This is a practice page for Density, molar mass, molar volume . We will not re-derive the bridges here — we will use them until every possible type of problem feels familiar . First we map out what kinds of questions even exist , then we walk one worked example for each kind.
Intuition The three bridges, on one picture
Every problem on this page is a journey between three "islands": mass (grams, what a balance reads), volume (litres or cm³, what a flask reads), and moles (how many particles — what chemistry actually cares about). The three bridges connect them:
density ρ = V m connects mass ↔ volume
molar mass n = M m connects mass ↔ moles
molar volume n = V m V connects volume ↔ moles
Every example below is just "which island am I on, which island do I want, which bridges cross the gap."
Before solving anything, let's list every distinct kind of situation this topic can hand you. If we cover each row, nothing on an exam can surprise us.
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Case class
What makes it different
Covered by
A
One bridge, forward
given mass, want moles (or vice-versa)
Ex 1
B
Two bridges chained
mass→moles→volume across an island
Ex 2
C
Gas at STP
use V m = 22.7 L mol − 1
Ex 3
D
Gas NOT at STP
must use P V = n R T , no shortcut
Ex 4
E
Unit-trap (mL/L, cm³/m³)
numbers right, units wrong
Ex 5
F
Degenerate / limiting
V → 0 , mixture, "what if identity unknown"
Ex 6
G
Solid/liquid density
packing matters, 22.7 forbidden
Ex 7
H
Reverse: find M from density
measure ρ of gas → identify molecule
Ex 8
I
Word problem (real world)
strip the story to numbers
Ex 9
J
Exam twist (find %, comparison)
multi-part reasoning
Ex 10
Definition Symbols we will reuse (earned once, here)
m = mass in grams ( g ) .
V = volume; we keep track of whether it's litres ( L ) or cubic centimetres ( cm 3 ) .
n = number of moles ( mol ) — a count of 6.022 × 1 0 23 particles.
M = molar mass ( g mol − 1 ) — grams per one mole.
ρ (Greek "rho") = density ( g cm − 3 or g L − 1 ) .
V m = molar volume ( L mol − 1 ) — litres per one mole.
P , V , T , R = pressure, volume, temperature, gas constant in P V = n R T (see Ideal Gas Law PV=nRT ).
Worked example Example 1 — grams to moles
How many moles are in 8.0 g of helium? (M H e = 4.0 g mol − 1 )
Forecast: one mole of He weighs 4 g. We have 8 g — that's two full bags. Guess: 2 mol .
Pick the bridge. We stand on the mass island, want the moles island → molar-mass bridge n = M m .
Why this step? Only this bridge connects grams to moles.
Plug in: n = 4.0 g mol − 1 8.0 g = 2.0 mol .
Why this step? Dividing grams by grams-per-mole cancels grams and leaves mol.
Verify: units g / mol g = mol ✓. Matches forecast of 2 mol ✓.
Worked example Example 2 — mass of solid → volume of its gas at STP
6.6 g of dry ice (C O 2 , M = 44 g mol − 1 ) sublimes to gas at STP. What volume of gas? (V m = 22.7 L mol − 1 )
Forecast: 6.6 g is much less than 44 g, so less than one mole — expect less than 22.7 L. Guess a few litres.
Cross bridge 1 (mass → moles): n = 44 6.6 = 0.15 mol .
Why this step? We start on the mass island; volume of a gas is found through moles, not directly.
Cross bridge 2 (moles → volume): V = n V m = 0.15 × 22.7 = 3.405 L .
Why this step? Molar-volume bridge turns a count of moles into litres of gas.
Verify: 0.15 mol < 1 mol , and 3.4 L < 22.7 L ✓ — consistent with the forecast that we have a fraction of a mole.
Worked example Example 3 — density of a gas at STP
Find the density of nitrogen gas N 2 (M = 28 g mol − 1 ) at STP.
