等离子体中弹丸消融的探讨

本文采用弹丸消融的双区域模型,对弹丸消融过程进行了数值求解。分析Parks的模型,发现其定标律不适合于高温度、低密度的等离子体中弹丸的消融。估计了热电子能量分布函数对消融率的影响。     

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建立了计算托卡马克加料中弹丸消融的物理模型,结合1维输运模型编制了1.5维弹丸消融计算机模拟代码。使用ITER-FEAT的相关参数,对半径为6mm,初速度为2000m·s?1,从低磁场侧注入弹丸的消融速率进行了模拟计算。结果显示,弹丸消融速率先随注入深度而逐渐增大,最大消融速率约6×1026s?1,然后由于弹丸半径的减小,消融速率迅速减小,穿透深度约0.45m。这一结果与中性气体屏蔽模型(NGS)的结果一致,证明计算代码正确有效。同时,从计算结果反映出,对ITER这样的堆级托卡马克,采用常规弹丸注入方式,尽管速度高达2000m·s?1,穿透深度也远未达到等离子体中心,因此应采取其他有效措施来提高等离子体加料效率。     

HL—1M多发弹丸加料等离子体的特性

对ＨＬ－１Ｍ装置在一次放电中注入３－８粒氢弹丸的欧姆加热等离子体密度分布和扰动特征进行了研究。实验表明,器壁再循环对高密度的获得有重要的影响。在再循环较高的条件下连续注入３粒１．０ｍｍ弹丸,获得了加料实验的最好参数：等离子体中心密度ｎｅ（０）＝５．３×１０１３ｃｍ－３,总体储能Ｗｐ＝６．０ｋＪ,τｅ＝２６ｍｓ。用ＣＣＤ相机拍摄了弹丸消融云的照片,并对消融过程进行了简要的分析。结果证实,消融的不对称和弹丸轨迹的偏转是电子侧消融强于离子侧的结果,弹丸发射间隙及完整性对密度扰动有重要的影响。     

HL—1M装置多发弹丸加料实验观测

首次在ＨＬ－１Ｍ装置上投放使用的多发弹丸加料系统，能一次注入多达４粒Φ１．０ｍｍ的氢弹丸，弹丸速度在５００－８００ｍ．ｓ＾－１之间。弹丸注入后，得到离子体密度峰化系数ｎｃ（０）／〈ｎｃ〉＝１．８能量约束时间与喷气加料放电的相比提高３０％以上的实验结果。观察到了弹丸注入等离子体引起弹丸消融物沿磁力线流动的图像变化，电子温度分布和ＭＨＤ行为的演变过程以及新的边缘等离子体特性。     

CCD在弹丸消融观测的应用

 描述CCD器件在HL-1M多发弹丸加料实验中观测短暂消融云的应用结果,并介绍一种有特色的触发方式 用弹丸自身辐射的氢a 射线启动相机。实验证明：这种安排能取得大量照片,CCD成功地应用于弹丸消融过程观测, 图片处理分析后获得消融云形状、结构和辐射强度分布等。可以相信CCD诊断方法不但加深了弹丸加料的认识,也会促进军事工程相关瞬态高速过程的研究。     

CCD在弹丸消融观测的应用

描述CCD器件在HL-1M多发弹丸加料实验中观测短暂消融云的应用结果,并介绍一种有特色的触发方式 用弹丸自身辐射的氢a 射线启动相机。实验证明:这种安排能取得大量照片,CCD成功地应用于弹丸消融过程观测, 图片处理分析后获得消融云形状、结构和辐射强度分布等。可以相信CCD诊断方法不但加深了弹丸加料的认识,也会促进军事工程相关瞬态高速过程的研究。     

CCD在弹丸消融观测的应用

描述CCD器件在HL-1M多发弹丸加料实验中观测短暂消融云的应用结果,并介绍一种有特色的触发方式 用弹丸自身辐射的氢a 射线启动相机。实验证明：这种安排能取得大量照片,CCD成功地应用于弹丸消融过程观测, 图片处理分析后获得消融云形状、结构和辐射强度分布等。可以相信CCD诊断方法不但加深了弹丸加料的认识,也会促进军事工程相关瞬态高速过程的研究。     

高温等离子体中固体弹丸消融过程的研究

本文求得了弹丸消融过程的自洽解析解。结果表明:Parks的弹丸消融理论需要修正;弹丸消融速率由消融物云和表面蒸发层共同控制;入射电子通过消融物云时慢化效应并不显著;消融物离开弹丸表面时一般呈部分电离态;聚变堆条件下,弹丸表面可能会出现激波。     

高速弹丸测速仪的研制

在等离子体物理实验中,注入弹丸的大小和速度对等离子体电子温度、密度扰动等均有影响,测量弹丸的速度有助于研究弹丸注入等离子体的深度、弹丸的消融及其对等离子体的作用。8发弹丸系统原有的测速仪是从俄罗斯引进的,其灵敏度、抗干扰能力都较差,加料实验时该测速系统根本无法正常工作。为此,必须研制一套精度高、抗干扰强、速度测量范围广（几m·s^-1-3000m·s^-1)的测速系统以满足实验的需要。     

Numerical simulation of fueling pellet ablation and transport in the EAST H-mode discharge

To understand the effect of injected deuterium (D) pellets on background plasma, the ablation of D pellets and the transport of D species in both atomic and ionic states in the EAST device are simulated using a modified dynamic neutral gas shield model combined with the edge plasma code SOLPS-ITER. The simulation results show that there is a phenomenon of obvious atomic deposition in the scrape-off layer (SOL) after pellet injection, which depends strongly on the injection velocity. With increasing injection velocity, the atomic density in the SOL decreases evidently and the deposition time is relatively shortened. Possible effects for triggering of edge localized modes (ELMs) by D and Li pellets are also discussed. With the same pellet size and injection velocity, the maximum perturbation pressure caused by D pellets is obviously higher. It is found that the resulting maximum perturbed pressure is remarkably enhanced when the injection velocity is reduced from 300 m/s to 100 m/s for a pellet with a cross section of 1.6 mm, which indicates that the injection velocity is important for ELM pacing. This work can provide reasonable guidance for choosing pellet parameters for fueling and ELM triggering.     

