Lifting and Ship Stability

Attach the mathcad file, please.

May be it is any help:

Center of gravity and center of ???

Hello again to all,

So firstly my sincerest apologies for being quite presumptuous and not taking the time to outline my understanding of the background. I will now try to do this.

Firstly, the topic is initial ship stability. It is called initial stability because for small angles of heel the righting moment for a ship is generated by the transverse height of the metacentre which is the pivoting point the ship pivots about for small angles of heel whereby the metacentre is assumed to be static and does not move. For large angles the metacentre moves up and down, but this is not relevant.

The basic theory is that:

The short story is that as a ship heels the centre of buoyancy will move as the under water shape changes and equilibrium occurs when the centre of buoyancy is beneath the centre of gravity. In this case the metacentre (subscript T for transverse metacentre), Centre of Gravity (G) and centre of Buoyancy (B) will be aligned.

There are two moments of interest which are the righting moment and the heeling moment.

The righting moment being the mass of the ship (usually denoted by greek symbol Delta) multiplied by GZ which is a theoretical righting lever given by the distance from the centre of gravity to the line between the metacentre and the centre of buoyancy (as the ship heels) which is seen in figure 8.1 above (except that the centre of buoyancy is not shown on the diagram but B would be would be below Z in line with Mt.

The heeling moment in this context being by a shit of mass transversely is the weight of the object shifted (w) multiplied by the distance of transverse shift (d) multiplied by cos (theta) where theta is the angle of heel of the ship.

Combining these together to give the equilibrium state of final heel it can be seen that the final heel angle can be obtained as tan (theta) = wd/Delta GMt where GMt is the distance from the centre of gravity to the transverse metacentre.

Now,

Regarding this specific problem, I am of the understanding that the above equation for movement of objects has been adapted noting that the centre of gravity of the weight to be shifted transversely i.e. by the action of the crane swinging a weight outboard acts through the crane's jib irrespective of the length of the crane wire suspending the weight.

Therefore the adapted formula is:

tan (theta) = w x H / Delta GMt'

Where theta is the final angle of heel, w is the weight of the cargo, H in this context is the transverse movement of the crane's jib as this is where the weight of the suspended cargo acts, Delta is the total weight of the ship and GMt' is the 'new' distance between the transverse metacentre and the new centre of gravity. the new centre of gravity having risen due to the lifting of the weight.

I have drawn some crude hand sketches to further explain my understanding.

Looking at my sketches one by one:

The first is a schematic of my understanding of the problem where the shift in the cargo's centre of gravity instantaneously shifts from its actual position at G1 to G2 when it is lifted i.e. it acts from its position to the suspension point instantly on lift.

Then an idea of how the ship's overall position of centre of gravity shift upward when the cargo is lifted and this effectively reduces GMt to GMt'

Then an overhead view of the ship and how the crane swings, and finally my understanding of how to calculate the H distance i.e. the transverse shift of the crane's jib i.e. the distance the weight of the cargo moves transversely.

Hopefully I have done my bit in further explaining the background and happy to go into more detail as needed. I will say that now I have gone through this the more I think I might be right.

Andy.

Andy,

can you give me the complete length of the ship (approximately length)?

Volker