首页> 外文期刊>Journal of Geophysical Research, C. Oceans: JGR >A turbulent convection model with an observational context for a deep-sea hydrothermal plume in a time-variable cross flow
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A turbulent convection model with an observational context for a deep-sea hydrothermal plume in a time-variable cross flow

机译:时变横流中具有观测环境的深海热液羽流的湍流对流模型

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[1] A turbulent convection model for a hydrothermal fluid discharging into a tidally modulated, stratified cross flow is used to investigate time-variable conditions in plumes, such as the one rising from Dante, a sulfide mound at ~2175 m depth on the Endeavour segment of the Juan de Fuca Ridge. That plume is the consequence of the coalescence of 10 or more small, individual plumes from chimneys discharging hot, salt-diminished fluid into the near-bottom ocean. At Dante, the discharge encounters ambient horizontal currents with speeds oscillating from near zero to a maximum of ~7 cm s~(-1), speeds which can bend a plume more than 45° from the vertical. Model results are compatible with field measurements of the plume footprint size and vertical velocity both 20 m above the source when earlier estimates for Dante's heat flux of ~50 MW drive the convection. The smallscale short period variability of velocities and properties distributions observed in the field is mimicked in model results. Plumes pool above a source during periods of weak cross flows but stream away from the source, with more diluted concentrations and lower rise heights, at other times. Plume distributions, at identical cross-flow speeds, differ whether the flow is accelerating or decelerating. Small changes in background hydrographic profiles create differences in rise heights comparable to those caused by large changes in source buoyancy flux. If put into an entrainment context, results suggest an entrainment coefficient (a_(EFF)) that varies from ~0.11 to ~0.025 with increasing height (2–76 m) above the source.
机译:[1]一种用于将热液流排入潮汐调制的分层错流的湍流对流模型,用于研究羽流中的时变条件,例如从但丁(奋进号上约2175 m深度的硫化物丘)升起的羽流。胡安德富卡山脊的一段。该羽流是烟囱中10个或更多的单个羽流聚结的结果,烟囱将热的,盐分减少了的流体排入了近乎底部的海洋。在但丁,放电遇到环境水平电流,其速度从接近零摆动到最大〜7 cm s〜(-1),该速度可能会使烟羽与垂直方向弯曲超过45°。当Dante约50 MW的热通量的早期估计推动了对流时,模型结果与在源上方20 m处的羽流足迹尺寸和垂直速度的现场测量结果兼容。模型结果模拟了在现场观测到的速度和特性分布的小规模短期变化。在较弱的横流期间,羽状流在源头上方汇聚,但在其他时间则从源头流出,稀释浓度更高且上升高度较低。无论流速是加速还是减速,在相同的横流速度下的羽流分布都不同。与水源浮力通量的大变化相比,背景水文剖面的小变化会产生上升高度的差异。如果放在夹带环境中,结果表明夹带系数(a_(EFF))随来源上方的高度增加(2-76 m)而在〜0.11至〜0.025之间变化。

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