改善ITER 弹丸注入芯部加料的研究

研究了五种不同组合的固态氢同位素靶丸H₂、HD、D₂、DT 和T₂ 在聚变等离子体中的消融率。结果表明, 燃料靶丸的同位素效应, 可导致更深的靶丸消融物质沉积。在同样的本底等离子体条件和弹丸初始参数下, 注入氚丸比氢丸的穿透深度增加约40%。适度减轻一些ITER 的加料困难。进一步的研究表明从中平面高场侧注入靶丸对芯部加料有显著改善。考虑托卡马克非均匀磁场的影响, 被电离的消融云内的垂直漂移电流产生极化, 引起带电消融物沿大半径方向朝外漂移。数值模拟计算表明, 只要用初始速度为每秒几百米的低速弹丸, 便能使靶丸的消融物质沉积到ITER 等离子体中心。     

A new method to calculate corneal ablation depth based on optical individual eye model

The corneal shape, axial lengths and the wavefront aberrations of the eye were all considered to calculate the ablation depth based on the individual eye model. The optimization method for the curves surface replaced the direct calculation from only the optical path difference method (OPD). We analyzed the eye's optical system on its exit pupil and offered the optimum corneal anterior surface. And the ablation depth was the difference between the pre- and post-optimization along the optical axis of the eye. In our experiment, the maximum ablation depth decreases by 8.5% and the mean ablation depth decreases by 8.2% compared with the OPD method.     

碘气流穿透深度和碘流量对COIL激光输出功率的影响

 通过采用Cl₂流量250mmol/s列管射流式氧发生器的COIL出光实验，得到了激光输出功率随碘副气流相对于氧主气流混合穿透深度的变化规律。实验结果表明，穿透深度对激光功率影响较大，存在最佳穿透深度，约为3.16mm,计算的最佳穿透深度与实验得到的最佳穿透深度基本一致。通过逐步改变供碘系统的碘气流流量，测量激光的输出功率，在实验上证实并找到了COIL的最佳碘流量值，约为4.5mmol/s，这一结果比以往文献所登载的最佳碘流量值要确切。     

托卡马克装置弹丸加料系统中一种新的低温制丸技术的探索

提出了一种新的低温制丸技术磁制冷技术 ,并探索其在托卡马克装置弹丸加料系统中的应用     

Ultra-short laser ablation of dielectrics: Theoretical analysis of threshold damage fluence and ablation depth

A coupled theoretical model based on Fokker–Planck equation for ultra-short laser ablation of dielectrics is proposed. Multiphoton ionization and avalanche ionization are considered as the sources during the generation of free electrons. The impact of the electron distribution in thermodynamic nonequilibrium on relaxation time is taken into account. The calculation formula of ablation depth is deduced based on the law of energy conservation. Numerical calculations are performed for the femtosecond laser ablation of fused silica at 526 and 1053 nm. It shows that the threshold damage fluences and ablation depths resulted from the coupled model are in good agreement with the experimental results; while the damage thresholds resulted from the approximate model significantly differ from the experimental results for lasers of long pulse width. It is concluded that the coupled model can better describe the micro-process of ultra-short laser ablation of dielectrics.     

Enhancement of ablation rate and production of colloidal nanoparticles by irradiation of metals with nanosecond pulsed laser in presence of external electric field

This paper presents the results of experimental study on the effect of electric field on the ablation rate during the nanosecond pulsed laser ablation of aluminum and copper in deionized water. The effect of electric field strength on the material removal rate and its mechanisms were investigated both in the electric field parallel and perpendicular to the laser beam path schemes. The ablation rate was estimated by measuring the dimensions of craters on the target induced by laser. The crater dimensions and optical properties of the produced colloidal nanoparticles were characterized by means of optical microscopy and UV–Vis absorption spectroscopy, respectively. The results indicate that pulsed laser ablation in the presence of an electric field significantly leads to higher material removal rate. The experimental results also confirm that the crater geometry extremely depends on the direction of the electric field with respect to the laser beam direction. The UV–Vis spectra show that the nanoparticles production efficiency increases with increasing the electric field strength.     

The Design for Automation of Pellet-Forming Process in HL-2A Pellet Fueling System

In the ever fusion experiments in SWIP, pellet forming process was carried out through adjusting relative devices by staff member in site, which will make every pellet-forming process slight distinction and will result in pellet difference in shape, size and intensity. In the intervals of HL-2A discharges, staff member have to go site to accomplish the pellet-forming process, this wastes human power and increase the potential danger. So it is necessary to develop a remote control system to perform the pellet-forming process. The control system needs have the features of real-time, reliability and be easy to operate and maintain.