转子流道倾斜式的外驱旋转压能交换器性能研究

为提高外驱式旋转压能交换器性能，设计了转子流道倾斜式的外驱式旋转压能交换器，以能量回收效率和体积混合率为性能指标，利用商业CFD软件Fluent对模型求解计算，并与直流道外驱式旋转压能交换器模拟数据对比分析。结果表明，处理量相等的情况下，能量回收效率和体积混合率均随转子转速的升高而降低；同一转速下，转子倾斜角度改变，能量回收效率变化不超过0.04%，而对体积混合率有明显影响。研究结果对于提高外驱式旋转压能交换器设备性能具有一定指导意义。     

转子流道倾斜式的外驱旋转压能交换器性能研究

为提高外驱式旋转压能交换器性能，设计了转子流道倾斜式的外驱式旋转压能交换器，以能量回收效率和体积混合率为性能指标，利用商业CFD软件Fluent对模型求解计算，并与直流道外驱式旋转压能交换器模拟数据对比分析。结果表明，处理量相等的情况下，能量回收效率和体积混合率均随转子转速的升高而降低；同一转速下，转子倾斜角度改变，能量回收效率变化不超过0.04%，而对体积混合率有明显影响。研究结果对于提高外驱式旋转压能交换器设备性能具有一定指导意义。     

涡节型、酒窝型强化管管内沸腾传热特性实验

以微型Capstone C30燃气轮机排放的烟气余热为热源,研究涡节结构强化管、酒窝结构强化管和光管管内沸腾换热特性。实验结果表明：涡节型结构强化传热管管内沸腾换热系数约为光管的1.6~2.1倍,管外对流传热系数约为光管的1.3~1.5倍,总传热系数约为光管的1.4~1.5倍;酒窝型强化传热管管内沸腾换热系数约为光管的2.1~2.5倍,管外对流传热系数约为光管的1.8~2.0倍,总传热系数约为光管的1.9~2.1倍。分析了涡节型强化传热管和酒窝型强化传热管较光管传热性能好的原因。     

管子管板检测机器人爬行脚的吊装负载能力研究

在爬行机器人携带无损检测（NDT）设备的情况下,为了保证其对立式换热器管子管板角焊缝检测过程的稳定性和可靠性,重点对立式换热器管子管板检测机器人的关键机构——爬行脚的负载能力进行了数值模拟分析和实验研究,应用Hypermesh和ANSYS Workbench联合仿真平台对爬行脚在充气和自锁工况下的结构强度和接触状态进行了仿真。模拟结果表明,在负载逐渐增加的过程中,两种工况下爬行脚与换热管内壁之间没有发生滑移失效,一直保持了良好的稳定性和可靠性。同时对爬行脚实验样机进行了开发和验证,并通过两种工况下的吊装负载实验,得到充气工况最大负载为38 kg,自锁工况最大负载为15 kg,验证了其良好的稳定性。     

制糖离子交换模糊控制系统的设计与仿真

针对传统制糖离子交换工艺系统的不足,利用爱默生PLC设计了离子交换流量模糊控制系统。提出把模糊控制理论和PID控制理论相结合的方法,设计实现模糊-PID复合控制系统。通过Matlab仿真可看到将模糊控制算法与PID控制原理相结合相互补偿的方法与常规PID控制方法相比,模糊控制PID系统具有控制精度高,可靠性好,适应性好的优点。     

同时测定肉制品中氯化物、亚硝酸盐、硝酸盐

本文应用离子色谱仪,兔肉脯为基质,建立了同时测定肉及肉制品中氯化物、亚硝酸盐和硝酸盐的分析方法.样品绞碎后纯水起声提取,提取液过c18柱除去有机杂质,经0.45μm过滤器直接进行测定.方法操作简单,重现性好,各组分加标回收率为：C1,103.0％; NO2-N,98.0％;NO,-N,94.2％.RSD在0.4％～1.3％（n=6）.方法检出限分别为：C1,0.01 mg/L; NO2-N,0.005 mg/L; NO3-N,0.02 mg/L.     

