河海大学学报(自然科学版)
河海大學學報(自然科學版)
하해대학학보(자연과학판)
JOURNAL OF HOHAI UNIVERSITY (NATURAL SCIENCES)
2014年
2期
130-136
,共7页
顾莉%袁航%华祖林%王兰兰%李秋兰%焦梓楠
顧莉%袁航%華祖林%王蘭蘭%李鞦蘭%焦梓楠
고리%원항%화조림%왕란란%리추란%초재남
分汊河道%温差剪切流%紊动强度%流速比%汊道宽度比
分汊河道%溫差剪切流%紊動彊度%流速比%汊道寬度比
분차하도%온차전절류%문동강도%류속비%차도관도비
braided river%thermally stratified shear flow%turbulent intensity%velocity ratio%width ratio of two anabranches
针对目前分汊河道分层流紊动特性研究的空白,通过物理模型试验探索分汊河道温差剪切分层流在不同上下层速度比与汊道宽度比影响下的紊动强度变化规律。结果表明:随着上下层流速比由大变小,汊道分层流发生从分层到混合的转捩。在混合流条件下,支汊沿程断面高紊动区由C形分布转变为倒C形分布,最终全断面紊动分布均匀;随着支汊宽度增大,高紊动区出现的断面位置呈现滞后性,且紊动能量值增大。其他分层流态条件下,强紊动能分布的范围和量值都有所变化。对于交汇口断面,对称汊道在断面中心处掺混剧烈,随着上下层流速比的增大,紊动能量值减小;不对称汊道出口断面紊动强烈区域向较窄的左支汊一侧移动,与岛屿尾尖位置密切相关。
針對目前分汊河道分層流紊動特性研究的空白,通過物理模型試驗探索分汊河道溫差剪切分層流在不同上下層速度比與汊道寬度比影響下的紊動彊度變化規律。結果錶明:隨著上下層流速比由大變小,汊道分層流髮生從分層到混閤的轉捩。在混閤流條件下,支汊沿程斷麵高紊動區由C形分佈轉變為倒C形分佈,最終全斷麵紊動分佈均勻;隨著支汊寬度增大,高紊動區齣現的斷麵位置呈現滯後性,且紊動能量值增大。其他分層流態條件下,彊紊動能分佈的範圍和量值都有所變化。對于交彙口斷麵,對稱汊道在斷麵中心處摻混劇烈,隨著上下層流速比的增大,紊動能量值減小;不對稱汊道齣口斷麵紊動彊烈區域嚮較窄的左支汊一側移動,與島嶼尾尖位置密切相關。
침대목전분차하도분층류문동특성연구적공백,통과물리모형시험탐색분차하도온차전절분층류재불동상하층속도비여차도관도비영향하적문동강도변화규률。결과표명:수착상하층류속비유대변소,차도분층류발생종분층도혼합적전렬。재혼합류조건하,지차연정단면고문동구유C형분포전변위도C형분포,최종전단면문동분포균균;수착지차관도증대,고문동구출현적단면위치정현체후성,차문동능량치증대。기타분층류태조건하,강문동능분포적범위화량치도유소변화。대우교회구단면,대칭차도재단면중심처참혼극렬,수착상하층류속비적증대,문동능량치감소;불대칭차도출구단면문동강렬구역향교착적좌지차일측이동,여도서미첨위치밀절상관。
At present, few studies have been conducted on turbulence characteristics of stratified flow in braided rivers. In this study, a physical model experiment was carried out to study the variation of the turbulent intensity of thermally stratified shear flow with different velocity ratios of two layers and width ratios of two anabranches. The results show that, as the velocity ratio decreased, the stratified flow in the braided river changed from stratified flow to neutrally stratified flow. As to the neutrally stratified flow, the sectional high-turbulence zone along the anabranches changed from a C-type distribution to an inverse C-type distribution, and the turbulent intensity was mixed well throughout the section in the end. With the increase of the channel width, the section of the high-turbulence zone appeared later, and the quantity of the turbulent intensity increased. Under other conditions of stratified flow, the range and quantity of high turbulent intensity all changed. At the confluence section, the flow in the center of the section was mixed violently in the symmetric braided river. With the increase of the velocity ratio, the quantity of the turbulent intensity decreased. The high turbulent intensity zone moved to the narrowed left anabranch in the non-symmetric braided river, which was associated with the tail position of the mid-bar.