. Challenge to better agreement between theoretical computations and measurements in ship hydrodynamics. Ships; Water waves. These constants give hydrodynamic coefficients in the coupled equation of heaving and pitching as follows. (a+pV) z + b zo + c z - dip - e$ - gl^J = F (A+kZ pV) i> + BT|> + OJ» - D z - E z - G z - M yy & & & (186) where V is the displacement volume and k is the radius of gyration. On yy account of Haskind's relation, we have the relation D = d E = e (187) For numerical example, the hull form of Series 60, C = is employed because reliable data of mo
. Challenge to better agreement between theoretical computations and measurements in ship hydrodynamics. Ships; Water waves. These constants give hydrodynamic coefficients in the coupled equation of heaving and pitching as follows. (a+pV) z + b zo + c z - dip - e$ - gl^J = F (A+kZ pV) i> + BT|> + OJ» - D z - E z - G z - M yy & & & (186) where V is the displacement volume and k is the radius of gyration. On yy account of Haskind's relation, we have the relation D = d E = e (187) For numerical example, the hull form of Series 60, C = is employed because reliable data of model experiments have been available for comparison. A it â¢& & The coefficients a , b , d , e , and also a, b, A, B, d, and e are calculated. They are compared with results computed by means of the strip theory and the measured results, as shown in Figures 5 through 7. One can X 10 -2 PRESENT CALCULATION ORIGINAL SLENDER BODY THEORY STRIP THEORY O EXPERIMENT BY GERRITSMA AND BEUKELMAN. â Q X 10. Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Maruo, H. (Hajime), 1922-; David W. Taylor Naval Ship Research and Development Center; United States. Navy Dept. Bethesda, Md. : David W. Taylor Naval Ship Research and Development Center
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