FA = ρ·g·V
Buoyancy force equals the weight of the displaced fluid, regardless of the submerged body's shape, mass or material.
Buoyancy force equals the weight of the displaced fluid, regardless of the submerged body's shape, mass or material.
Select a target and calculate.
Buoyancy force equals the weight of the displaced fluid, regardless of the submerged body's shape, mass or material.
ρ=1,000 kg/m³, g=9.81 m/s² and V=10 l (0.01 m³) give FA≈98.07 N.
Fully submerged, rigid body in a homogeneous fluid under gravity; surface tension, flow forces and partially submerged (floating) bodies with an equilibrium condition are excluded.
This calculator determines the static buoyancy force on a fully submerged body, one of the oldest and most fundamental principles of fluid mechanics.
Per Archimedes, buoyancy force equals the weight of the fluid displaced by the body: FA=ρ·g·V, where V is displaced volume and ρ the fluid's density.
FA = ρ·g·V
FA = ρ·g·V| Symbol / input | Meaning |
|---|---|
| Buoyancy force FA | Upward force the fluid exerts on the submerged body. |
| Fluid density ρ | Density of the displaced fluid; water at 4 °C is exactly 1,000 kg/m³. |
| Gravitational acceleration g | Local gravitational acceleration, about 9.81 m/s² near sea level. |
| Displaced volume V | Volume of the fully submerged part of the body, which displaces the fluid. |
ρ is the density of the fluid the body is submerged in, g gravitational acceleration and V the volume displaced by the body.
Take ρ from material tables (water 1,000 kg/m³, seawater about 1,025 kg/m³, air about 1.2 kg/m³), compute V from the geometry of the submerged part.
ρ=1,000 kg/m³, g=9.81 m/s² and V=10 l (0.01 m³) give FA≈98.07 N.
Buoyancy force depends only on displaced volume and fluid density, not on the body's mass or material; whether a body floats or sinks is decided by comparison with its weight force.
ρ is a density, g an acceleration and V a volume. FA is output as a force.
Sizing floats, submerged bodies and ballast tanks, estimating weight reduction of submerged components, and fundamental physics teaching.
Fully submerged, rigid body in a homogeneous, still fluid; surface tension, flow forces and the floating case with equilibrium between buoyancy and weight (only partially submerged) are not included.
Common mistake: Do not use the total volume of a partially submerged body; V is only the submerged portion.
Sizing floats, submerged bodies and ballast tanks, estimating weight reduction of submerged components, and fundamental physics teaching.
ρ is the density of the fluid the body is submerged in, g gravitational acceleration and V the volume displaced by the body.
Fully submerged, rigid body in a homogeneous, still fluid; surface tension, flow forces and the floating case with equilibrium between buoyancy and weight (only partially submerged) are not included.