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Experimental investigations on turbulence structure over rough walls and grazing behavior of calanoid copepods.

机译:粗糙壁湍流结构和and足类足动物掠食行为的实验研究。

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摘要

This thesis consists of two parts. In part I, turbulence statistics and flow structure are studied in a fully-developed rough-wall channel flow Retau in the 3520--5360 range. A facility with optically index-matched fluid enables applying Particle Image Velocimetry (PIV) very near a rough surface composed of closely-packed pyramidal elements with height k=0.46 mm and wavelength lambda=3.2 mm. The flow and roughness settings achieve "well-characterized" (Jimenez 2004) flow conditions with h/k≈50 (h is half channel height) and k+=60∼100, which is suitable for investigating wall-similarity hypothesis. By performing planar and time-resolved PIV measurements of streamwise-wall-normal (x-y)and streamwise-spanwise ( x-z) planes at multiple resolutions, we examine the turbulence statistics and dynamics of flow structure from within the roughness to the channel centerline. The results show that the spatial variations in mean flow, Reynolds stresses, as well as turbulent kinetic energy (TKE) production and dissipation rates are confined to 2k above the surface, the region referred to as the roughness sublayer in the present context. Moreover, all the spatially-averaged Reynolds stress components have local maxima at slightly higher elevations, but the streamwise-normal component increases rapidly within 1k away from the wall, peaking at the top of the pyramids. Similarly, the TKE production and dissipation rates also peak near the wall, and their ratio has a maximum below 1k above the roughness but decreases to below one in the outer layer. Wall-normal turbulence transport is significant only close to the roughness. The spatial turbulent energy and shear spectra show an increasing contribution of large-scale motions, and diminishing role of small scale ones with increasing distance from the wall. However, as the spectra steepen at low wavenumbers, they flatten and develop bumps in wavenumbers corresponding to 1-3k. In compensated spectra, these bumps appear as additional maxima at scales corresponding to 15--30 times the Kolmogorov scales, i.e. within the dissipation range. Following this observation, we decompose the turbulence to large (>lambda), intermediate (3--6k), roughness (1--3k) and small (k) scales, where k and lambda are roughness height and wavelength, respectively. With decreasing distance from the wall, there is a remarkable increase in the 'non-local' SGS energy flux directly from large to small scale, and the fraction of turbulence dissipated by roughness scale eddies.;In part II, the grazing behaviors of calanoid copepod Acartia tonsa are investigated. Our objective is to quantify the response of marine copepods to varying diets, in particular when they are exposed to toxic dinoflagellates involved with harmful algal blooms (HABs). The conjectured role of toxins as a grazing deterrent is investigated by implementing digital holographic cinematography to compare the behavior of free-swimming Acartia tonsa on the nutritional diet of Storeatula major to that occurring during exposure to toxic and non-toxic strains of Karenia brevis and Karlodinium veneficum. Statistical analysis of the duration of the copepod's feeding appendage beating enables us to distinguish between two beating modes with lognormal distributions: "sampling beating" that has short durations (100 ms) and involves little fluid entrainment, and "grazing beating" that persists for longer periods (up to 1200 ms) and generates feeding currents. Without prey, A. tonsa only samples the water at low frequency, and upon introduction of desired food, it increases its sampling time moderately and the grazing substantially. On mono algal diets of either toxic dinoflagellate, the sampling frequencies are high, but the grazing remains low, and the copepod demonstrates aversion to both. In mixtures of S. major and toxic K. brevis, the sampling and grazing diminish rapidly, presumably due to neurological effects of consuming brevetoxins during while trying to feed on S. major. In contrast, on mixtures of toxic K. veneficum, both modes persist, indicating that intake of karlotoxins does not inhibit the copepod's grazing ability. Possible reasons for the lognormal distributions of duration, and the ecological impact of the different responses to toxins are discussed. (Abstract shortened by UMI.)
机译:本文分为两部分。在第一部分中,在3520--5360范围内充分发展的粗糙壁通道Retau中研究了湍流统计和流结构。具有光学折射率匹配流体的设备可以在非常紧密的粗糙表面上应用粒子图像测速(PIV),该粗糙表面由高度k = 0.46 mm和波长λ= 3.2 mm的紧密堆积的锥体元素组成。流动和粗糙度设置以h / k≈ 50(h为半通道高度)和k + = 60〜100达到“特征明确”(Jimenez 2004)的流动条件,适用于研究壁相似性假设。通过以多种分辨率对流向壁法线(x-y)和流向跨度(x-z)平面进行平面和时间分辨的PIV测量,我们研究了从粗糙度到通道中心线的湍流统计和流动结构动力学。结果表明,平均流量,雷诺应力以及湍动能(TKE)产生和耗散率的空间变化被限制在表面以上2k处,该区域在本文中称为“粗糙度子层”。此外,所有空间平均的雷诺应力分量在稍高的高度处都具有局部最大值,但流法线分量在距墙1k内迅速增加,并在金字塔的顶部达到峰值。类似地,TKE的产生和耗散率也在壁附近达到峰值,并且它们的比率在粗糙度以上1k以下具有最大值,但在外层中则降至1以下。壁面法向湍流传输仅在粗糙度附近才有意义。空间湍流能和切变谱显示出大尺度运动的贡献增加,而小尺度运动的作用随着与壁的距离增加而减小。但是,随着光谱在低波数处变陡,它们变平并在对应于1-3k的波数中产生凸起。在补偿光谱中,这些凸点在对应于Kolmogorov刻度的15--30倍的刻度处(即在耗散范围内)显示为附加最大值。根据此观察结果,我们将湍流分解为大尺度(> lambda),中间尺度(3--6k),粗糙度尺度(1--3k)和较小尺度(

著录项

  • 作者

    Hong, Jiarong.;

  • 作者单位

    The Johns Hopkins University.;

  • 授予单位 The Johns Hopkins University.;
  • 学科 Biology Ecology.;Engineering Mechanical.;Applied Mechanics.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 162 p.
  • 总页数 162
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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