CFETR稳态运行模式的0.5维集成模拟及其杂质粒子比例影响的分析

采用快速集成模拟软件METIS完成了CFETR1GW稳态反剪切运行模式的设计。该反剪切运行模式由40MW离轴电子回旋电流驱动(ECCD)与60MW的离轴中性束电流驱动(NBCD)所实现，获得了稳定的安全因子剖面，其在ρ=0.52处具有最小安全因子q_min=3.1，从而可避免危险的m/n=2/1、3/2、5/3的新经典撕裂模(NTM)。此外，本文还分析了Ar杂质粒子的含量对此稳态反剪切模式约束性能的影响。     

库特（Couette）剪切流准确解的一般形式

 从N-S方程出发,得到了轴对称异型断面管纯剪切流动速度分布的一般解,进而推出了纯剪切流动有限宽度矩形断面管的速度分布和流量计算公式,证明了库特剪切流是有限宽度矩形断面管当宽度趋向无穷大时的一种特例。并对库特剪切流流量的计算误差进行了分析,给出了该公式的适用范围,同时对有限宽度矩形断面管剪切流公式进行了曲线拟合,得到了便于工程使用的流量计算公式。     

研究大分子溶液流变性质的核磁共振成象实验装置

在Bruker MSL-400微成象谱仪上建立了一个研究大分子溶液流变性质的核磁共振成象的装置.此方法取决于两个方面:1)具有一个能产生稳态流动的Couete cell装置,2)使用能得到正常核磁共振流速象的脉冲序列.从成象数据很易得到剪切应力与剪切速度的关系.     

CTAC表面活性剂水溶液的流变特性

在25℃条件下,测量了质量分数w=0.007%～0.15%范围内表面活性剂水溶液的流变特性。实验结果表明,表面活性剂稀溶液在剪切作用下出现剪切增稠转变,随着溶液浓度的增加,剪切增稠转变越来越弱。当浓度达到某一临界饱和浓度时,不再有剪切增稠转变发生,该浓度所对应的流变曲线称为最大黏度线;对于表面活性剂稀溶液,剪切诱导时间和剪切平衡时间均是剪切速率的幂函数,幂指数为-1.0;剪切增稠转变结束后,表面活性剂稀溶液的稳态黏度随浓度增大而增大,当w>0.05%时,稳态黏度逼近最大黏度线,继续增大浓度,稳态黏度几乎保持不变。     

托卡马克等离子体不同运行模式下的电子回旋波电流驱动

在给定等离子体密度分布下，从电子、离子的能量方程出发，根据不同运行模式下等离子体的热传导率不同，分别求出了中心负剪切模式，常规剪切H模式和L模式下的等离子体温度分布，然后通过求解波迹方程与相对论情况下的Fokker-Planck方程，分别计算了这些模式下的电子回旋波电流驱动和波功率沉积.得到在中心负剪切下，驱动电流最大，驱动效率最高，功率沉积和电流分布区间跨度大；在常规剪切H模式下，驱动电流较小，分布区间跨度比较窄，驱动效率相对较低；在常规剪切L模式，驱动电流效率最低，分布区间跨度也非常集中. 关键词： 托卡马克 电子回旋波电流驱动 中心负剪切 常规剪切     

背景磁场下Y系超导带材临界电流的测量

高温超导电力装置一般工作于低磁场情况下,测量超导带材在低场下的临界电流特性非常重要.文中通过自行设计的实验平台,采用四引线法对Y系超导带材低场下的临界电流特性进行了测量,得到了带材临界电流随外加磁场变化的曲线,并与Bi系带材低场下的临界电流特性进行比较.     

分散介质和温度对纳米二氧化硅胶体剪切增稠行为的影响

对分散介质和温度对纳米二氧化硅胶体剪切增稠行为的影响进行了系统研究. 用四种液体分散介质(乙二醇, 聚乙二醇400, 丙二醇, 聚丙二醇400)制备的纳米二氧化硅胶体表现出不同的连续剪切增稠或者跳变剪切增稠行为. 温度上升降低了分散介质的黏度, 进而降低了胶体的表观黏度. 剪切增稠的临界黏度与温度的关系符合“Arrhenius”公式的描述. 胶体黏度与分散介质黏度的比值用来归一化不同温度下的稳态剪切流变曲线. 在低剪切速率的剪切变稀阶段, 剪切变稀现象与分散介质黏度没有明显相关性, 而与分散介质的化学性质密切相关. 在高剪切速率的剪切增稠阶段, 分散介质黏度越高, 胶体剪切增稠现象越强烈.     

