用高精度有限差分法模拟烧蚀瑞利-泰勒不稳定性

求解烧蚀面附近流场的定常解,并以此作为基本流实现用高精度的WENO格式对烧蚀瑞利-泰勒不稳定性的数值模拟.线性增长率与Lindl公式以及线性稳定性分析给出的结果相符合,证明该数值模拟方法的准确性与精度,该方法还具有较好的界面变形捕捉能力.     

神光Ⅱ装置上间接驱动烧蚀瑞利-泰勒不稳定性实验分析

在神光Ⅱ激光装置上开展了一系列辐射烧蚀Rayleigh-Taylor(RT)不稳定性实验。平面靶烧蚀加速飞行轨迹实验结果与LARED-S模拟结果的比较表明腔壁辐射源能流明显小于激光注入孔的辐射能流,且辐射源的非平衡Planckian谱对靶的飞行轨迹和扰动增长有重要影响。实验分别观测到初始小扰动幅度烧蚀RT明显的增长和初始大扰动幅度尖钉变窄和气泡变宽的清晰物理图像。通过提高空间分辨率,实验获得了二次和三次谐波的增长数据,模拟结果与实验结果相符合。神光Ⅱ激光装置上开展的流体不稳定性实验考核了LARED-S程序的一维和二维计算。     

神光Ⅱ装置上间接驱动烧蚀瑞利-泰勒不稳定性实验分析

在神光Ⅱ激光装置上开展了一系列辐射烧蚀Rayleigh-Taylor(RT)不稳定性实验。平面靶烧蚀加速飞行轨迹实验结果与LARED-S模拟结果的比较表明腔壁辐射源能流明显小于激光注入孔的辐射能流, 且辐射源的非平衡Planckian谱对靶的飞行轨迹和扰动增长有重要影响。实验分别观测到初始小扰动幅度烧蚀RT 明显的增长和初始大扰动幅度尖钉变窄和气泡变宽的清晰物理图像。 通过提高空间分辨率, 实验获得了二次和三次谐波的增长数据, 模拟结果与实验结果相符合。 神光Ⅱ激光装置上开展的流体不稳定性实验考核了LARED-S程序的一维和二维计算。     

激光烧蚀瑞利－泰勒不稳定性模拟

给出了激光烧蚀流体不稳定性计算程序EUL2D的物理方程,介绍了计算中使用的活动网格和一些技术问题处理。EUL2D程序的计算结果与Takabe公式、FAST2D程序和LASNEX程序的结果较好符合。数值计算日本大阪大学激光烧蚀瑞利－泰勒不稳定性实验,再现了实验结果。发现了横向电子热传导烧蚀在长波长扰动的非线性瑞利－泰勒不稳定性演变中起重要作用。     

激光烧蚀瑞利－泰勒不稳定性模拟

 给出了激光烧蚀流体不稳定性计算程序EUL2D的物理方程,介绍了计算中使用的活动网格和一些技术问题处理。EUL2D程序的计算结果与Takabe公式、FAST2D程序和LASNEX程序的结果较好符合。数值计算日本大阪大学激光烧蚀瑞利－泰勒不稳定性实验,再现了实验结果。发现了横向电子热传导烧蚀在长波长扰动的非线性瑞利－泰勒不稳定性演变中起重要作用。     

高温烧蚀初始印记及其瑞利-泰勒不稳定性发展的研究

直接驱动惯性约束聚变中,高温烧蚀初始印记在压缩过程的不稳定性发展中起着重要作用.利用X射线针孔辅助点投影成像法,研究了不同波形激光脉冲驱动下CH平面靶及其瑞利-泰勒不稳定性发展的情况.结果表明,在相同驱动激光能量作用下,初始阶段激光强度越低,上升越缓慢,高温烧蚀初始印记引起的密度调制幅度越大.提高预脉冲强度能显著抑制高温烧蚀初始印记效应. 关键词： 高温烧蚀初始印记 激光脉冲形状 瑞利-泰勒不稳定性 针孔辅助点投影     

瑞利-泰勒不稳定性中尺度效应的数值模拟研究

 瑞利-泰勒不稳定性是一种由于密度梯度引起的界面不稳定性，在惯性约束聚变中具有重要的意义。利用被动标量输运模型对包含不同尺度初始扰动的界面演化过程进行数值模拟。计算结果表明界面的初始形状对不稳定性的发展具有很大的影响，狭长型扰动比正方型扰动发展慢。另外，不同尺度扰动的相互作用一般会减小沿界面发展方向运动的动能，使能量更多地用于平行于界面方向的运动。     

二维不可压流体瑞利-泰勒不稳定性的非线性阈值公式

分析了二维情况下平面几何、柱几何和球几何中瑞利-泰勒不稳定性发生非线性偏离的阈值问题，给出了三种几何中密度扰动振幅的定义，以及与界面扰动振幅的关系.由此得到了三种几何中密度扰动的非线性阈值公式，用高精度流体程序对三种几何中的不稳定性进行了数值模拟，验证了得到的非线性阈值公式. 关键词： 瑞利-泰勒不稳定性 非线性阈值 密度振幅     

磁瑞利-泰勒不稳定性非线性演化数值模拟

基于理想磁流体力学模型,采用5阶WENO有限差分格式结合磁场伪散度清除投影算法,发展二维数值模拟程序,利用线性理论对程序进行检验,在此基础上研究磁瑞利-泰勒(MRT)不稳定性非线性演化物理过程和发展规律.结果表明:垂直于加速度方向磁场在线性和非线性阶段对MRT扰动发展都有较强的制稳作用,而平行于加速度方向磁场在线性阶段...     

