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Basics of Fluid Mechanics, 2014a

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4.6. BUOYANCY AND STABILITY 135<br />

A new point can be defined as G c . This point is the intersection <strong>of</strong> the center line with<br />

the vertical line from G ′ .<br />

GG c = GG′<br />

sin β<br />

(4.169)<br />

The distance that was used before GM is replaced by the criterion for stability by G c M<br />

and is expressed as<br />

G c M = gρ A I xxA<br />

ρ s V body<br />

− BG − 1<br />

m total<br />

I xxb<br />

V b<br />

(4.170)<br />

If there are more than one tank partially filled with liquid, the general formula is<br />

G c M = gρ A I xxA<br />

ρ s V body<br />

− BG − 1<br />

m total<br />

n ∑<br />

i=1<br />

I xxbi<br />

V bi<br />

(4.171)<br />

One way to reduce the effect <strong>of</strong><br />

the moving mass center due to liquid<br />

is done by substituting a single<br />

tank with several tanks. The moment<br />

<strong>of</strong> inertial <strong>of</strong> the combine two<br />

h<br />

T d<br />

tanks is smaller than the moment <strong>of</strong><br />

G<br />

inertial <strong>of</strong> a single tank. Increasing<br />

the number <strong>of</strong> tanks reduces the moment<br />

<strong>of</strong> inertia. The engineer could<br />

design the tanks in such a way that Fig. -4.45. Measurement <strong>of</strong> GM <strong>of</strong> floating body.<br />

the moment <strong>of</strong> inertia is operationally<br />

changed. This control <strong>of</strong> the stability, GM, can be achieved by having some tanks<br />

spanning across the entire body with tanks spanning on parts <strong>of</strong> the body. Movement<br />

<strong>of</strong> the liquid (mostly the fuel and water) provides way to control the stability, GM, <strong>of</strong><br />

the ship.<br />

4.6.1.2 Metacentric Height, GM, Measurement<br />

The metacentric height can be measured by finding the change in the angle when a<br />

weight is moved on the floating body.<br />

Moving the weight, T a distance, d then the moment created is<br />

This moment is balanced by<br />

M weight = Td (4.172)<br />

M righting = W total GM new θ (4.173)<br />

Where, W total , is the total weight <strong>of</strong> the floating body including measuring weight.<br />

The angle, θ, is measured as the difference in the orientation <strong>of</strong> the floating body. The

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