自组装双硫醇分子膜在交流电场下的介电特性

研究了交流电场下双巯基烷烃硫醇自组装分子膜的阻抗谱.利用汞金属作为衬底,制备出双巯基烷烃硫醇自组装分子膜,并通过交流频谱仪对其进行频谱的扫描.通过实验明确了膜的作用范围为阻抗谱中频部分,并给出相应的等效电路对阻抗谱进行了拟合.同时,根据损耗谱中损耗峰随硫醇碳链原子数的增加而向低频方向移动的现象得出双巯基硫醇Cn(n=3～10)在交流电场下的动能为14～48 meV.     

环状聚合物及其对应的线性链熔体在启动剪切场下流变特性的分子动力学模拟研究

采用非平衡分子动力学方法研究了环状聚合物及其对应的线性链熔体在启动剪切场下的结构与流变特性.模拟结果显示:低剪切速率下(■1×10~(-4)τ~(-1))环状链分子体系相比于同分子量的线性链体系并没有出现明显的过冲现象.该结果表明,在启动剪切场下环状分子与其对应的线性链相比较表现出了更弱的分子形变,同时模拟结果也与最近实验观察的结果一致.为了进一步探究这种现象背后的分子机理,在分子层面统计了不同流场强度下,链段的长度和取向角分布随着应变的演化,统计结果证明了环状聚合物分子链段弱的形变是导致其弱的剪切变稀和峰值应变的主要因素.本文还给出了过冲点和稳态在不同剪切速率下环状分子与其对应的线性链的流变特性(过冲应变、最大应力、最大黏性和稳态黏性)、结构和取向参数与维森伯格数(Wi_R)所满足的标度关系.     

自组装双硫醇分子膜阻抗谱的研究

对交流电场下双巯基烷烃硫醇自组装分子膜的阻抗谱进行了研究.利用汞金属作为衬底,制备出双巯基烷烃硫醇自组装分子膜,并通过交流频谱仪对其进行频谱的扫描．明确了膜的作用范围为阻抗谱中频部分为了解释该阻抗谱,提出了一种串联的等效电路来进行了拟合,并与其他的模型进行比较.同时,观察到在损耗谱中损耗峰随硫醇碳链原子数的增加而向低频方向移动并得出双巯基硫醇(C6-C10)在交流电场下的激活能为23～39 meV．     

Phase transition in electrorheological plasmas

Applying an external electric AC field to a dusty plasma, the micro-particles arrange in strings or chains. In analogy to electrorheological fluids, such a system is called electrorheological plasma. Turning gradually the AC field into a DC field, the string formation is diminished until it vanishes completely in the DC case. In this way, a cross-over transition from a string-like to an isotropic micro-particle many-body system can be investigated. Experimental investigations of electrorheological plasmas are performed under microgravity conditions in parabolic flights. For analysing the image data, a supervised machine learning code was developed and a continuous cross over was found. A molecular dynamics simulation showed qualitatively similar results but also some deviations from the experimental results.     

极性分子型电流变液导电机理研究

极性分子型电流变液是一种新型的电流变材料.其介电颗粒上吸附极性分子,极性分子在颗粒间强局域电场作用下发生取向是产生巨电流变效应的关键.通过对Ca—Ti—O(CTO)体系极性分子型电流变液电流密度的测量发现,其导电行为遵从Poole-Frenkel效应的规律,这是极性分子型电流变液的重要特征之一.而500 ℃处理过的CTO粉体不含极性分子,所配制的电流变液无巨电流变效应,其电流密度随外电场强度近似地呈线性关系,显示出传统电流变液特性.     

TiO2包覆石墨颗粒/硅油电流变液的研究

理论计算表明,介质包覆导体颗粒用作电流变液的分散相,可以获得高剪切应力的电流变液.采用溶胶-凝胶技术在尺度为5—10μm的石墨颗粒表面成功地包覆了TiO₂,获得了金红石相TiO₂包覆石墨的复合颗粒.配制成复合颗粒/硅油电流变液,其剪切应力与纯TiO₂/硅油电流变液相比,可提高一个数量级.当电场强度为1.7kV/mm时,复合颗粒/硅油电流变液的剪切应力可达1.25kPa,电流密度小于10μA/cm². 关键词： 电流变液 包覆 2')" href="#">TiO₂ 石墨     

Carbon nanotube/polyaniline nanocomposites and their electrorheological characteristics under an applied electric field

