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竖琴海豹和环斑海豹游泳的运动学及估计推力产生

Kinematics and estimated thrust production of swimming harp and ringed seals.

作者信息

Fish F E, Innes S, Ronald K

机构信息

Department of Biology, West Chester University, PA 19383.

出版信息

J Exp Biol. 1988 Jul;137:157-73. doi: 10.1242/jeb.137.1.157.

Abstract

The propulsive motions of swimming harp seals (Phoca groenlandica Erxleben) and ringed seals (Phoca hispida Schreber) were studied by filming individuals in a flume. The seals swam at velocities ranging from 0.6 to 1.42 m s-1. Locomotion was accomplished with alternate lateral sweeps of the hind flippers generated by lateral flexions of the axial body in conjunction with flexion of the flippers. The frequency of the propulsive cycle increased linearly with the swimming velocity, and the maximum angle of attack of the flipper decreased, but the amplitude remained constant. The kinematics and morphology of this hind flipper motion indicated that phocid seals do not swim in the carangiform mode as categorized by Lighthill (1969), but in a distinct mode that mimics swimming by thunniform propulsors. The hind flippers acted as hydrofoils, and the efficiency, thrust power and coefficient of thrust were calculated from unsteady wing theory. The propulsive efficiency was high at approximately 0.85. The thrust power increased curvilinearly with velocity. The drag coefficient ranged from 0.012 to 0.028 and was found to be 2.8-7.0 times higher than the theoretical minimum. The drag coefficient was high compared with that of phocid seals examined during gliding or towing experiments, indicating an increased drag encumbered by actively swimming seals. It was determined that phocid seals are capable of generating sufficient power for swimming with turbulent boundary layer conditions.

摘要

通过在水槽中拍摄个体,研究了竖琴海豹(Phoca groenlandica Erxleben)和环斑海豹(Phoca hispida Schreber)的游泳推进运动。海豹的游速范围为0.6至1.42米/秒。其运动是通过轴向身体的侧向弯曲与鳍状肢的弯曲相结合,使后鳍状肢交替进行侧向摆动来完成的。推进周期的频率随游泳速度线性增加,鳍状肢的最大攻角减小,但幅度保持不变。这种后鳍状肢运动的运动学和形态学表明,海豹科海豹并非如Lighthill(1969年)所分类的那样以鲹科模式游泳,而是以一种独特的模式游泳,类似于金枪鱼形推进器的游泳方式。后鳍状肢起到水翼的作用,并根据非定常机翼理论计算了效率、推力功率和推力系数。推进效率较高,约为0.85。推力功率随速度呈曲线增加。阻力系数在0.012至0.028之间,发现比理论最小值高2.8至7.0倍。与在滑行或拖曳实验中检查的海豹科海豹相比,该阻力系数较高,表明主动游泳的海豹承受的阻力增加。研究确定,海豹科海豹能够在湍流边界层条件下产生足够的游泳动力。

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