Thursday, October 12, 2023

Stability of Ship



Stability of Ship.     Ship stability is an area of naval architecture and ship design that deals with how a ship behaves at sea, both in still water and in waves, whether intact or damaged

Stable            A ship is in a stable condition of stability if, when heeled by an external force in still water to a small angle of inclination, it returns to the upright when the force is removed.

Unstable       condition : a state of equilibrium of a body (as a pendulum standing directly upward from its point of support) such that when the body is slightly displaced it departs further from the original position — compare stable equilibrium.

 

Neutral equilibrium condition :              A ship is in a neutral condition of stability if, when heeled by an external force in still water to a small angle of inclination, it comes to rest at an indeterminate angle of heel within small angles of inclination.

 

 

Righting Lever :      The vessel's centre of gravity (G) has a distinct effect on the righting lever (GZ) and consequently the ability of a vessel to return to the upright position. The lower the centre of gravity (G), the bigger is the righting lever (GZ).

 

Righting Moment. :            A moment that tends to restore an airplane or a naval vessel to its previous attitude after any small rotational displacement called also restoring moment.

 

Metacenter -             (shipbuilding) the point of intersection between two vertical lines, one line through the center of buoyancy of the hull of a ship in equilibrium and the other line through the center of buoyancy of the hull when the ship is inclined to one side; the distance of this intersection above the center of gravity is an indication of the stability of the ship.


 

Metacentric Height (GM):  Is a measurement of the initial static stability of a floating body. It is calculated as the distance between the centre of gravity of a ship and its metacentre. A larger metacentric height implies greater initial stability against overturning.

Centre Of Gravity (Cg):      The centre of gravity of an object is the point at which the whole weight of the object may be regarded as acting . if the object is suspended from this point , then it will remain balanced and will not tilt

 


 

Curve of stability:

 

STABILITY AT LARGE ANGLES OF HEEL

 

When a ship heels to an angle greater than about 10°, the principles on which the initial stability were based are no longer true. The proof of the formula for BM was based on the assumption that the two water planes intersect at the centerline and that the wedges are right angled triangles. Neither of these assumptions may be made for large angles of h«l and the stability of the ship must be determined from nest principles.

The righting lever is the perpendicular distance from a vertical axis through the centre of gravity G to the centre of buoyancy Bt . This distance may be found by dividing the moment of buoyancy about this axis by the buoyancy. In practice recourse is made to an instrument known as an integrator which may be used to determine the area of any plane and the moment of the plane about a given axis. The method used is as follows.



 The position of the centre of gravity G must be assumed at some convenient position above the keel. since the actual position is not known. Sections through the ship are drawn at intervals along the ship's length. These sections are inclined toan angle of, say ISO, The integrator is set with its axis in the vertical through G. The outline of each section is traced by the integrator up to a given waterline and the displacement andrighting lever obtained. This is repealed for different waterlines and for angles of 30". 45 D, 60°. 75° and 90°. The GZ values attach angle are planed 00 a base of clisp1acement to form the cross OIfWS 01 Stability fOT the ship. The displacement, height of centre of parity and metacentric height of a vessel may be cakulated for any loaded condition. At this displacement tbe righting levers may be obtained at the respective angles for the assumed position of the cCDtre of Vanity. These values must be amended to suit the actual bight of the centre of ,gravity. Let G - assumed position of cenue of gravity  0 1 "" actual position of centre of gravity

 


 

The amended righting levers are plotted on a base of angle of heel to form tbe Curve of Statical Stability for the ship in this condition of loading. The initial slope of the curve lies along a line drawn from the origin to Complotted vertically at one radian (57.3·). The area under this curve to any given angle, multiplied by the gravitational weight of the ship, is the work done in heeling the ship to that angle and is known as the Dynamical Stability.



Intact stability

                         For a cargo vessel, the intact stability requirements are follows-

·         Initial GM or meta centric height should not be less then 0.15 m.

·         Righting lever GZ should be at least 0.2 m and angle of heel Ѳ ≥ 30̊.

·         Maximum righting lever should occur at heel >30̊ preferably but not less than 25̊.

·         The Area of the GZ curve should be at least:

a)      0.055 m radian up to Ѳ = 30̊

b)      0.090 m radian up to Ѳ = 40̊

c)     0.03 m radian between 30̊ and 40̊ or between 30̊ and angle of        down flooding.



 

 

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