Water Displacement and Archimedes' Principle
Why a multi-ton steel ship floats and a small pebble sinks — the physics of displacement, the buoyancy formula behind it, and how to use it yourself.
Archimedes' principle states that any object submerged in water, fully or partly, experiences an upward buoyant force equal to the weight of the water it displaces. That one sentence explains why a steel ship carrying thousands of tons of cargo floats, why an ice cube bobs with most of its bulk hidden below the surface, and why dunking an odd-shaped object in a measuring cup is a reliable way to find its volume. The idea is more than 2,200 years old and it still underpins naval architecture, submarine design and laboratory measurement today.
Skip the math Water Displacement Calculator Open →What Archimedes' principle says
The principle is credited to the Greek mathematician Archimedes of Syracuse, who lived in the third century BC. According to a story recorded centuries later by the Roman architect Vitruvius, Archimedes was asked to determine whether a goldsmith had cheated the king by mixing silver into a crown that was supposed to be pure gold. He is said to have realized, while lowering himself into a bath and watching the water level rise, that an irregular object's volume could be measured by how much fluid it displaces — and, from there, that its density (and therefore what it was made of) could be worked out. The bathtub detail cannot be verified historically, but the physical insight is sound and is the basis for the principle that bears his name.
In modern terms: an object immersed in a fluid is pushed on from every direction by the surrounding fluid's pressure, and that pressure increases with depth. Because the bottom of a submerged object sits deeper than its top, the upward push on its underside is stronger than the downward push on its top. The net result is a single upward force called the buoyant force, and Archimedes' principle says its magnitude is exactly equal to the weight of the fluid the object has pushed out of the way — no more, no less, regardless of what the object itself is made of.
The core idea in one line. Buoyant force = weight of the fluid displaced. It does not depend on the object's own weight, shape or material — only on how much fluid it pushes aside.
What water displacement means
Displacement is simply the volume of water an object pushes out of the way when it enters the water. Drop any solid object into a full container and the water that spills over the rim has a volume exactly equal to the volume of the submerged part of the object. That is true whether the object floats on the surface with part of it sticking out, or sinks to the bottom fully covered.
Two cases matter here:
- Fully submerged objects (a rock on a lakebed, a submarine at cruising depth) displace a volume of water equal to their entire own volume.
- Floating objects (a boat, an ice cube, a beach ball) only displace water equal to the volume of the part that sits below the waterline. The part above the surface displaces nothing.
This is the mechanism behind the classic "overflow can" method used in physics labs to measure the volume of an oddly shaped object: submerge it completely in a container filled to the brim, catch the water that spills out, and measure that volume. It equals the object's own volume exactly, with no need to calculate the shape mathematically.
The buoyancy formula
Archimedes' principle turns into a simple, usable equation once you have three quantities: the density of the fluid, the volume displaced, and the local gravitational acceleration.
For everyday work in US units, it's easier to skip gravity entirely and use the fluid's weight density instead of mass density. Fresh water weighs about 62.4 pounds per cubic foot, so:
Whether that buoyant force is enough to make the object float depends on one comparison: is the buoyant force at full submersion greater than, equal to, or less than the object's actual weight? That comparison is covered next.
Why some things float and others sink
An object floats, sinks, or hangs suspended based on how its average density compares with the density of the fluid around it — not on how heavy it is in absolute terms. A loaded cargo ship weighing tens of thousands of tons floats, while a single steel bolt weighing a few grams sinks, because what matters is weight per unit of volume, not total weight.
| Material | Typical density vs. water | Behavior in water |
|---|---|---|
| Cork | about 0.24× as dense | Floats high |
| Ice | about 0.92× as dense | Floats, mostly submerged |
| Oak (dry) | about 0.75× as dense | Floats |
| Fresh water (reference) | 1.0× | — |
| Seawater | about 1.02–1.03× | Slightly more buoyant than fresh water |
| Aluminum (solid) | about 2.7× as dense | Sinks |
| Steel (solid) | about 7.8× as dense | Sinks |
| Gold (solid) | about 19.3× as dense | Sinks |
Solid steel sinks. A steel ship floats. The difference is shape, not material: a hull is a hollow shell that encloses a large volume of air. Spread the same mass of steel over a wide, hollow form and the vessel's average density, steel plus the air-filled space inside it, drops below the density of water. The ship settles into the water only until it has displaced a volume of water whose weight matches its own total weight, at which point the buoyant force and the weight balance and it floats at that draft.
Worked examples
A few concrete numbers make the relationship easier to picture. These are estimates for illustration, not lab-precise figures.
Rubber duck bath toy
≈ 0.03 lb
Displaces roughly a cubic inch of water to support its own light weight, floating almost entirely above the surface.
10-lb block of oak
≈ 7.5 lb submerged
About three-quarters of the block's volume sits below the waterline before it displaces enough water to balance its weight.
Solid steel cube, 1 ft³
62.4 lb buoyant force
Against roughly 490 lb of actual weight — nowhere near enough lift, so it sinks straight to the bottom.
Cargo ship hull
Thousands of tons
Settles lower as cargo is loaded, displacing more water until the buoyant force again matches the new, heavier total weight.
