Buoyancy and Archimedes' Principle — The Complete Physics Guide
Buoyancy is the upward force exerted by a fluid on any object immersed in it. Archimedes' Principle — discovered around 250 BCE and still the cornerstone of fluid statics — states that this buoyant force equals the weight of fluid displaced by the object. This single principle explains why ships float, submarines dive, hot air balloons rise, and fish hover effortlessly at any depth.
Legend holds that Archimedes discovered the principle while stepping into an overfull bath and noticing the water overflow. He reportedly ran naked through the streets of Syracuse shouting "Eureka!" (I have found it). Whether true or not, the story captures the power of the insight — a simple observation leading to a universal physical law.
Archimedes' Principle — The Physics
The buoyant force arises from the pressure difference between the bottom and top of a submerged object. Fluid pressure increases with depth (P = ρgh), so the pressure on the bottom of an object is higher than on its top. The net upward force from this pressure difference equals the weight of fluid displaced.
Mathematically: F_b = ρ_fluid × V_displaced × g. Where ρ_fluid is the fluid density (kg/m³), V_displaced is the volume of fluid displaced (m³), and g = 9.81 m/s². The buoyant force depends only on the displaced fluid volume and the fluid density — not on the object's material, shape, or density.
An object floats when F_b ≥ weight (mg). At equilibrium, F_b = mg, meaning ρ_fluid × V_displaced × g = ρ_object × V_object × g. If the object is fully submerged, V_displaced = V_object, giving the condition for floating when fully submerged: ρ_object ≤ ρ_fluid. If ρ_object > ρ_fluid, the object sinks. If ρ_object < ρ_fluid, it floats partially submerged, displacing only the volume of fluid whose weight equals its own weight.
Worked Example 1 — Steel Ball in Water
Problem: A solid steel ball (ρ = 7,800 kg/m³) of diameter 5 cm is submerged in water (ρ = 1,000 kg/m³). Find the buoyant force and the apparent weight.
V = (4/3)π(0.025)³ = 6.545 × 10⁻⁵ m³
F_b = ρ_water × V × g = 1000 × 6.545 × 10⁻⁵ × 9.81 = 0.642 N
True weight = ρ_steel × V × g = 7800 × 6.545 × 10⁻⁵ × 9.81 = 5.01 N
Apparent weight = 5.01 − 0.642 = 4.37 N — the ball feels lighter when weighed underwater.
Worked Example 2 — Ship Floating
Problem: A ship has mass 50,000 tonnes (5 × 10⁷ kg). What volume of seawater (ρ = 1,025 kg/m³) must it displace to float?
At equilibrium: F_b = weight → ρ_seawater × V × g = mg
V = m/ρ_seawater = 5×10⁷/1025 = 48,780 m³ — roughly the volume of 20 Olympic swimming pools. The ship's hull must enclose this displaced volume, which is why large ships have hollow hulls rather than being solid steel.
Apparent Weight and Density Measurement
The apparent weight of an object immersed in fluid is W_apparent = W_true − F_b = mg − ρ_fluid × V × g. Rearranging: ρ_object = ρ_fluid × W_true/(W_true − W_apparent). This allows density measurement using only two weight measurements — true weight in air and apparent weight submerged in water. This is exactly Archimedes' original method for testing whether Hiero's crown was pure gold.
Modern applications: hydrostatic weighing for body composition measurement (more accurate than BMI), measuring densities of geological samples, quality control testing of cast metal components, and calibrating precision instruments.
Submarines, Fish and Neutral Buoyancy
A submarine achieves neutral buoyancy (neither rising nor sinking) by adjusting the amount of water in ballast tanks. Adding water increases the submarine's effective density until it equals the surrounding seawater — the submarine then floats at constant depth. Expelling water (using compressed air) reduces density — the submarine rises. This simple mechanism, based entirely on Archimedes' Principle, enables precise depth control.
Fish achieve the same result biologically using a swim bladder — a gas-filled organ they expand or contract to adjust their overall density. Bony fish (teleosts) use this to hover at any depth with minimal muscular effort. Sharks, lacking a swim bladder, must swim continuously to maintain depth — they sink when they stop moving.
Hot air balloons work by the same principle in air. Heating the air inside the envelope reduces its density below ambient air — the balloon now displaces air that weighs more than the total weight of balloon plus payload. The net buoyant force lifts the balloon. Descending is achieved by cooling the air (allowing it to vent) or by venting hot air through the parachute valve.