The density formula, ρ = m/V, defines density as an object’s mass divided by the volume it occupies. Density (ρ) tells you how much matter is packed into a given space, and is measured in kilograms per cubic metre (kg/m³). A higher density means more mass squeezed into the same volume.
Pick up a cricket ball and a party balloon of roughly the same size. The ball thuds into your palm; the balloon barely registers. Same volume, wildly different mass — and that gap has a name: density.
Density is why steel ships float while a steel nail sinks, why oil sits on top of vinegar in your salad dressing, and why a hot-air balloon climbs. Get this single idea straight and a surprising amount of the physical world falls into place.
What Is Density?
Density answers a simple question: for a given lump of stuff, how much matter is crammed into the space it takes up? Two objects can be identical in size yet feel completely different in the hand, because one packs far more mass into that volume.
Formally, density is the mass of a substance per unit of volume. Physicists label it with the Greek letter ρ (pronounced “rho”).
Here’s the part students often miss. Density is a property of the material itself, not of how much of it you have. A teaspoon of mercury and a whole bucket of mercury share exactly the same density. Double the sample and you double both the mass and the volume, so their ratio — the density — doesn’t budge.
Two boxes of equal volume: pack in more mass and the density rises.
The Density Formula: ρ = m/V
The whole idea fits in one short equation.
In plain words: divide an object’s mass by the volume it fills. Each symbol carries an SI unit:
- ρ (rho) — density, in kilograms per cubic metre (kg/m³)
- m — mass, in kilograms (kg)
- V — volume, in cubic metres (m³)
Because the three quantities are tied together, knowing any two gives you the third. Rearranging for mass:
And rearranging for volume:
That’s the same relationship read three different ways — handy for the “density triangle” some teachers draw. To skip the arithmetic, drop your numbers into our Density Calculator, which solves for density, mass or volume.
How to Calculate Density Step by Step
Finding a density in the lab comes down to three moves: get the mass, get the volume, then divide.
Step 1 — Measure the mass. Place the object on a balance and read the mass in grams or kilograms. This is the easy part.
Step 2 — Measure the volume. For a neat shape, use geometry: a cuboid is length × width × height, a sphere is (4/3)πr³. For an awkward, lumpy object, geometry fails — so you use displacement instead.
The displacement trick: lower the object into a measuring cylinder of water and read how far the level rises. The volume of water pushed aside equals the volume of the object. A stone that lifts the level from 50 mL to 85 mL has a volume of 35 cm³ (since 1 mL = 1 cm³).
Step 3 — Divide. Put the numbers into ρ = m/V and keep your units consistent. In practice, the most common slip is mixing grams with cubic metres — convert one so both match before dividing.
Density Units: kg/m³, g/cm³ and Specific Gravity
The SI unit of density is the kilogram per cubic metre (kg/m³) — mass in kg over volume in m³, exactly as the units of a derived quantity should combine (see the NIST guide to SI units). It’s the right unit for engineering, but the numbers get large: water comes out as 1000 kg/m³.
So in the lab you’ll often meet grams per cubic centimetre (g/cm³) instead, where water is a tidy 1.00. Note that g/cm³ and g/mL are the same thing, because 1 mL = 1 cm³.
Switching between the two units uses one fixed factor:
- 1 g/cm³ = 1000 kg/m³. To go from g/cm³ to kg/m³, multiply by 1000; to go back, divide by 1000.
Why 1000? Because a gram is one-thousandth of a kilogram while a cubic centimetre is one-millionth of a cubic metre — and 10⁻³ divided by 10⁻⁶ is 10³.
You’ll also hear about relative density (older name: specific gravity). That’s simply a material’s density divided by the density of water. It carries no units, and it tells you at a glance whether something floats on water: less than 1 floats, more than 1 sinks. Aluminium’s relative density is about 2.7, so it sinks.
Real-World Examples of Density
Densities span an enormous range, from wispy gases to metals that feel impossibly heavy for their size. The table below lists everyday materials at ordinary conditions.
| Material | Density (kg/m³) | Density (g/cm³) | In water |
|---|---|---|---|
| Air (sea level) | ≈ 1.2 | ≈ 0.0012 | far less dense |
| Cork | 240 | 0.24 | floats |
| Ice (0 °C) | 917 | 0.917 | floats |
| Fresh water (4 °C) | 1000 | 1.000 | reference |
| Seawater | 1025 | 1.025 | denser than fresh |
| Aluminium | 2700 | 2.70 | sinks |
| Iron | 7870 | 7.87 | sinks |
| Lead | 11 340 | 11.34 | sinks |
| Mercury | 13 534 | 13.53 | sinks (liquid metal) |
| Gold | 19 300 | 19.30 | sinks |
| Osmium | 22 590 | 22.59 | densest natural element |
A few highlights are worth pausing on. Air still has mass — about 1.2 kg sits in every cubic metre of the room around you. At the other extreme, osmium is the densest naturally occurring element, roughly 22,590 kg/m³, about twice as dense as lead and a whisker ahead of iridium.
Water is the quiet star of the table. Its density is famously close to 1 g/cm³ — more precisely 0.9998 g/cm³ at 4 °C, the temperature at which water is densest, according to the USGS Water Science School. Warm it or cool it below that point and it expands slightly, becoming a touch less dense.
Why Do Objects Float or Sink?
Forget weight for a moment. Whether something floats has almost nothing to do with how heavy it is and everything to do with how its density compares to the fluid around it.