一种带中间换热器的双热源高温热泵系统

为了提高工业高温热泵系统的热力性能,实现对工业低温余热的高效综合回收,提出了一种带中间换热器的双热源高温热泵系统。第一级热泵以CO2为工质、以空气为热源,在超临界状态下将冷水加热到中间温度。第二级热泵以R152a(二氟乙烷)作为工质,从工业余热源吸收热量,将用水加热到所需的高温,并且在中间换热器中将CO2加热到过热状态。对该双热源热泵系统进行热力学分析,发现给定R152a在中间换热器温降的情况下,CO2存在最大的过热度,使得整个系统达到最佳运行工况。以回收50℃废水余热为例与单热源热泵进行比较,平均供水量是后者的两倍多,单位质量热水的耗功量减少43.2%,性能系数和火用效率分别平均提高41.9%和23.96%。     

板式换热器内两相流流量分配的模拟及实验验证

针对带有分配器的钎焊板式换热器内各支路的气液流量分配特性建立了预测模型.基于各支路的压降平衡方程,分别建立了板间流道和分配器流道压降计算模型;基于分配器处的气液分离关系方程,分别建立了两相流体在分配器处相分离和在分配器入口处液膜分布的计算模型.通过将压降平衡方程、气液分离方程分开迭代计算,开发了适用于模型的求解算法.模拟结果与实验测试数据对比表明,换热器总压降的相对误差在±20%以内,两相区高度的相对误差在±13%以内.     

High-energy ion treatments of amorphous As40Se60 thin films for optical applic ations

The treatment of 100 MeV Ag swift-heavy ion(SHI) irradiation with five different fluences(3 1010, 1 1011, 3 1011, 1 1012, and3 1012ions/cm2) was used to design optical and structural properties of amorphous(a-) As40Se60 chalcogenide thin films. Swanepoel method was applied on transmission measurements to determine the changes in optical bandgap, Tauc parameter and linear optical parameters, i.e., linear optical absorption, extinction coefficient and linear refractive index. Dispersion of the material was determined by Wemple–DiDomenico relation.Changes in nonlinear optical parameters of third-order optical susceptibility and nonlinear refractive index were determined using semi-empirical relations. Changes in surface morphology of the films were investigated using SEM observation, which indicated that fluence 3 1012ions/cm2was upper threshold limit for these films for ion treatment. It is observed that optical bandgap reduces from 1.76 eV to 1.64 eV, and nonlinear refractive index increases from 1.31 10 10[esu] to 1.74 10 10[esu]. Linear refractive index initially increases from 2.80 to 3.52(for fluence3 1010ions/cm2) and then keeps decreasing. The observed changes in optical properties upon irradiation were explained in terms of structural rearrangements by Raman measurement. The study was compiled with the previous literature to propose SHI as an effective optical engineering technique to achieve desired changes according to the need of optical/photonic applications.     

Ion flux dropout observed near dipolarization front

An ion flux dropout near the dipolarization front （DF） at around XGSM =- 11 RE in the Earth＇ s plasma sheet was observed by Time History of Events and Macroscale Interaction during substorms （THEMIS） on March 31, 2009. The ion differential energy fluxes at energies from 450 eV to 150 keV measured by the ESA and SST instruments from THC began to decrease about 2 s before the detection of the DF and reached a local minimum 6 s later. Then, the ion fluxes gradually increased to form a dropout around the DF. The spatial extent of the dropout was about 4,000 km. For energies above 20 keV, the ion fluxes after the dropout are greater than those before it, contrary to the fluxes at energies below 20 keV. The associated ion density variation indicates that the ion flux dropout coincides with the ion density dropout. Taking advantage of multipoint observations, THD, THC, and THE detected the same DF consecutively. Only THC detected an obvious ion flux dropout; THD observed an indistinct one about 2 s before THC; no high-energy （E 〉 30 keV） ion flux dropout was observed by THE. Our study suggests that the ion flux dropout may evolve with the earthward-propagating DF, and its properties can depend on locations relative to the DF.