RAFMs �к��TIG ���µ��¶ȳ���Ӧ�����о�

应用ANSYS软件对低活化马氏体/铁素体钢(RAFMs)中厚板多道焊接过程进行三维有限元模拟,将得到的温度场和应力场分别与实验对比,对焊缝区和热影响区宽度进行预测,并通过焊接实验进行验证,同时对焊后的试件进行了金相分析和硬度测试。结果表明：温度场和应力场模拟结果和实测结果基本一致,焊缝区以及热影响区宽度的模拟结果和实测结果基本吻合;采用316L焊丝填充的焊缝,焊缝与母材熔合较好,焊缝没有明显缺陷;硬度检测呈现：焊缝的硬度大大高于热影响区和母材。     

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For simplifying the calculation the magnetic distribution on tokamak, some two-dimensional analytic models including the effect of the iron core were established, such as the infinite long iron core model and the spool model. The assumptions of these two-dimensional analytic models lead to different results with the actual magnetic field due to the distinctive boundary condition. In order to accurately calculate the three-dimensional magnetic field distribution in the tokamak with iron core, a three-dimensional numerical finite element model was established based on J-TEXT tokamak. In two conditions, where the total toroidal current is nonzero or zero respectively, more comparison were carried out between the derived results of two-dimensional models and the results at different toroidal positions in three-dimensional models. Furthermore, the toroidal asymmetry of the magnetic field distribution of the three-dimensional model of tokamak with iron core was investigated. The results indicate that the three-dimensional construction of iron core causes the toroidal asymmetric poloidal magnetic field and the difference between the two- and three-dimensional models in the condition with total current of nonzero. However, in the condition with total current of zero, the intensity of toroidal asymmetric is reduced and the difference between the two- and three-dimensional models is smaller.     

HL-2Mƫ�������ۺ�ģ�⼼�������о�

利用SOLPS和DINA程序,对偏滤器的数值模拟进行综合研究。结合HL-2M装置,针对偏滤器的结构优化、脱靶物理过程、偏滤器送气与抽气、垂直位移事件(VDE)等问题进行了模拟研究。分析了偏滤器靶板位形以及脱靶对偏滤器靶板热载荷的影响,研究了偏滤器的送气位置、送气速率、抽气速率等因素对于偏滤器性能的影响;同时,利用DINA程序对HL-2M装置的VDE过程进行了预测分析,并给出了HL-2M装置发生VDE过程的等离子体电流剖面变化,从而为HL-2M装置的偏滤器结构设计和分析提供输入数据。     

�۱����CLF-1 ����316L ��TIG ���ӽ�ͷ��֯�����ܳ����о�

A preliminary study of microstructure and properties of the welded joint of low activation CLF-1 steel used for fusion reactor and 316L dissimilar metal by tungsten inert gas (TIG) welding using W19123L as filler material, has been performed. The welded joint forming is proved well and without defect. The welded joint consists of CLF-1 zone [base metal (BM), heat affected zone (HAZ), fusion zone (FZ)], inside layer (IL), weld zone (WZ), and 316L zone (BM, HAZ, FZ). Tensile strength of the joint is better than the base metal minimum value in room temperature. Both surfaces of welded joint are without crack and with deformation uniformity under the bending test. The distribution of impact value of the joint is concave-like and satisfies the designed values for the welded joint, the WZ’s value is the lowest, the HAZ’s of both WZ zones is the second, the BM’s was the best, and the 316L steel zone’s is slightly larger than the CLF-1 zone’s. The hardness values of the point under the 1.6mm top surface of welded joint have a larger fluctuation range, and is slightly higher than those of 1/2T and above down surface 1.6mm position. The hardness distribution of 1/2T and above the down surface 1.6mm position is roughly uniform, and has a downward trend from the CLF-1 zone to 316L zone. Welding properties generally has remained stable and satisfy the requirement of dissimilar steel welding performance matching.     

