Graham's Law states that the rate of gas effusion (or diffusion) is inversely proportional to the square root of molar mass. Lighter gases move faster than heavier gases.
Rate₁ / Rate₂ = √(M₂/M₁)
Or equivalently:
Rate₁ / Rate₂ = √(MM₂/MM₁)
Units: mol/s, mL/s, or any volume/time
How fast gas passes through opening or spreads
💡 Can also be velocity (m/s) or average speed
Units: g/mol
Molecular weight of the gas
⚠️ Notice: heavier gas (M₂) goes in numerator, making ratio less than 1
Gas escaping through a tiny hole into vacuum
Example: Helium balloon deflating
Gas spreading through space or another gas
Example: Perfume smell spreading across room
Rate(He) / Rate(O₂) = √[M(O₂) / M(He)]
Note: Heavier gas (O₂) goes in numerator
Rate(He) / Rate(O₂) = √(32/4) = √8
√8 = 2.83
Answer: He effuses 2.83 times faster than O₂
Makes sense! He is 8× lighter, so it moves √8 ≈ 2.83× faster.
M₂ = M₁ × (Rate₁/Rate₂)²
Square both sides and solve
Rate₁/Rate₂ = √(M₂/M₁)
Standard form
t₁/t₂ = √(M₁/M₂)
Time ratio is inverted (slower = more time)
v₁/v₂ = √(M₂/M₁)
Same relationship as rates
It's √(M₂/M₁) with HEAVIER molar mass in numerator. Getting this backwards gives upside-down answer!
It's √(M₂/M₁), NOT just M₂/M₁. The square root is critical!
For O₂, use 32 g/mol (molecular), not 16 g/mol (atomic). For H₂, use 2 g/mol, not 1 g/mol.
Graham's Law is about SPEED (how fast), Dalton's is about PRESSURE (how much). Different concepts!
Rate₁/Rate₂ = √(M₂/M₁). The rate of gas effusion or diffusion is inversely proportional to the square root of molar mass. Lighter gases move faster.
Effusion is gas escaping through a tiny hole into vacuum. Diffusion is gas spreading through space or another gas. Graham's Law applies to both.
From kinetic molecular theory: lighter molecules move faster at the same temperature because KE = ½mv². Same energy with less mass means higher velocity.
Comes from kinetic energy equation: v ∝ √(T/M). Velocity is proportional to square root of temperature divided by mass.
No, Graham's Law is for ideal gases only. Liquids have strong intermolecular forces that dominate diffusion behavior.