A conducting polyaniline (PANI) was synthesized via an oxidative dispersion polymerization technique, using poly(vinyl alcohol) (PVA) as a polymeric stabilizer, in the presence of multi-walled carbon nanotubes (MWNT) purified in acidic solution, and dispersion stability of the MWNT in an aqueous solution of PVA was studied for different PVA concentrations. Their morphology was confirmed by a scanning electron microscope. Its electrorheological (ER) characteristics were also investigated by dispersing the PANI/MWNT composite particles in an insulating silicone oil. Its ER properties were examined using a rotational rheometer under varying applied DC electric field strengths, in which the ER fluid is generally composed of a suspension of conducting particles dispersed in an insulating fluid, which shows a rapid and reversible change in shear viscosity with an applied electric field. Synthesized PANI/MWNT composite particles are observed to enhance interparticular interactions, since the degree of polarization of PANI/MWNT composite particle increases with applied electric field strengths. The shear stresses of the PANI/MWNT nanocomposite based ER fluid increase with the electric field strength for a broad range of shear rates.     

Conductivity effect in electrorheological fluids

Based on conduction model and cubic particle model, the relationship between current density and shear yield stress of electrorheological (ER) fluids was calculated and compared with some reported experimental results. The conductivity of the insulating oils is found to have been changed by the mixed particles. Several ways to decrease insulating liquid conductivity and increase the conductivity ratio of ER fluids have been proposed to prepare ER fluids with high shear yield stresses but low current densities.     

Conductivity effect in electrorheological fluids

Based on conduction model and cubic particle model, the relationship between current density and shear yield stress of electrorheological (ER) fluids was calculated and compared with some reported experimental results. The conductivity of the insulating oils is found to have been changed by the mixed particles. Several ways to decrease insulating liquid conductivity and increase the conductivity ratio of ER fluids have been proposed to prepare ER fluids with high shear yield stresses but low current densities.     

电流变液的流变学响应与其非线性介电性质的关系

对两类电流变液的介电性质的测量结果表明，强交流电场下电流变液经历介面极化；而且是一种非线性极化．根据海藻酸钠和NaY沸石电流变液的动态剪切应力与强电场介电谱相似这一事实，确定了这两种样品的流变学响应时间下限，它们分别是1ms和0.7ms．还发现NaY电流变液的动态切应力与非线性三次谐波的强度有关；一种高分子半导体电流变液的流变学响应基本不受样品含水量的影响．对上述实验结果进行了解释 关键词：     

Shear Stress and Dielectric Analysis of H3PO4 Doped Polyaniline Based Electrorheological Fluid

We synthesized phosphoric acid (PA) doped polyaniline (PANI) particles (PANI‐PA) and investigated their electrorheological (ER) and dielectric characteristics when they were dispersed in silicone oil. Flow curves of the PANI‐PA based ER fluid under several applied electric field strengths were analyzed using a shear stress model. We also examined ER characteristics based on the relaxation time obtained from the dielectric spectrum.     

固液双相电流变系统流动过程的相转变特性

考虑电流变液多粒子近程相互作用，利用等效平板电导模型，研究了电流变液流动过程相转变点的特性，并设计实验观察了电流变液中的这种相转变现象.研究结果表明，电流变液在一定压力梯度作用下发生流动，此时为双相流；当外加电场达到某一值时，电流变液中颗粒不流动，由固液双相流转变为液体单相流动，发生场控相转变，理论模拟结果与实验观察结果基本相符.阈值电场随外加压力梯度的增加而加大，随颗粒浓度的增加而减小. 关键词： 电流变液 颗粒流 相转变     

Shear Stress and Dielectric Characteristics of Polyaniline/TiO2 Composite‐Based Electrorheological Fluid

Adopting both conducting polyaniline (PANI) and organic titanium dioxide (TiO₂), which possesses a high dielectric constant, we synthesized PANI/TiO₂ hybrids via in situ oxidative polymerization to prepare an electrorheological (ER) materials. These were then characterized via thermogravimetric analysis (TGA) and scanning electron microscopy (SEM). The ER responses and dielectric properties of the synthesized hybrids dispersed in silicone oil were measured as a function of different particle fractions of TiO₂ under an applied electric field. Series of analyses revealed that composite composition (the ratio of TiO₂ to PANI) plays a crucial role in affecting the ER performance, which exhibited interesting behaviors when the ratio of TiO₂ to PANI approaches a critical value. Interestingly, we found that our proposed constitutive equation fit the shear stress in the low shear rate region better than the Bingham fluid model. The dielectric spectra of the ER fluid, along with polarizability, were found to explain the flow behaviors of the PANI/TiO₂ under applied electric fields.