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Upthrust

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A body immersed, partially or wholly, in a fluid experiences an upthrust U pushing it against gravity with magnitude equal to the weight of the fluid displaced by the body. This buoyancy principle was first discovered by Archimedes.
 
Consider a cylinder of height h and area A made of a material of density \rho, immersed in a fluid of density \sigma.

The weight of the cylinder can also be expressed as

mg=\rho hAg

If the object is in equilibrium,

P_{2}A-P_{1}A-mg=0

The buoyant force on the cylinder is given by

U=P_{2}A-P_{1}A=\left(P_{2}-P_{1}\right)A

The pressure difference \left(P_{2}-P_{1}\right) is given by

P_{2}-P_{1}=h\sigma g

Therefore, the buoyant force, or upthrust U, is equal to

U=\sigma hAg

which is the weight of the fluid displaced.

Last Updated on Wednesday, 25 August 2010 11:20  

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