HIRFL-CSRm纵向随机冷却-槽形滤波冷却模拟研究

 通过Fokker Planck方程,对拟在HIRFL-CSRm上建造的纵向槽形滤波器（notch filter）的冷却机理进行了研究,得出了冷却原理及冷却时间的表达式,并对影响冷却时间和冷却效果的因素进行了模拟和讨论,模拟结果表明,噪信比越小,冷却时间越短,冷却效果越好;带宽越宽冷却越快。该研究为具体纵向冷却系统的设计和优化提供了依据。     

HIRFL–CSRm Betatron振荡随机冷却

对拟在HIRFL CSRm上建造的横向自由振荡随机冷却进行了数值优化计算和设计,得到了最佳带宽、冷却时间、频谱上束流谱密度分布函数随时间的变化,以及在冷却过程中束流横向位移的分布等值,并且对功率限定情况作了讨论,从而为冷却系统的设计、优化、建造和运行提供了理论依据     

储存环内电子冷却过程模拟

考虑储存环内离子的横向振荡和纵向振荡的运动特性,模拟了HIRFL-CSR内重离子束的电子冷却过程.给出了离子束的横向发射度和纵向动量散度随时间连续变化的图象,由此分析了电子束的空间电荷效应,冷却段色散函数和横向电子束温度对冷却过程快慢的影响.     

储存环中横向和纵向相空间随机冷却的二维计算

 对兰州重离子冷却储存环HIRFL CSR的随机冷却装置进行了设计。基于Fokker Planck方程，对陷波器方式纵向冷却及横向冷却时间作了二维计算，在计算过程中，得到并使用了冷却最快的增益曲线。     

CSRm随机冷却初步设计

根据实际情况对兰州重离子加速器冷却储存环主环随机冷却做了初步设计和优化, 用冷却方程对主环随机冷却做了详细的数值模拟计算. 研究表明, 随机冷却对主环束流冷却速度很快, 冷却效果很好. 通过对电子冷却和随机冷却的比较, 提出主环的束流冷却采用电子冷却和随机冷却相结合的办法, 这样可以加快冷却速度, 得到更高流强、更好品质的束流.     

新型双射流冷却孔对气膜冷却效率影响的研究

气膜冷却是现代航空燃气轮机涡轮冷却技术的一种重要方法,冷却孔形状的改进是提高气膜冷却效率的重要手段。本文对双射流冷却孔形状进行了改型,并对新型双射流冷却孔在吹风比分别为0．5,1．0,1．5,2．0时的冷却效率进行了数值模拟。模拟结果表明新型双射流冷却孔与原双射流冷却孔相比在各吹风比下均优化了气膜在热表面上的分布,抑制...     

CSR实验环电子冷却装置的纵向电子束温度

电子冷却装置中, 电子束纵向温度是计算冷却力的主要参量之一. 当电子与被冷却离子的相对速度很小时, 纵向冷却力与离子速度呈线性关系, 并且线性区域的宽度与电子束纵向温度有关. 通过分析影响电子束纵向温度的主要因素, 得到了兰州重离子冷却储存环实验环(CSRe)电子冷却装置中电子束纵向温度的大小.     

交叉扭转椭圆冷却通道流动和换热研究

本文基于场协同理论,提出了一种可用于燃气透平叶片内部冷却的交叉扭转椭圆形截面内部冷却通道,其基本原理在于通过椭圆形截面通道的交叉扭转,能够实现纵向二次涡的产生,从而强化透平叶片的内部冷却。结合Fluent软件,对该通道内的流动阻力和换热特性进行了计算,并在此基础上分析了交叉扭转角度和长短轴长度比对通道内部流动和换热特性的影响。结果表明:交叉扭转椭圆截面通道使内部冷却显著强化,而流阻增加较少,计算工况下同功耗下的强化换热指标可达1.5;通道的最佳扭转角度范围宽广,实际应用中交叉扭转角度可以在45°～90°之间灵活选取;通道截面的最佳长短轴长度比为1.3～1.5。     

直接冷却高温超导电流引线的有限时间热力学分析

用有限时间热力学最小熵产率的方法对连续冷却电流引线进行优化 ,比较高温超导电流引线连续冷却和冷端冷却两种直接冷却方式。优化后的连续冷却电流引线上热流量随温度的降低而减小 ,温度在高温段变化较快 ,熵产率小。冷端冷却时在整个引线上热流量分布相同 ,温度在低温端变化较明显 ,熵产率较大。优化后的连续冷却方式比冷端冷却方式合理。     

离散孔纵向波纹隔热屏气膜冷却特性研究

本文对离散气膜孔型纵向波纹隔热屏的冷却特性进行数值计算.研究中主要参数有冷却通道无量纲高度h,波纹板无量纲高度b及气膜孔无量纲直径d.波纹板高度的变化对冷却效果的影响最为明显.波纹板高度越小,隔热屏壁面冷却效果越好.降低冷却通道高度可以提高隔热屏前面部分的冷却效果.开孔率一定,气膜孔直径较小,隔热屏冷却效果较好.     

