Understanding the Buoyancy Experiment
This tool implements the classic hydrostatic-weighing experiment used to teach and apply Archimedes' principle: any object submerged in a fluid experiences an upward buoyant force equal to the weight of the fluid it displaces. Weigh an object in air, then weigh it again while fully submerged in a fluid (usually water) using a hanging scale or a balance and a thread — the object always appears lighter underwater, and that apparent loss of mass is exactly the mass of the fluid it pushed out of the way.
The formulas
Let m_air and m_fluid be the mass readings in air and submerged (in kilograms), ρ_fluid the fluid's density, and g the local gravitational acceleration:
- Mass of displaced fluid: Δm = m_air − m_fluid
- Buoyant force: F₌ = Δm × g (Newtons) — equivalently F₌ = ρ_fluid × V × g
- Displaced volume: V = Δm / ρ_fluid (this equals the object's own volume, since it is fully submerged)
- Object density: ρ_object = m_air / V
- Specific gravity: SG = ρ_object / 1000 kg/m³ (density relative to pure water)
Notice that gravity cancels out of the density calculation entirely — V = Δm / ρ_fluid does not contain g. That is why this method works the same on a lab bench regardless of the local value of g; the gravity field only affects how much force the scale itself reads in Newtons, not the density result.
Common reference densities
- Water (4°C): 1000 kg/m³ — the standard specific-gravity reference.
- Seawater: about 1025 kg/m³.
- Aluminum: about 2700 kg/m³.
- Steel/iron: about 7750–8050 kg/m³.
- Gold (pure, 24k): about 19,300 kg/m³.
Why it works
A submerged object pushes fluid out of the space it occupies. That displaced fluid "wants" to return to its original position and the surrounding fluid pressure resists the object, producing an upward force equal to the weight of the fluid displaced. Because the scale can only report the net downward force, the reading in fluid is smaller than in air by exactly that buoyant force — a mass-equivalent drop of Δm. Since Δm/ρ_fluid gives volume regardless of the object's shape, this method finds the density of oddly shaped objects (rocks, castings, jewelry) without ever measuring their dimensions directly.