Forecast: one mole (28 g) fills 22.7 L, so density = 28 ÷ 22.7, a bit over 1 g/L. Guess ~1.2.
Use the gas density link ρ = V m M .
Why this step? One mole is simultaneously M grams and V m litres, so grams-per-litre is just their ratio — no particle counting needed. See Avogadro's Law .
ρ = 22.7 28 = 1.234 g L − 1 .
Verify: air is ~1.2 g/L and is mostly N₂ — perfectly sensible ✓.
Common mistake The 22.7 shortcut only works at STP
V m = 22.7 L mol − 1 is P R T evaluated at 273.15 K and 1 bar . Change T or P and that number changes. Off STP you must return to P V = n R T .
Worked example Example 4 — gas away from standard conditions
What volume does 0.50 mol of an ideal gas occupy at P = 2.0 × 1 0 5 Pa and T = 300 K ? (R = 8.314 J mol − 1 K − 1 )
Forecast: double the pressure and slightly higher temperature than STP — pressure squeezes volume down, so expect well under the 0.5 × 22.7 = 11.35 L we'd get at STP.
Rearrange the ideal gas law for volume: V = P n R T .
Why this step? We can't use V m — it's the wrong P , T . The law itself is always valid.
Plug in SI units: V = 2.0 × 1 0 5 0.50 × 8.314 × 300 = 6.24 × 1 0 − 3 m 3 .
Why this step? Joules and pascals give cubic metres.
Convert: 6.24 × 1 0 − 3 m 3 × 1000 = 6.24 L .
Verify: 6.24 L < 11.35 L ✓ — the extra pressure compressed the gas, exactly as forecast.
Worked example Example 5 — mL vs L / cm³ vs m³
A 500 mL sample of mercury has density 13.6 g cm − 3 . Find its mass.
Forecast: mercury is famously heavy; half a litre should be a hefty ~7 kg. Guess several kilograms.
Match the volume unit to the density unit. Density is per cm³ , so express volume in cm³: 500 mL = 500 cm 3 (they are identical).
Why this step? ρ = m / V is only numerically correct when V is in the same unit density uses.
m = ρ V = 13.6 × 500 = 6800 g = 6.8 kg .
Verify: the number 6800 g ≈ 6.8 kg matches the "several kilograms" forecast ✓. Had we sloppily left volume as "0.5 L" and multiplied by 13.6, we'd get 6.8 g — a 1000 × error, the classic mistake.
Intuition What happens at the edges?
Good problems test the boundaries: what if the volume is zero? What if you don't know the gas's identity? These "degenerate" cases reveal whether you actually understand the formulas.
Worked example Example 6 — the identity-independent limit
(a) As V → 0 for a fixed mass m , what does density ρ = m / V do?
(b) You have 1 mol of an unknown ideal gas at STP. Can you state its volume without knowing what it is?
Forecast: (a) shrinking the box while keeping the mass should make density blow up. (b) Avogadro says gas volume ignores identity, so yes.
(a) In ρ = V m , hold m fixed and let V → 0 + . The denominator shrinks toward zero, so ρ → + ∞ .
Why this step? Cramming any mass into no space means infinite density — a black-hole-like limit; physically it's why solids resist compression.
(b) By Avogadro's law every ideal gas has V m = 22.7 L mol − 1 at STP, independent of M . So V = 1 × 22.7 = 22.7 L .
Why this step? Molar volume is set by spacing (T , P ), not by molecule size. See STP and Standard Conditions .
Verify: (a) sign check — as V halves, ρ doubles; toward zero it diverges ✓. (b) Note the mass would differ per gas (via ρ = M / V m ), but the volume is fixed at 22.7 L ✓.
Worked example Example 7 — molar volume of liquid water (why it is NOT 22.7 L)
Liquid water has ρ = 1.00 g cm − 3 and M = 18 g mol − 1 . Find its molar volume.
Forecast: water is packed tight, not gas-spaced, so expect a tiny molar volume — nowhere near 22.7 L. Guess a few tens of mL.
