Mechanical Engineer's Handbook

Archimedes' Principle and Buoyancy

Archimedes' Principle and the buoyant force govern objects submerged in or floating on fluids.

The Buoyant Force

The buoyant force is the upward force exerted by a fluid on any object submerged in it.

Because pressure in a fluid increases with depth (p=hρgp = h \rho g), the upward force pushing on the bottom of a submerged object is greater than the downward force on its top. This net upward force is present whether the object floats, sinks, or remains suspended.

An object's floating or sinking behavior depends on the balance between the buoyant force and its weight:

  • Sinks: Buoyant force is less than the object's weight (FB<wobjF_B < w_{\text{obj}}).
  • Floats/Suspended: Buoyant force equals the object's weight (FB=wobjF_B = w_{\text{obj}}).

Archimedes' Principle

The buoyant force on an object equals the weight of the fluid it displaces:

FB=wfl=mflg=ρflVflgF_B = w_{\text{fl}} = m_{\text{fl}} g = \rho_{\text{fl}} V_{\text{fl}} g
(1)

Density and Floating

An object's average density (ρobj\rho_{\text{obj}}) determines whether it floats or sinks relative to the fluid's density (ρfl\rho_{\text{fl}}):

  • ρobj<ρfl\rho_{\text{obj}} < \rho_{\text{fl}}: The object floats because displacing its entire volume yields a fluid weight greater than its own weight.
  • ρobj>ρfl\rho_{\text{obj}} > \rho_{\text{fl}}: The object sinks.

Example: A lump of clay sinks in water, but molding the same lump into the shape of a boat allows it to float. The boat shape displaces a larger volume of water without changing mass, creating a greater buoyant force.

Fraction Submerged

For a floating object in equilibrium, its mass equals the mass of displaced fluid (mobj=mflm_{\text{obj}} = m_{\text{fl}}). Substituting m=ρVm = \rho V yields the fraction of the object's volume submerged:

Fraction Submerged=VsubVobj=ρobjρfl\text{Fraction Submerged} = \frac{V_{\text{sub}}}{V_{\text{obj}}} = \frac{\rho_{\text{obj}}}{\rho_{\text{fl}}}
(2)

Apparent Weight

When an object is weighed while completely submerged, it suffers an apparent weight loss equal to the weight of the displaced fluid:

wapparent=wobjFB=wobjwflw_{\text{apparent}} = w_{\text{obj}} - F_B = w_{\text{obj}} - w_{\text{fl}}
(3)

Measuring an object's true weight in air and its apparent weight submerged allows determination of unknown densities.

Example 1

A 60.0 kg60.0\text{ kg} person floats in fresh water (ρfl=1000 kg/m3\rho_{\text{fl}} = 1000\text{ kg/m}^3) with 97.0%97.0\% of her volume submerged when her lungs are full of air. What is her average density?

Rearrange Equation 2 to solve for ρobj\rho_{\text{obj}} using the fraction submerged.

Using Equation 2:

VsubVobj=ρpersonρfl\frac{V_{\text{sub}}}{V_{\text{obj}}} = \frac{\rho_{\text{person}}}{\rho_{\text{fl}}}
ρperson=(Fraction Submerged)ρfl=(0.970)(1000 kg/m3)=970 kg/m3\rho_{\text{person}} = \left(\text{Fraction Submerged}\right) \cdot \rho_{\text{fl}} = (0.970)(1000\text{ kg/m}^3) = 970\text{ kg/m}^3

Example 2

A solid metal crown weighs 24.5 N24.5 \text{ N} in air. When completely submerged in fresh water (ρfl=1000 kg/m3\rho_{\text{fl}} = 1000 \text{ kg/m}^3), its apparent weight is measured to be 22.6 N22.6 \text{ N}. Find the average density of the crown.

Find the buoyant force using FB=wobjwapparentF_B = w_{\text{obj}} - w_{\text{apparent}}, then relate FBF_B to the displaced fluid volume to calculate ρobj\rho_{\text{obj}}.

First, find the buoyant force from the apparent weight loss (Equation 3):

FB=wobjwapparent=24.5 N22.6 N=1.90 NF_B = w_{\text{obj}} - w_{\text{apparent}} = 24.5 \text{ N} - 22.6 \text{ N} = 1.90 \text{ N}

Since the crown is fully submerged, the volume of displaced water equals the volume of the crown (Vfl=VobjV_{\text{fl}} = V_{\text{obj}}). Use Archimedes' Principle (Equation 1) to find this volume:

FB=ρflVobjg    Vobj=FBρflg=1.90 N(1000 kg/m3)(9.80 m/s2)1.939104 m3F_B = \rho_{\text{fl}} V_{\text{obj}} g \implies V_{\text{obj}} = \frac{F_B}{\rho_{\text{fl}} g} = \frac{1.90 \text{ N}}{(1000 \text{ kg/m}^3)(9.80 \text{ m/s}^2)} \approx 1.939 \cdot 10^{-4} \text{ m}^3

Calculate the mass of the crown from its true weight:

mobj=wobjg=24.5 N9.80 m/s2=2.50 kgm_{\text{obj}} = \frac{w_{\text{obj}}}{g} = \frac{24.5 \text{ N}}{9.80 \text{ m/s}^2} = 2.50 \text{ kg}

Calculate the crown's average density:

ρobj=mobjVobj=2.50 kg1.939104 m31.29104 kg/m3\rho_{\text{obj}} = \frac{m_{\text{obj}}}{V_{\text{obj}}} = \frac{2.50 \text{ kg}}{1.939 \cdot 10^{-4} \text{ m}^3} \approx 1.29 \cdot 10^4 \text{ kg/m}^3