Stochastic Momentum Cooling——Palmer Cooling at HIRFL-CSRm

The Palmer cooling is always used for large dispersion momentum cooling in storage ring. So it will be used during the stripping injection of HIRFL-CSRm. Here the Palmer cooling is described. The optimum cooling time, optimum gain and optimum cooling bandwidth are obtained in the simulation with Palmer method. Using the Fokker-Planck equation, the particle distribution with respect to the momentum dispersion is also obtained numerically during the stochastic cooling process. This is useful for analysis of experimental data and for design of the cooling system, i.e, optimization of the system passband and gain, specification of accuracy of the signal transmission, etc.     

储存环内纵向Palmer方式随机冷却过程模拟

基于Fokker–Planck方程,模拟了兰州重离子加速器冷却储存环(HIRFL–CSR)实验环内重离子束的Palmer方式纵向动量冷却过程,在模拟过程中,得到并应用使冷却达到最快的系统最优增益曲线.对模拟结果进行了讨论.     

实验环Betatron振荡随机冷却的模拟

随机冷却是一种基于带宽反馈系统对束流振荡进行衰减的冷却方法,更适合冷却较大发射度和动量分散的次级粒子束,与电子冷却互补,可以得到更高品质的束流。兰州重离子研究装置(HIRFL) 目前处于冷却存储环的实验环随机冷却系统的设计和建造阶段。通过对横向Betatron 振荡的模拟,得到了提高系统带宽、增加探测器(Pick-up) 和冲击器(Kicker) 的个数、降低系统噪声温度等对缩短冷却时间和减小冷却平衡值的重要作用。同时,分析了较大的动量分散或较大的放大器增益对Betatron 振荡冷却过程产生的加热现象。Stochastic cooling, based on a feedback system, aims at damping the oscillation of particles. Stochastic cooling is more suitable to cool secondary beam with larger size and momentum spread, and it is therefore can be complemented with electron cooling, in order to obtain beam of higher quality. Stochastic cooling system is being designed and constructed on the experimental Cooling Storage Ring of HIRFL. By simulation of Betatron stochastic cooling, it is obtained that the importance for shortening the cooling time and reducing cooling equilibrium by improving bandwidth, increasing the numbers of pickup and kicker, and decreasing the system noises. Meanwhile, the heating during the cooling process caused by larger momentum spread or larger gain of amplifier is analyzed.     

HIRFL-CSR主环电子冷却模拟计算

以¹⁶O⁸⁺为例,用电子冷却模拟程序计算了冷却时间随离子能量、初始发射度、初始动量分散、离子流强以及离子电荷态的变化规律,研究了储存环在冷却段的β函数和色散函数对冷却时间的影响.     

Commissioning of electron cooling in CSRe

The 400 MeV/u 12C6+ion beam was successfully cooled by the intensive electron beam near 1 A in CSRe.The momentum cooling time was estimated near 15 s.The cooling force was measured in the cases of different electron beam profiles,and the different angles between the ion beam and electron beam.The lifetime of the ion beam in CSRe was over 80 h.The dispersion in the cooling section was confirmed as positive close to zero.The beam sizes before cooling and after cooling were measured by the moving screen.The beam diameter after cooling was about 1 mm.The bunch length was measured with the help of the signals from the beam position monitor.The diffusion was studied in the absence of the electron beam.     

Effects of the Various Cooling Conditions on 1,064-nm nd:Yag Laser Treatment for Selective Photothermolysis

The purpose of this study was to find optimum treatment conditions for selective photothermolysis by evaluating internal–external heat distributions according to different cooling methods. The 1,064-nm Nd:YAG laser was transmitted into a skin-mimicking phantom with different cooling conditions, and its minimum temperatures and sub-zero times were measured. The cooling methods were classified into a total of eight conditions composed of five cryogen spray cooling conditions and three air cooling conditions. Based on the experimental results, condition 2 was selected as the optimum cooling condition for selective photothermolysis obtained from the cryogen spray cooling method.