Get the volume of one mole's worth of mass. One mole weighs M = 18 g .
Why this step? Molar volume V m = V / n ; for n = 1 mol we just need the volume of M grams.
Convert mass to volume using density: V = ρ m = 1.00 g cm − 3 18 g = 18 cm 3 = 18 mL .
Verify: 18 mL vs 22 700 mL for a gas — liquid water is ~1260× more compact ✓. This is exactly why "22.7 L applies to everything" is wrong: in liquids the molecules touch .
Worked example Example 8 — identify a mystery gas
An unknown ideal gas at STP has density ρ = 1.25 g L − 1 . What is its molar mass, and what might it be?
Forecast: its density is close to nitrogen's (1.23 from Ex 3), so expect M ≈ 28 — maybe N 2 or C O .
Invert the gas density link. From ρ = V m M solve for M : M = ρ V m .
Why this step? We know ρ and V m ; the only unknown is M , so rearrange for it.
M = 1.25 × 22.7 = 28.375 g mol − 1 ≈ 28 g mol − 1 .
Why this step? Multiplying grams-per-litre by litres-per-mole cancels litres, leaving grams-per-mole.
Verify: M ≈ 28 matches N 2 (or CO) ✓ — consistent with the forecast. This is how real chemists ID gases: measure density, compute M , look it up in Relative Atomic Mass & Atomic Mass Unit .
Worked example Example 9 — the propane tank
A cook uses propane C 3 H 8 (M = 44 g mol − 1 ). A tank holds 11 kg of propane. How many moles is that, and what volume would it occupy as a gas at STP?
Forecast: 11 kg = 11000 g; divide by 44 ≈ 250 mol; times 22.7 L ≈ 5700 L. That huge gas volume is why it's stored as a compressed liquid!
Strip the story to a mass: m = 11 kg = 11000 g .
Why this step? Formulas need grams; "a tank" is just m .
Bridge to moles: n = 44 11000 = 250 mol .
Bridge to gas volume: V = n V m = 250 × 22.7 = 5675 L .
Why this step? Same chain as Example 2 (mass→moles→volume), just bigger numbers.
Verify: 5675 L ≈ 5.7 m 3 — larger than most rooms ✓. Storing it as liquid (tiny volume) instead of gas is the whole point of a gas cylinder.
Worked example Example 10 — which balloon rises, and by how much lighter?
At STP, compare helium (M = 4 ) and air (M ˉ = 29 ) as gases. Find both densities and the percentage by which helium is lighter than air.
Forecast: helium is famously light — expect its density far below air's, and it should be roughly 85–90% lighter.
Density of each via ρ = M / V m :
ρ H e = 22.7 4 = 0.1762 g L − 1 , ρ ai r = 22.7 29 = 1.2775 g L − 1 .
Why this step? Same V m for both, so density just tracks M (Avogadro again).
Percentage lighter: ρ ai r ρ ai r − ρ H e × 100% = 1.2775 1.2775 − 0.1762 × 100% .
Why this step? "X % lighter than air" means the fractional drop relative to air .
= 1.2775 1.1013 × 100% = 86.2% .
Verify: shortcut — since V m cancels, the fraction is just 1 − 29 4 = 1 − 0.1379 = 86.2% ✓. Helium is ~86% lighter than air, so the balloon rises.
Recall Which bridge(s) does each case need?
Grams → moles ::: molar-mass bridge n = m / M (Case A)
Solid mass → gas volume at STP ::: two bridges, n = m / M then V = n V m (Case B)
Gas volume off STP ::: P V = n R T , NOT V m (Case D)
Density of a liquid's one mole ::: V = m / ρ with m = M (Case G)
Gas density → identity ::: M = ρ V m (Case H)
Mnemonic Solve any of them in 3 questions
"Where am I? Where do I want to be? Which bridge crosses the gap?" Island = mass / volume / moles. That's the entire method.