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A manual of naval architecture for the use of officers of the Royal Navy, officers of the Mercantile Marine, yachtsmen, shipowners, and shipbuilders (1894)

White, W. H. (William Henry), Sir, 1845-1913 · London : J. Murray · leaf 152

An illustration from A manual of naval architecture for the use of officers of the Royal Navy, officers of the Mercantile Marine, yachtsmen, shipowners, and shipbuilders, 1894, leaf 152
al position, BD to the newone, B, the line BXB being parallel to gxg2, and the length— BBx = 1 x g,g* It thus becomes obvious that, when the positions of the centresof gravity of the wedges (g± and g2) for any inclination are known,the new position of the centre of buoyancy (B) can be… … 60° SO /OO ISO Angles of mclination. ieo° dicular to WL, then, by the same principle as is used above, thelength BXB = — x hJh- Also, if the angle of inclination WSWi be called a— GZ = BjE - BXG sin a, and consequently— ., Moment of statical stability = V X GZ = V(BXE - B& sin a) = v x hjt2 - V…

Naval architecture

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