The rule is short: an object floats if it is less dense than the fluid, and sinks if it is denser. This is Archimedes’ principle in disguise — a submerged object is pushed up by the weight of fluid it displaces, and a low-density object can displace enough fluid to hold itself up.
For a floating object, the fraction submerged equals its density divided by the fluid’s density.
That last point is quietly powerful. Ice has a density of about 917 kg/m³ and seawater about 1025 kg/m³, so 917/1025 ≈ 0.90 — which is why roughly 90% of an iceberg hides below the surface, with only a tenth showing.
It also explains the steel-ship puzzle. Solid steel sinks, yet a ship floats, because what counts is the ship’s average density — steel hull plus a vast volume of air inside. Spread the same mass over a big hollow shape and the average density drops below water’s.
One last party trick: lead sinks in water but floats on mercury, because lead (11,340 kg/m³) is less dense than liquid mercury (13,534 kg/m³). Float and sink are always relative to the fluid.
Common Misconceptions About Density
Density is intuitive enough to feel obvious — which is exactly why a few wrong ideas stick. Here are the big ones.
“Heavier objects are always denser”
Not so. A kilogram of feathers and a kilogram of lead have the same mass, yet the feathers fill a sack while the lead is a small block. Density compares mass and volume together; a large light object can easily out-mass a tiny dense one while being far less dense.
“Density depends on how much you have”
It doesn’t. Density is an intensive property — snap a metal bar in half and each piece keeps the same density as the whole. In that respect it behaves like specific heat capacity: a fixed characteristic of the material, independent of sample size.
“Density is based on weight”
The formula uses mass (kg), not weight (newtons). It’s a subtle distinction that matters: carry a rock to the Moon and its weight drops to a sixth, but its mass — and therefore its density — is unchanged.
“If it sinks, it must be heavy”
Sinking is about density relative to the fluid, not raw weight. A 100-tonne ship floats; a 5-gram steel bolt sinks. The bolt loses not because it’s heavy, but because it’s denser than water.
How Density Connects to Weight, Pressure and Buoyancy
Density rarely works alone — it threads through much of mechanics, especially anything involving fluids.
Weight. Density needs mass, and mass is what links to weight through W = mg. Keeping mass and weight straight is the same care you take with Newton’s second law, where force depends on mass, not on how heavy something happens to feel under local gravity.
Pressure in a fluid. The pressure at a depth h in a still fluid is P = ρgh — denser fluids build pressure faster with depth. That’s why deep-sea pressure is crushing and why mercury barometers are short while a water version would need to be over ten metres tall.
Drag and falling. When an object falls through air or water, both its own density and the fluid’s density help set how fast it ends up moving. That balance is the heart of terminal velocity — a denser object, or a thinner fluid, means a higher final speed.
Worked Problems
Show Solution
Step 1: Use ρ = m/V.
Step 2: ρ = 240 g ÷ 100 cm³ = 2.4 g/cm³.
Step 3: Convert: 2.4 g/cm³ × 1000 = 2400 kg/m³. Since 2.4 g/cm³ is greater than water’s 1.0 g/cm³, it sinks.
Answer: 2.4 g/cm³ = 2400 kg/m³; it sinks.
Show Solution
Step 1: Rearrange to m = ρ × V.
Step 2: m = 1000 kg/m³ × 2.0 m³.
Step 3: m = 2000 kg.
Answer: 2000 kg (2 tonnes).
Show Solution
Step 1: Rearrange to V = m/ρ.
Step 2: V = 0.500 kg ÷ 19 300 kg/m³ = 2.59 × 10⁻⁵ m³.
Step 3: Convert: 2.59 × 10⁻⁵ m³ × 10⁶ = 25.9 cm³.
Answer: ≈ 25.9 cm³ (about the size of a large dice).
Show Solution
Step 1: Volume = level rise = 85.0 − 50.0 = 35.0 mL = 35.0 cm³.
Step 2: Apply ρ = m/V = 87.5 g ÷ 35.0 cm³.
Step 3: ρ = 2.50 g/cm³ = 2500 kg/m³ (denser than water, so it sinks).
Answer: 2.50 g/cm³ = 2500 kg/m³.
Show Solution
Step 1: Compare densities. 850 is less than 1000, so it floats in water.
Step 2: Fraction submerged = object density ÷ fluid density = 850 ÷ 1000 = 0.85 (85%).
Step 3: In oil, 850 is still less than 920, so it floats; submerged fraction = 850 ÷ 920 = 0.92 (92%).
Answer: Floats in both; 85% submerged in water, 92% in oil.
Show Solution
Step 1: Convert: 13.53 g/cm³ × 1000 = 13 530 kg/m³.
Step 2: Compare with iron at 7870 kg/m³.
Step 3: 7870 is less than 13 530, so iron is less dense than mercury and floats on it.
Answer: 13 530 kg/m³; yes, iron floats on mercury.
Show Solution
Step 1: Relative density = substance density ÷ water density.
Step 2: RD = 1260 ÷ 1000.
Step 3: RD = 1.26 (a pure number, with no units).
Answer: Relative density = 1.26.
Show Solution
Step 1: Find each volume with V = m/ρ. V(A) = 300 ÷ 0.60 = 500 cm³; V(B) = 300 ÷ 1.20 = 250 cm³.
Step 2: Total mass = 600 g; total volume = 500 + 250 = 750 cm³.
Step 3: ρ = 600 ÷ 750 = 0.80 g/cm³. It isn’t the simple average (0.90) because the lighter liquid takes up more volume, so it weights the result toward its own low density.
Answer: 0.80 g/cm³.