电动车上的东阳“特使”

透过昏黄的夕阳余晖,看着周围一辆辆快速驶过的汽车。翟继红的眼中始终是那么的安然与宁静。手推着自己的爱车,一步步耐心地向前走着……这是某天下午的一幅画面,而像这样的画面几乎每天都会在这个地方重新上演一遍。而这,起源于她的那辆电动车。2008年,满怀憧憬的翟继红毅然离开老家,选择北上,在大都市里寻找心中那美好的     

荷兰SKALAR流动分析仪在线测定水中总磷的比对研究

磷是水质评价的重要指标,磷在水中的逐渐富集,将引起藻类物质的大量滋长,使水质富营养化。水质的富营养化将消耗水中的溶解氧,损害鱼类等水生动物的生长,降低水的透明度,降低水资源在饮用、景观和养殖等方面的利用价值。天然水和废水中的磷是以各种磷酸盐的形式存在,     

临界区雷诺数下翼型流场电磁力控制的脱体涡模拟

利用Maxwell方程直接数值计算表面包覆电极与磁极翼型产生的三维Lorentz力分布,将其加入到流体控制方程的动量方程中,采用脱体涡模拟方法对临界区雷诺数下受Lorentz力作用下翼型绕流场进行数值模拟,研究分析了电磁力作用系数和攻角对翼型绕流场结构及其升阻力系数的影响机理和规律。结果表明,Lorentz力可以有效地改善翼型周围的流场结构,达到减阻、增升、消涡以及延缓和抑制其失速的目的,因此是翼型的一种有效流动控制手段。     

淮河流域行洪区洪水风险管理指标体系研究

新时期行洪区的洪水风险管理面临着人口、资源、环境等问题,传统洪水管理模式已经不能满足其要求。采取主客观结合的方法,通过识别行洪区潜在风险,从行洪危险性和受体脆弱性两方面筛选评价指标。以15个淮河干流行洪区为例,使用熵值法确定指标权重,构建了淮河行洪区洪水风险管理指标体系,对行洪区洪水风险管理进行了系统分析。结果表明：新时期淮河流域行洪区的洪水风险管理的重点是提高行洪区承灾能力,降低经济脆弱性和社会脆弱性。     

TRANSPORT OF BICOMPONENT CONTAMINANT IN FREE-SURFACE WETLAND FLOW

This paper presents a theoretical analysis of a pulsed bicomponent contaminant emission into a free-surface wetland flow.The basic equations are for the bicomponent contaminant transport in the wetland flow under the combined action of advection,mass dispersion,and ecological reaction at the phase averaged scale.The effect of the ecological reaction is separated from the hydro-dynamic effect via a set of widely used transforms.The analytical solution for the evolution of the depth-averaged concentration is rigorously derived,with a limiting case covering the known solution for the single component contaminant transport.It is found that the depth-averaged species concentration of the bicomponent contaminant can approach an equilibrium state determined by the distri-bution coefficient.     

梯级电站建设对水质的影响

采用一维水动力数学模型和水质数学模型,对梯级电站建设前后的CJ江干、支流的水质变化进行研究,预测CJ江2020年5个梯级电站建设后干流水质主要参数的变化情况。结果表明,各梯级电站水库蓄水后各坝址处平均DO质量浓度将较建库前略有下降,BOD5和NH3-N的质量浓度呈下降趋势,TP质量浓度变化较小。     

同心环管圆孔射流流动特性的数值模拟

采用标准的k-ε模型及混合有限分析法对均匀横流条件下三维受限同心环管中单孔和双孔的横向紊动射流流动进行数值模拟.分别得到单圆孔不同流速比下的射流轨迹线与数学表达式、双圆孔不同间距下的速度场.结果显示：射流比越大,射流深度越深,射流越不容易发生弯曲;射流横断面上速度最大值的偏离程度随横流距离的增加而增大,但增大率越来越小;双孔射流孔间距影响射流轨迹线,由于前一个射流的遮挡作用,后面射流更不容易发生弯曲.     

Hot compressive deformation behavior and constitutive relationship of Al-Zn-Mg-Zr alloy with trace amounts of Sc

Abstract： The hot deformation behaviors of AI-Zn-Mg-Sc-Zr alloy were investigated in a temperature range of 340-500℃ and a strain rate range of 0.001-10 s 1 using uniaxial compression test on Gleeble-1500 thermal simulation machine. The results show that the flow stress increases with increasing strain and tends to be constant after a peak value. The flow stress increases with increasing strain rate and decreases with increasing deformation temperature. The phenomenon of dynamic recovery and dynamic recrystallization can be observed by microstructural evolutions. Based on the hyperbolic Arrhenius-type equation, the true stress-true strain data from the tests were employed to establish the constitutive equation considering the effect of the true strain on material constants （α, β, Q, n and A）, which reveals the dependence of the flow stress on strain, strain rate and deformation temperature. The predicted stress-strain curves are in good agreement with experimental results, which confirms that the developed constitutive equations are suitable to research the hot deformation behaviors of Al-Zn-Mg-Sc-Zr alloy.     

Fluid flow characteristics of single inclined circular jet impingement for ultra-fast cooling

The fluid flow characteristics of the single bunch inclined jet impingement were investigated with different jet flow velocities, nozzle diameters, jet angles and jet-to-target distances for ultra-fast cooling technology. The results show that the peak pressure varying significantly from nearly 0.5 to above 13.4 kPa locates at the stagnation point with different jet diameters, and the radius of impact pressure affected zone is small promoted from 46 to 81 mm in transverse direction, and 50 to 91 mm in longitude direction when the jet flow velocity changes from 5 to 20 m/s. However, the fluid flow velocity is relatively smaller near the stagnation point, and increases gradually along the radius outwards, then declines. There is an obvious anisotropic characteristic that the flow velocity component along the jet direction is about twice of the contrary one where the jet anlge is 60°, jet diameter is 5 mm, jet length is 8 mm and jet height is 50 mm.