Categories: Fluid mechanics, Fluid statics, Physics.

# Archimedes’ principle

Many objects float when placed on a liquid,
but some float higher than others,
and some do not float at all, sinking instead.
**Archimedes’ principle** balances the forces,
and predicts how much of a body is submerged,
and how much is non-submerged.

In truth, there is no real distinction between the submerged and non-submerged parts, since the latter is surrounded by another fluid (air), which has a pressure and thus affects it. The right thing to do is treat the entire body as being submerged in a fluid with varying properties.

Let us consider a volume $V$ completely submerged in such a fluid. This volume will experience a downward force due to gravity, given by:

$\begin{aligned} \va{F}_g = \int_V \va{g} \rho_\mathrm{b} \dd{V} \end{aligned}$Where $\va{g}$ is the gravitational field, and $\rho_\mathrm{b}$ is the density of the body. Meanwhile, the pressure $p$ of the surrounding fluid exerts a force on the entire surface $S$ of $V$:

$\begin{aligned} \va{F}_p = - \oint_S p \dd{\va{S}} = - \int_V \nabla p \dd{V} \end{aligned}$Where we have used the divergence theorem.
Assuming hydrostatic equilibrium,
we replace $\nabla p$,
leading to the definition of the **buoyant force**:

For the body to be at rest, we require $\va{F}_g + \va{F}_p = 0$. Concretely, the equilibrium condition is:

$\begin{aligned} \boxed{ \int_V \va{g} (\rho_\mathrm{b} - \rho_\mathrm{f}) \dd{V} = 0 } \end{aligned}$It is commonly assumed that $\va{g}$ is constant everywhere, with magnitude $\mathrm{g}$. If we also assume that $\rho_\mathrm{f}$ is constant on the “submerged” side, and zero on the “non-submerged” side, we find:

$\begin{aligned} 0 = \mathrm{g} (m_\mathrm{b} - m_\mathrm{f}) \end{aligned}$In other words, the mass $m_\mathrm{b}$ of the entire body is equal to the mass $m_\mathrm{f}$ of the fluid it displaces. This is the best-known version of Archimedes’ principle.

Note that if $\rho_\mathrm{b} > \rho_\mathrm{f}$, then the displaced mass $m_\mathrm{f} < m_\mathrm{b}$ even if the entire body is submerged, and the object will therefore continue to sink.

## References

- B. Lautrup,
*Physics of continuous matter: exotic and everyday phenomena in the macroscopic world*, 2nd edition, CRC Press.