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Based on ORBIT code of a guiding center motion of single particle, the loss of energetic ions in different radial positions of tokamak plasma is studied by using test particle simulation method. The results show that the local magnetic perturbations can cause loss of many energetic ions near the central region of the plasma, but they have little effect on the ion loss near the plasma boundary, assuming that the local field is mainly located near a magnetic surface and its toroidal field is similar to the ripple field. These energetic ions are trapped ions, and the greater their pitch angle is, the easier they lose. In addition, the radial position of the local field that causes the maximum loss rate of energetic ions is usually offset from the initial radial position of these loss ions, and this shift is closely related to the energy of these ions. When the local field appears in certain locations, the ions of lower energy have some loss, but the ions higher energy does not lose.     

HL-2Mװ�ü�����Ȧ�����ͭ��������칤���о�

介绍了HL-2M装置极向场线圈所需的大截面外方内圆铜导体的规格,用二辊周期式轧管机进行冷轧的工艺技术以及所做的多项检测.用这个技术制造了具有冷却水孔道的大截面外方内圆铜管.测试结果表明,该工艺生产的外方内圆铜管在尺寸及各项性能上均满足HL-2M托卡马克装置极向场线圈的加工要求.     

HL-2M�������崹ֱ���ȶ����о�

用DⅢ-D的TokSys研究了HL-2M等离子体垂直不稳定性控制问题.使用真空室和主动线圈控制等离子体垂直不稳定性,分析了真空室的本征模和电流分布,极大简化真空室建模难度,建立了垂直不稳定性数学模型,验证了主动线圈和电源模型参数,计算了不同拉长比位形的等离子体增长率和最大可控垂直位移.利用TokSys建立了雪花、单零、双零偏滤器位形垂直不稳定仿真模型,然后通过simulink对采用PD算法的垂直不稳定系统进行仿真.结果表明,构建的模型能够较好控制不同位形的垂直不稳定性.     

HL-2Mƫ����CFC/CuCrZr�а�ķǾ�ǥ�������о�

The brazing process of chlorofluorocarbon/oxygen-free-copper (CFC/OFC) composite mockup and CuCrZr at 710~750°C by vacuum brazing and with STEMET-1101 amorphous filler is studied. Firstly, the microstructure and melt behaviors of the filler are characterized by means of XRD and differential scanning calorimetry and then the organism form, elemental distributions, phase structures, and mechanical property in the bonding seams are studied by using optical microscopy, electron probe microanalysis and tensile tests. The thermal fatigue property of CFC/OFC/CuCrZr brazing mockup is measured with the high heat flux facility. The results show that the bonding seam consists of Ni(Cr, Cu)2P particles, Cu(Ni)3P phase and Cu matrix in brazing temperature of 710~750°C, which is smooth and crack-free. Especially, a continued intermetallic phase network in the bonding seam is depressed in the case of 750°C/15min treatment. The welding strength of the OFC/CuCrZr is higher than tensile strength of OFC. The bonding strength of CuCrZr/CuCrZr joint is 210MPa and fracture is partly ductile. The CFC/Cu/CuCrZr mockup prepared in the case of 750°C/15min treatment can tolerate 7MW·m^-2 high heat flux under 1000 cycles.     

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HL-2A和HL-1M装置采用了激光吹气注入高Z杂质来缓减大破裂中的等离子体电流衰竭,并给出了初步实验结果。在HL-2A装置上建立了利用MHD扰动的参量预报放电破裂先兆的报警系统,研制了MHD实时检测与处理系统,实现了放电破裂先兆的预报、快速触发激光吹气、形成阻性高辐射等离子体、消耗热能和磁能,缓减大破裂。实验证明,这是一种使得大型聚变实验装置在放电破裂之前显著减少等离子体中热能和磁能,而且能安全终止放电的简单、快速和有效的途径。     

HL-2M �������Inconel 625 ���������о�

HL-2M真空室的主体材料被选为Inconel 625。通过研究3个产地的Inconel 625母材和焊缝的性能,对比分析了该种材料的各项性能参数。通过比较得到进口Inconel 625母材和焊接接头综合性能均最优。各项试验结果及分析对真空室部件的制造有重要的指导意义。     

