Buoyancy and StabilityWhat is the vertical force acting on a body which is completely submerged in a fluid? Answer to such a question can be very well found in the theory developed in the previous section. Archimedes seems to have discovered the laws concerning submerged bodies as well as floating bodies. What is well known as Archimedes principle states -
Proof is straight forward. Consider an elemental volume within the immersed body as shown in Fig.2.16 . Now the buoyant force is given by,
where is the area of cross section of the elemental volume chosen. We have from Eq. 2.48 It can be shown that the buoyant force, passes through the centroid of the displaced volume as shown in Fig.2.17. The point where this force acts is called "Center of Buoyancy", denoted as . The above result holds good even in the case of a partially submerged body i.e., a floating body. It is assumed that part of the body above the liquid level is in air. The weight of air displaced as a consequence is ignored. (Fig. 2.18). For this case as well,
The theory developed so far does hold good in case of a fluid for which specific gravity is not a constant, a layered fluid for example. However now the buoyant force may not act at the centroid of the displaced volume. The theory developed is also applicable where the fluid involved is a gas, say air. Convection currents established in atmosphere depend upon the buoyant forces generated.
Subsections (c) Aerospace, Mechanical & Mechatronic Engg. 2005 University of Sydney |