{"title":"Initiation of Sediment Resuspension by Combined Wave-Current Conditions in an Artificial Seagrass Meadow","authors":"Chuyan Zhao, Heidi Nepf","doi":"10.1029/2024JF008050","DOIUrl":null,"url":null,"abstract":"<p>Laboratory experiments examined the impact of current on ripple formation and the onset of wave-driven resuspension within an artificial seagrass meadow modeled after <i>Zostera marina.</i> Within the meadow, the current was less than or equal to the wave velocity. Meadows were constructed with three shoot densities: 247, 455 and 962 stems/m<sup>2</sup>, and each shoot had six flexible blades. The sediment bed, consisting of <span></span><math>\n <semantics>\n <mrow>\n <mn>65</mn>\n <mspace></mspace>\n <mi>μ</mi>\n <mi>m</mi>\n </mrow>\n <annotation> $65\\,{\\upmu }\\mathrm{m}$</annotation>\n </semantics></math> spherical grains, was initially 1.4 cm thick, allowing ripple and scour hole formation. The formation of wave-orbital ripples was dependent on meadow density and current magnitude. Over bare beds and sparse meadows, ripples were present and not impacted by the addition of current, such that the wave velocity resuspension threshold with current was the same as that in pure wave conditions. In medium-density meadows, the addition of current reduced ripple height due to plant-generated turbulence. As current increased, ripple size and ripple-generated turbulence decreased, requiring a higher wave velocity to resuspend sediment. That is, for medium density meadows, the critical wave velocity increased as the current velocity increased. Finally, in dense meadows, no ripples formed and resuspension was driven by a critical value of plant-induced turbulence, which was proportional to the total velocity (current plus wave velocity), such that as the current velocity increased, the critical wave velocity decreased. A model predicting the critical wave velocity for the dense meadow was derived based on the assumption that resuspension was driven by a critical level of stem-generated turbulence.</p>","PeriodicalId":15887,"journal":{"name":"Journal of Geophysical Research: Earth Surface","volume":"130 6","pages":""},"PeriodicalIF":3.8000,"publicationDate":"2025-06-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1029/2024JF008050","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Geophysical Research: Earth Surface","FirstCategoryId":"89","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1029/2024JF008050","RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"GEOSCIENCES, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Laboratory experiments examined the impact of current on ripple formation and the onset of wave-driven resuspension within an artificial seagrass meadow modeled after Zostera marina. Within the meadow, the current was less than or equal to the wave velocity. Meadows were constructed with three shoot densities: 247, 455 and 962 stems/m2, and each shoot had six flexible blades. The sediment bed, consisting of spherical grains, was initially 1.4 cm thick, allowing ripple and scour hole formation. The formation of wave-orbital ripples was dependent on meadow density and current magnitude. Over bare beds and sparse meadows, ripples were present and not impacted by the addition of current, such that the wave velocity resuspension threshold with current was the same as that in pure wave conditions. In medium-density meadows, the addition of current reduced ripple height due to plant-generated turbulence. As current increased, ripple size and ripple-generated turbulence decreased, requiring a higher wave velocity to resuspend sediment. That is, for medium density meadows, the critical wave velocity increased as the current velocity increased. Finally, in dense meadows, no ripples formed and resuspension was driven by a critical value of plant-induced turbulence, which was proportional to the total velocity (current plus wave velocity), such that as the current velocity increased, the critical wave velocity decreased. A model predicting the critical wave velocity for the dense meadow was derived based on the assumption that resuspension was driven by a critical level of stem-generated turbulence.
在模拟Zostera码头的人工海草草甸中,实验室实验研究了水流对波纹形成和波浪驱动再悬浮的影响。在草甸内,水流小于或等于波速。草甸的枝密度分别为247、455和962茎/m2,每枝有6片柔性叶片。沉积层由65 μ m $65\,{\upmu}\mathrm{m}$球形颗粒组成,初始厚度为1.4 cm,可形成波纹和冲刷孔。波轨纹的形成与草甸密度和电流大小有关。在光秃秃的河床和稀疏的草甸上,波纹存在,不受水流的影响,因此有水流的波速再悬浮阈值与纯波条件下相同。在中等密度的草甸中,由于植物产生的湍流,电流的增加降低了纹波高度。随着水流的增加,波纹大小和波纹产生的湍流减小,需要更高的波速来重新悬浮沉积物。即对于中密度草甸,临界波速随流速的增大而增大。最后,在茂密的草甸中,没有形成波纹,再悬浮是由植物诱导湍流的临界值驱动的,该临界值与总流速(电流+波速)成正比,随着流速的增加,临界波速降低。在假设再悬浮是由一个临界水平的茎生湍流驱动的基础上,推导了一个预测稠密草甸临界波速的模型。