51.1: Archimedes’ Principle
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One of the simplest principles of fluid statics is Archimedes' principle, which states that if a body is wholly or partially submerged in a fluid, then it is buoyed upward by a buoyant force B equal to the weight of the displaced fluid:
B=W
where B is the buoyant force, and W=ρgV is the weight of the displaced fluid: ρ is the density of fluid displaced, V is the volume of fluid displaced, and g is the acceleration due to gravity.
Suppose we have a body of volume V and density ρb completely submerged in a fluid of density ρf. What will happen? There will be two forces acting on the body: the weight of the body, acting downward 1 ( W=−ρbVg ), and the buoyant force, acting upward (B=ρfVg). The net force is then F=B+W= (ρf−ρb)Vg. This implies that:
- If ρb=ρf (the body is the same density as the fluid), then there is no net force on the body.
- If ρb<ρf (the body is less dense than the fluid), then F>0 and there is a net upward force on the body: the body will float up toward the surface.
- If ρb>ρf (the body is denser than the fluid), then F<0 and there is a net downward force on the body: the body will sink.
1 We take positive to be upward, and negative downward.