass difference as a tiny rate difference — is what powers Isotope Separation (Uranium Hexafluoride) .
Molecule mass m and molar mass M
Mean speed and mean square speed
Kinetic energy = half m v squared
Equal translational energy = three halves kB T
mean speed = sqrt 8RT over pi M
R = NA kB and M = NA m in kg per mol
Effusion flux = one quarter n mean-v A
Graham law rate ∝ 1 over sqrt M
Test yourself — reveal only after answering out loud.
What is the difference between m and M , and in what units? m = mass of one molecule (kg); M = molar mass = mass of one mole. SI is kg/mol, and M = N A m holds when m is in kg.
What does the overline / bracket mean, and how do ⟨ v ⟩ and v 2 differ? Both mean "average over all molecules." ⟨ v ⟩ averages the speeds; v 2 averages the squares of the speeds.
Write the kinetic energy of one molecule in terms of m and v . K E = 2 1 m v 2 .
Why does energy involve v 2 and not v ? Doubling speed quadruples the impact energy; this square is the source of the square root in Graham's law.
State the equal-energy law and its crucial qualifier. K E trans = 2 3 k B T ; it is the translational energy only, depends only on T , and excludes rotation/vibration.
Why can we ignore internal (rotation/vibration) energy for effusion? Only translational motion carries a molecule toward the hole, so only 2 3 k B T matters for escape.
Which average speed governs effusion flux, and via what formula? The mean speed ⟨ v ⟩ , through the kinetic-theory flux r = 4 1 n ⟨ v ⟩ A .
Why does r ∝ v r m s (parent) and r ∝ ⟨ v ⟩ give the same Graham's law? ⟨ v ⟩ and v r m s differ by the same constant factor for every gas, so their ratio is identical.
How do R and k B relate, and what unit must M be in? R = N A k B ; use M in kg/mol for absolute speeds (g/mol only cancels in ratios).
In r 2 r 1 = M 1 M 2 , why do the masses swap? Rate is inverse to
M , so forming the ratio flips the mass labels top-for-bottom.