粒子通量和运动流体:萨尔加索海同步捕集的经验

G Gust , R.H Byrne , R.E Bernstein , P.R Betzer , W Bowles
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引用次数: 96

摘要

使用配备传感器的沉积物捕集器进行的一系列24小时同步实验表明,较高的颗粒收集率与较高的接近速度有关。对于成对的400米部署和成对的1500米部署,具有可变阻力配置的水面系留式陷阱在接近速度上存在明显差异。位于沉积物捕集器内外的小型热膜流体动力学传感器检测到捕集器内的流动细胞,其速度在外部流体接近速度的50%和100%之间。结合实验室水槽模拟,这些观测结果表明,颗粒不会在重力作用下通过捕集器孔隙沉降。总之,粒子被平流扫入阱孔下游部分的阱中,然后大多数粒子在阱孔上游部分被排出。在漂移陷阱内检测到的流体流动范围从1.2到31厘米s−1,l可能会淹没所有与这些采样潜水器相互作用的最强“游泳者”。在我们的两个采样层(400米和1500米),系绳运动产生了周期约为10秒、振幅约为0.5米的陷阱深度振荡。在模拟沉积物陷阱收集实验的水槽中,尚未考虑到这种影响。
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Particles fluxes and moving fluids: experience from synchronous trap collection in the Sargassso sea

A series of synchronous, 24-h experiments using sensor-equipped sediment traps revealed that higher particle collection rates were associated with higher approach velocieties. Surface-tethered traps with variable drag configurations provided distinct differences in approach velocities for paired 400 m deployments and paired 1500 m deployments. Small-scale hot-film hydrodynamics sensors located both inside and outside the sediment traps detected flow cells within the traps with velocities between 50 and 100% of the external fluid approach velocities. In conjunction with laboratory flume simulations, these observations reveal that particles do not settle gravitationally across trap apertures. Intead, particles are swept advectively into traps at the downstream portion of trap apertures, and most are then expelled at the upstream portions of trap apertures. Fluid flows detected inside the drifting traps, which ranged from 1.2 to 31 cm s−1,l probably overwhelm all but the strongest “swimmers” that interact with these sampling divices. At our two sampling horizons (400 and 1500 m), tether-line motions generated trap depth oscillations with a period of the order of 10 s and an amplitude of about 0.5 m. Such effects have not been accounted for in flume simulated of sediment traps collection experiments.

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