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1.
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。  相似文献   

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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。  相似文献   

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HL—1M装置多发弹丸加料实验观测   总被引:9,自引:2,他引:7  
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。  相似文献   

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HL—1M多发弹丸加料等离子体的特性   总被引:5,自引:0,他引:5  
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。  相似文献   

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焦一鸣  周艳  姚良骅  董家齐 《物理学报》2004,53(4):1123-1128
讨论并研究了超声分子束在托卡马克等离子体中的消融和穿透问题,其中包括了分子束的绝热膨胀,团簇的形成和解离,束的静电屏蔽效应和冷通道效应.研究结果表明,在考虑了这些效应以后数值得到的结果与实验结果相近.这些研究对于更好地理解超声分子束与等离子体的相互作用和优化设计加料系统有一定作用. 关键词: 超声分子束 加料 托卡马克等离子体 消融和穿透  相似文献   

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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  相似文献   

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报道了HL-2A装置最新的实验结果,讨论并研究了超声分子束的注入位置对分子束在等离子体中的消融和穿透的影响,其中包括电离后的分子束粒子在磁场梯度作用和 E × B 漂移下的加速或减速及由此形成的冷通道效应.研究结果表明,磁场梯度和 E × B 漂移对于超声分子束的加料效果、消融和穿透有着重要的作用.强场侧注入可使电离后的电子和离子更深地进入等离子体芯部.这些研究对于更好地理解超声分子束与等离子体的相互作用和优化设计加料系统有一定作用.  相似文献   

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Wan-Ting Chen 《中国物理 B》2022,31(7):75204-075204
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.  相似文献   

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改善ITER 弹丸注入芯部加料的研究   总被引:1,自引:1,他引:0  
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。  相似文献   

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 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。  相似文献   

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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.  相似文献   

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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.  相似文献   

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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.  相似文献   

17.
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.  相似文献   

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