Archimedes Principle

004-archimedes.gif
Archimedes (287-212 B.C.)

Any body immersed in a fluid is subjected to an upward force called buoyant force equal to the weight of the displaced fluid.
 

$BF = \gamma V_D$

 

Where
$BF$ = buoyant force
$\gamma$ = unit weight of fluid
$V_D$ = volume of fluid displaced by the body
 

Buoyant force acting on a body submerged in fluid is merely the resultant of two vertical hydrostatic forces. Consider the cylindrical body shown below to have some length perpendicular to the drawing. The horizontal components of hydrostatic force acting on the body are in equilibrium because the vertical projection of the body in opposite sides is the same.
 

004-proof-of-buoyancy.gif

 

The upward force   $F_{V1}$   is the total force exerted by the fluid on the under surface of the body; the downward force   $F_{V2}$   is the total force exerted by the fluid on the upper surface of the body. Since liquid pressure increases by depth,   $F_{V1}$   is greater than   $F_{V2}$.   The difference   $F_{V1} - F_{V2}$   is therefore upward, and this difference is the buoyant force.
 

For homogeneous body of volume   $V$   "floating" in a homogeneous liquid at rest, the volume displaced is
 

$V_D = \dfrac{sg_{body}}{sg_{fluid}}V = \dfrac{\gamma_{body}}{\gamma_{fluid}}V$

 

For a floating body of height   $H$   and constant cross-sectional area parallel to the liquid surface, the submerged length   $D$   is given by
 

004-horizontal-area.gif

 

$D = \dfrac{sg_{body}}{sg_{fluid}}H = \dfrac{\gamma_{body}}{\gamma_{fluid}}H$

 

For a floating body whose cross-sectional area   $A$   is perpendicular to the liquid surface, the area submerged is given by
 

004-vertical-area.gif

 

$A_s = \dfrac{sg_{body}}{sg_{fluid}}A = \dfrac{\gamma_{body}}{\gamma_{fluid}}A$

 

Stability of Floating Bodies

Any floating body is subjected by two opposing vertical forces. One is the body's weight W which is downward, and the other is the buoyant force BF which is upward. The weight is acting at the center of gravity G and the buoyant force is acting at the center of buoyancy BO. W and BF are always equal and if these forces are collinear, the body will be in upright position as shown below.
 

005-floating-body-upright-position.gif

 

The body may tilt from many causes like wind or wave action causing the center of buoyancy to shift to a new position BO' as shown below.
 

005-floating-body-tilted-position-stable-and-unstable.gif

 

Point M is the intersection of the axis of the body and the line of action of the buoyant force, it is called metacenter. If M is above G, BF and W will produce a righting moment RM which causes the body to return to its neutral position, thus the body is stable. If M is below G, the body becomes unstable because of the overturning moment OM made by W and BF. If M coincides with G, the body is said to be just stable which simply means critical. The value of righting moment or overturning moment is given by
 

$RM \, \text{ or } \, OM = Wx = W \, (MG \sin \theta)$

 

The distance MG is called metacentric height.
 

Metacentric height, $MG = MB_O \pm GB_O$

 

Use (-) if G is above BO and (+) if G is below BO. Note that M is always above BO.
 

Value of MBO
Assume that the body is rectangular at the top view and measures B by L at the waterline when in upright position. The moment due to the shifting of the buoyant force is equal to the moment due to shifting of wedge.
 

005-floating-body-compute-for-mbo.gif

 

$BF \, z = Fs$

$\gamma V_D \, (MB_O \sin \theta) = (\gamma v)s$

$V_D MB_O \sin \theta = vs$

$MB_O = \dfrac{vs}{V_D \sin \theta}$

 

$MB_O = \dfrac{[ \, \frac{1}{2}(\frac{1}{2}B)(\frac{1}{2}B \tan \theta)L \,](\frac{2}{3}B)}{V_D \sin \theta}$

$MB_O = \dfrac{\frac{1}{12}LB^3 \tan \theta}{V_D \sin \theta}$
 

For small value of θ, tan θ ≡ sin θ and note that (1/12)LB3 = I, thus,

$MB_O = \dfrac{I \sin \theta}{V_D \sin \theta}$

$MB_O = \dfrac{I}{V_D}$

The formula above can be applied to any section.
 

Where
W = weight of the body
BF = buoyant force
M = metacenter
G = center of gravity of the body
BO = center of buoyancy in upright position
BO' = center of buoyancy in tilted position
MG = metacentric height or the distance from M to G
MBO = distance from M to BO
GO = distance from G to BO
v = volume of the wedge either immersion or emersion
s = horizontal distance between the center of gravity of the wedges
θ = angle of tilting
I = moment of inertia of the waterline section of the body
RM = righting moment
OM = overturning moment
 

For rectangular section

$MB_O = \dfrac{B^2}{12D}\left(1 + \dfrac{\tan^2 \theta}{2} \right)$

 

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