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Forward Speed Calm Water Roll Decay for Surface Combatant 5415: Global and Local Flow Measurements

机译:地面战斗机5415的前进速度平静水滚动衰减:整体和局部流量测量

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Global and local flow measurements for forward speed calm water roll decay are performed in a towing tank for surface combatant model 5415 for both bare hull (BH) and bilge keel (BK) conditions. Roll motion is oscillatory with underdamped exponential decay and linear with respect to initial roll angles less than the average initial roll angle (9°). For larger mean roll angles (> 3°), damped natural frequency is a few percent below the hydrostatic natural roll frequency with larger values for BH than BK condition and increasing Froude number (Fr), whereas for smaller mean roll angles, it sharply increases toward the hydrostatic natural roll frequency. For larger mean roll angles, logarithmic decrement and linear damping linear increase with larger values for BK than BH condition and increasing Fr, whereas for smaller mean roll angles, they sharply increase. For increasing Fr, mean and initial roll angle averaged mean roll angle decreases by 50%; damped natural frequency increases by 6% with larger values for BH than BK condition; and logarithmic decrement/linear damping coefficient increase by a factor of three/four with larger values for BK than the BH condition. Logarithmic decrement and Himeno method linear damping coefficients are qualitatively similar. Nonlinear damping coefficient is two orders of magnitude smaller than linear damping coefficient. Roll reconstruction errors are smallest for Himeno with linear and nonlinear damping. The phase-averaged wave pattern and velocity and axial vorticity fields at x/L = 0.675 initially show larger amplitudes followed by oscillatory exponential decay. Alternating vortex pairs are shed from the bilge keel tip with damped magnitudes for decreasing mean roll angles. The local flow indicates lower frequencies and larger damping than the roll motion.
机译:对于裸船(BH)和舱底龙骨(BK)条件,在水面战斗员型号5415的拖船上进行向前和向后静水滚动衰减的全局和局部流量测量。横摇运动是振荡性的,具有衰减不足的指数衰减,并且相对于小于平均初始横摇角(9°)的初始横摇角是线性的。对于较大的平均侧倾角(> 3°),阻尼固有频率比静液压侧倾频率低百分之几,而BH值大于BK条件,并且弗洛德数(Fr)增大,而对于较小的平均侧倾角,其急剧增大朝向静水自然侧倾频率。对于较大的平均横摆角,对数减量和线性阻尼线性随着BK的值大于BH条件和Fr的增加而线性增加,而对于较小的平均横摆角,则急剧增加。对于增加的Fr,平均和初始侧倾角平均平均侧倾角减小50%。 BH值比BK条件大时,阻尼固有频率增加6%;与BH值相比,BK值较大时,对数减量/线性阻尼系数将增加三/四倍。对数减量和Himeno方法的线性阻尼系数在质量上相似。非线性阻尼系数比线性阻尼系数小两个数量级。对于具有线性和非线性阻尼的Himeno,滚动重建误差最小。 x / L = 0.675时的相位平均波型,速度和轴向涡度场最初显示出较大的振幅,随后出现振荡指数衰减。从舱底龙骨尖端散发出交替的涡流对,其阻尼大小可减小平均侧倾角。本地流量表示比侧倾运动更低的频率和更大的阻尼。

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