ForsideBøgerA Treatise On The Princip… Of Harbour Engineering

A Treatise On The Principles And Practice Of Harbour Engineering

Forfatter: Brysson Cunningham

År: 1908

Forlag: Charles Griffin & Company

Sted: London

Sider: 410

UDK: Vandbygningssamlingen 134.16

With18 Plates And 220 Illustrations In The Text

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Side af 416 Forrige Næste
PIERHEADS, QUAYS, AND LANDING-STAGES. 207 is cut off within the parabola, and bisect it at the point C. Draw CB2 parallel to the axis QK, intersecting the curve at the point B2. Then B2 is the centre of buoyancy for the water-line FS. From B2 draw B2M2 at right angles to FS so as to cut the axis QK in M2. M2 is the metacentre under the same conditions. The proof of the foregoing construction lies in the facts that the tan- gent at the extremity of a diameter of a parabola is parallel to the chords which are bisected by that diameter, and that the tangent to the curve of buoyancy at any point is parallel to the line of flotation corresponding to that point as centre of buoyancy. Thus far, we have only dealt with centres of buoyancy lying within the section HON ; that is for water-lines rauging between GN and HP. For water-lines between HP and NG, it is necessary to construct the parabola GZH. This being done (fig. 180), the curve of buoyancy is defined from ß to y, and the corresponding positions of the metacentre may be determined as already explained. They will lie, however, not on the axis QK, but on the axis RT, parallel to which the lines, from the water surface to the curve, must be drawn. It is interesting to consider the water-line HP. There are two parabolic chords appertaining to the position, viz., Hy and aP. The middle point of the former is a, and of the latter y. Both the line aß, drawn parallel to the axis RT of the parabola GZH, and the line yß, drawn parallel to the axis QK of the parabola GBjP, meet at the point ß, which is the limiting position of the centre of buoyancy for both parabolas. The line /3M8, perpendicular to HP, gives extreme positions for the metacentre on the respective axes: the upper limit M8 on QK, and the lower limit M4 on RT. In fig. 180, owing to the particular ratio of L to D, the point M8 coincides with the point Q. The curve of buoyancy for the remaining moiety of the pontoon is simply a replica, upon the other side of the diagonal HP, of the curve aßy. The parabolas GBjP and GZH have three point contact ; that is, the curves not only touch one another, but cross when continued.