金属丝阵列Z箍缩装置中的瑞利-泰勒不稳定性

磁流体瑞利－泰勒（RT）不稳定性是Z箍缩装置研究中的重要理论课题。引入一个金属丝阵列型Z箍缩的雪耙模型,对RT不稳定性的扰动幅值进行了初步的定量分析,提出了用剪切轴向流来抑制和减弱Z箍缩中的RT不稳定性,并探索了其它可用来抑制这种超快过程产生的不稳定性的方法。     

Nonlinear theory of the ablative Rayleigh-Taylor instability

A fully nonlinear sharp-boundary model of the ablative Rayleigh-Taylor instability is derived and closed in a similar way to the self-consistent closure of the linear theory. It contains the stabilizing effect of ablation and accurately reproduces the results of 2D DRACO simulations. The single-mode saturation amplitude, bubble and spike evolutions in the nonlinear regimes, and the seeding of long-wavelength modes via mode coupling are determined and compared with the classical theory without ablation. Nonlinear stability above the linear cutoff is also predicted.     

Bubble acceleration in the ablative Rayleigh-Taylor instability

The highly nonlinear evolution of the single-mode Rayleigh-Taylor instability (RTI) at the ablation front of an accelerated target is investigated in the parameter range typical of inertial confinement fusion implosions. A new phase of the nonlinear bubble evolution is discovered. After the linear growth phase and a short constant-velocity phase, it is found that the bubble is accelerated to velocities well above the classical value. This acceleration is driven by the vorticity accumulation inside the bubble resulting from the mass ablation and vorticity convection off the ablation front. While the ablative growth rates are slower than their classical values in the linear regime, the ablative RTI grows faster than the classical RTI in the nonlinear regime for deuterium and tritium ablators.     

Weakly nonlinear theory for the ablative Rayleigh-Taylor instability

A weakly nonlinear model is proposed for the Rayleigh-Taylor instability in the presence of ablation and thermal transport. The second harmonic generation efficiency of a single-mode disturbance is computed, as well as the nonlinear correction to the exponential growth of the fundamental modulation. Mode coupling in the spectrum of a multimode disturbance is thoroughly analyzed. The ablative stabilization can be clearly discussed because the derived formulas for the evanescent ablation rate are in agreement with previously known results for incompressible, inviscid, irrotational, and immiscible fluids [S. W. Haan, Phys. Fluids B 3, 2349 (1991)]; M. Berning and A. M. Rubenchik, Phys. Fluids 10, 1564 (1998)]].     

Stabilizing effect of anisotropic thermal diffusion on the ablative Rayleigh-Taylor instability

Linear theory of the ablative Rayleigh-Taylor instability in anisotropic diffusive materials is presented. This analysis indicates that enhancing diffusion in a plane transverse to the mean longitudinal flow can strongly reduce the growth of the instability. In the context of inertial confinement fusion, it is shown that anisotropic diffusion can be achieved using a laminated ablator made of successive layers of different diffusive properties. Numerical simulations confirm the theoretical predictions and indeed exhibit a significant stabilization of the ablation front for laminated ablators.     

烧蚀RT不稳定性X射线分幅诊断研究进展

在神光II装置上,利用高动态范围高性能X射线分幅相机开展了辐射驱动烧蚀RT不稳定性面背光实验研究.在神光II 8路2ns辐射源和第九路Mo背光条件下,利用二维时空照相获得了周期20 μupm、初始扰动1 μupm烧蚀RT样品清晰的增长过程,并通过掺Br比例1.1%样品观测到RT非线性增长的结果.实验为惯性约束聚变(inertial confinement fusion,ICF)RT不稳定性定量表征和数值模拟奠定了良好的基础.     

Comprehensive diagnosis of growth rates of the ablative Rayleigh-Taylor instability

The growth rate of the ablative Rayleigh-Taylor instability is approximated by gamma = square root[kg/(1 + kL)] - beta km/rho(a), where k is the perturbation wave number, g the gravity, L the density scale length, m the mass ablation rate, and rho(a) the peak target density. The coefficient beta was evaluated for the first time by measuring all quantities of this formula except for L, which was taken from the simulation. Although the experimental value of beta = 1.2+/-0.7 at short perturbation wavelengths is in reasonably good agreement with the theoretical prediction of beta = 1.7, it is found to be larger than the prediction at long wavelengths.     

掺杂对CH样品Rayleigh-Taylor不稳定性增长的影响

在神光II激光装置上进行了辐射驱动不同掺杂样品的单模Rayleigh-Taylor(RT)不稳定性实验.结果显示:与纯碳氢(CH)样品相比,掺Br的CH样品的扰动更早、更快地进入非线性区,产生二次谐波,并且掺Br比例越高,CH样品扰动进入非线性区的时间越早,相同时刻扰动的二次谐波的幅度越高.这是因为密度梯度效应抑制了二次谐波的产生,掺Br比例越高,密度梯度标长越小;同时密度梯度效应还抑制三次谐波对基模增长的负反馈,造成基模具有更大的线性增长,导致线性饱和幅值大于经典值0.1λ.     

Ablation effects on weakly nonlinear Rayleigh-Taylor instability with a finite bandwidth

A weakly nonlinear but numerically tractable model (to third order in amplitude and including bandwidth effects) has been developed for the ablative Rayleigh-Taylor (RT) instability. Model results clearly show growth reduction from linear ablative RT values and even amplitude saturation in some realistic cases. For excitation of a band of wave numbers near the cutoff for growth, the behavior is dominated by the mode with the largest linear growth rate, and not by the mode with the largest initial amplitude. This type of model is likely to be important for the future assessment of the RT effects on specific target designs of the inertial confinement fusion.