Two-photon E1M1 and E1E2 transitions between 2p and 1s levels in hydrogen

Two-photon transitions in the hydrogen atom are analytically evaluated within the nonrelativistic limit utilizing the Coulomb Green function method. The two-photon emission probability for the transition process 2s→2γ(E1)+1s serves as a test for the other calculations and was compared with the results of previous analytical and numerical calculations. The two-photon emission probabilities for the processes 2p→ γ(E1)+γ(M1)+1s and 2p→γ(E1)+γ(E2)+1s are also evaluated and compared with previous numerical calculations. Different nonrelativistic “forms" for the decay probabilities in combination with different gauge choices are considered.     

金等离子体中Au51+能级寿命的相对论多组态计算

根据扩展的相对论多组态 Dirac-Fock理论,采用"多功能相对论原子结构程序(Grasp2) ",选用二参数Fermi有限核模型计算类镍Au51+ 的能级寿命和能级宽度及光谱跃迁波长、跃迁几率和振子强度,计算所得波长值与实验值符合得很好,能级寿命与能级宽度的大小关系符合海森堡的能量与时间测不准原理.     

激光金等离子体中Au52+静态能级寿命的相对论多组态计算

根据扩展的相对论多组态Dirac-Fock理论,采用"多功能相对论原子结构程序(GRASP2)",计算类钴Au52+的能级寿命、能级宽度和光谱跃迁波长,计算所得波长值与实验结果符合较好.能级寿命与能级宽度的大小关系符合海森堡的能量与时间测不准原理.     

M1 and E2 transitions in 59Ni

Employing the Kuo-Brown interaction, M1 and E2 transition rates for the low-lying levels of ⁵⁹Ni are calculated and the results are found to be in reasonably good agreement with the observed values.     

金等离子体中Au48+—Au52+平衡分布的统计热力学研究

基于全相对论多组态Dirac-Fock理论，采用“多功能相对论原子结构程序(GRASP2)”，考虑量子电动力学(QED)效应和Breit修正，涉及实验谱中Au等离子体M带的几类重要跃迁，计算了Au48+—Au52+离子的能级结构和能级简并度.用统计热力学方法计算 各离子的配分函数，由配分函数计算等离子体内这五种离子的电离与复合平衡常数，根据同 时反应的平衡理论研究电离与复合达到平衡时等离子体内各离子的相对分布. 关键词： 金等离子体 配分函数 平衡常数 离子丰度     

金等离子体中Au48+-Au52+平衡分布的统计热力学研究

基于全相对论多组态Dirac Fock理论 ,采用“多功能相对论原子结构程序 (GRASP2 )” ,考虑量子电动力学 (QED)效应和Breit修正 ,涉及实验谱中Au等离子体M带的几类重要跃迁 ,计算了Au4 8 —Au52 离子的能级结构和能级简并度 .用统计热力学方法计算各离子的配分函数 ,由配分函数计算等离子体内这五种离子的电离与复合平衡常数 ,根据同时反应的平衡理论研究电离与复合达到平衡时等离子体内各离子的相对分布基于全相对论多组态Dirac Fock理论 ,采用“多功能相对论原子结构程序 (GRASP2 )” ,考虑量子电动力学 (QED)效应和Breit修正 ,涉及实验谱中Au等离子体M带的几类重要跃迁 ,计算了Au4 8 —Au52 离子的能级结构和能级简并度 .用统计热力学方法计算各离子的配分函数 ,由配分函数计算等离子体内这五种离子的电离与复合平衡常数 ,根据同时反应的平衡理论研究电离与复合达到平衡时等离子体内各离子的相对分布     

Observation of Au + Au → Au + Au + ρ 0 and Au + Au → Au* + Au* + ρ 0 with STAR

We report the first observation of the reactions Au + Au → Au + Au + ρ ⁰ and Au + Au → Au* + Au* + ρ ⁰ with the STAR detector. The ρ are produced at small perpendicular momentum, as expected if they couple coherently to both nuclei. We discuss models of vector meson production and the correlation with nuclear breakup, and present a fundamental test of quantum mechanics that is possible with the system.