Real-world applications
Naval architecture. Every ship is designed around a target displacement: the weight of water it must push aside to float at a safe depth with its intended cargo. The Plimsoll line painted on a ship's hull marks the maximum safe draft for different water conditions, directly derived from displacement calculations.
Submarines. A submarine controls its depth by adjusting how much water it lets into or pumps out of its ballast tanks, changing its average density relative to seawater. Fill the tanks and the sub's weight exceeds the buoyant force at that volume, so it sinks; pump them out and it rises.
Hydrometers. These simple floating instruments measure the density of a liquid, battery acid, wine must, or antifreeze, by how deep they sink; a calibrated scale on the stem reads the density directly, based entirely on Archimedes' principle.
Volume measurement. Labs, jewelers and manufacturers use the overflow (displacement) method described earlier to measure the volume of irregularly shaped solids that can't be measured with a ruler.
Life jackets and diving weights. A life jacket adds low-density, air-filled volume to a swimmer to raise their average density below that of water; a diver's weight belt does the opposite, adding dense mass to counteract natural buoyancy so the diver can stay submerged.
Common misconceptions
"Heavy objects always sink." Not true — density, weight divided by volume, is what matters, not total weight. A massive aircraft carrier floats; a small dense pebble sinks.
"Buoyant force gets stronger the deeper you go." For a fully submerged, rigid object, the buoyant force stays essentially constant with depth. Water is nearly incompressible, so its density barely changes as pressure increases, and the object's displaced volume doesn't grow just because it's deeper.
"Shape doesn't matter, only material does." Shape matters enormously, because it determines how much volume, and therefore how much water, an object can displace before going fully underwater. The same mass of steel sinks as a solid block and floats as a hollow hull.
"Displacement and buoyancy are the same thing." They're related but distinct: displacement is the volume of fluid moved aside, while buoyancy is the resulting upward force. Displacement is the cause; buoyant force is the measurable effect.
The bottom line
Archimedes' principle reduces a seemingly complicated question, will this float?, to one comparison: does the object's weight exceed the weight of the water it can displace? Get the volume displaced and the fluid's density, multiply them (times gravity, or just use a weight-density figure like 62.4 lb/ft³ for fresh water), and you have the buoyant force. Compare that number to the object's actual weight and you know whether it floats, sinks, or hangs in balance. It's the same arithmetic whether you're sizing a toy boat or a cargo ship.
Frequently asked questions
What is Archimedes' principle in simple terms?
Any object placed in water, whether it floats or sinks, pushes aside (displaces) a volume of water equal to the part of the object that is underwater. The water pushes back with an upward force equal to the weight of that displaced water. If that upward force matches the object's own weight, it floats; if not, it sinks.
How do you calculate buoyant force?
Buoyant force equals the weight density of the fluid multiplied by the volume of fluid displaced: Fb = ρ × V × g. In everyday units, buoyant force in pounds equals the volume displaced in cubic feet times 62.4, the weight density of fresh water.
Why do steel ships float if steel is denser than water?
A solid block of steel sinks because it's about eight times denser than water. A ship's hull is a hollow shell, so the vessel as a whole, steel plus the air-filled space inside it, has an average density lower than water. It displaces enough water to generate a buoyant force equal to its total weight, so it floats even though the steel itself would sink.
What is the difference between water displacement and buoyancy?
Displacement is the act of an object pushing water out of the way, and the volume of water that gets moved. Buoyancy is the upward force that results from that displacement. Displacement is the cause; buoyancy is the effect Archimedes' principle describes.
Did Archimedes really discover this in a bathtub?
That's the popular legend, recorded centuries later by the Roman writer Vitruvius: Archimedes is said to have noticed the water level rise as he lowered himself into a bath and shouted "Eureka." Historians can't verify the bathtub detail, but the underlying physics he's credited with, that displaced volume reveals density, is sound and still used today.
Does the shape of an object affect whether it floats?
Yes, indirectly. Shape doesn't change how much an object weighs, but it changes how much water the object can displace before going fully underwater. A flat, wide, hollow shape displaces more water at a shallow draft than a compact, solid shape of the same weight — which is why a bowl-shaped hull floats and a solid lump of the same material and mass may not.
Is the buoyant force on an object the same at any depth underwater?
For a fully submerged, rigid object, essentially yes. Once it's completely underwater, it displaces the same volume regardless of depth, and water is nearly incompressible, so its density barely changes with depth. The buoyant force stays practically constant until pressure at extreme depth becomes large enough to compress the object itself.
Sources & references
The physics in this guide follows standard reference treatments of buoyancy and fluid density:
- NASA Glenn Research Center — Buoyancy: Archimedes Principle. Statement of the principle and worked buoyancy problems.
- HyperPhysics, Georgia State University Department of Physics & Astronomy — Buoyancy. Derivation of the buoyant-force equation from fluid pressure.
- Encyclopaedia Britannica — Archimedes' Principle. History and statement of the law of buoyancy.
- U.S. Geological Survey, Water Science School — Water Density. Reference density values for fresh water used in the calculations above.