127_add_Added Masses of Ship Structures.pdf - 116 4 Added Masses of Interacting Bodies Fig 4.7 Coefficient of added mass of a parallelepiped moving

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116 4 Added Masses of Interacting Bodies Fig. 4.7 Coefficient of added mass of a parallelepiped moving between two walls Fig. 4.8 Coefficients of added masses of a cylinder of revolution moving near a flat solid wall

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4.2 Added Masses of Bodies Moving Close to a Solid Boundary 117 Fig. 4.9 Coefficients of added masses of a cylinder of revolution moving near a flat solid wall 4.2.7 Three-Axial Ellipsoid Moving Near a Flat Wall In first approximation the added masses of a three-axial ellipsoid moving near a flat hard wall can be computed via a method proposed by Bloch and Ginevsky [30]. Let us briefly outline this method for the case of motion of two bodies in an ideal fluid which does not move at infinity. The potential of velocities Φ of the fluid motion can be represented in the form Φ = Φ 1 + Φ 2 , where Φ 1 is the potential of velocities corresponding to the motion of the first body in the presence of the second body, which stays at rest; Φ 2 is the potential of ve-

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