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Stability Analysis of the Quasidiffusion Method on Periodic Heterogeneous 1D Transport Problems 周期非均质一维输运问题准扩散方法的稳定性分析
Pub Date : 2009-11-24 DOI: 10.1080/00411450903372084
A. Constantinescu, Dmitriy Anistratov
We study the convergence of the quasidiffusion (QD) method on one-dimensional spatially periodic heterogeneous problems. The QD method is a nonlinear projection-iterative method. A Fourier analysis of the linearized QD equations is performed. The convergence rates of the QD method in the vicinity of the solution are obtained. We also analyze the Second Moment (SM) method, which can be interpreted as a linear version of the QD method. The presented analysis gives a new insight on the convergence behavior of the QD method in a discretized form and reveals the differences in the convergence of the QD and SM methods. Numerical results are presented to confirm theoretical predictions.
研究了一维空间周期非均质问题的准扩散方法的收敛性。QD法是一种非线性投影迭代法。对线性化QD方程进行了傅里叶分析。得到了QD方法在解附近的收敛速率。我们还分析了二阶矩(SM)方法,它可以被解释为QD方法的线性版本。本文的分析对离散形式下QD方法的收敛性有了新的认识,揭示了QD方法和SM方法收敛性的不同。数值结果证实了理论预测。
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引用次数: 1
Nonlinear Envelope Equation and Nonlinear Landau Damping Rate for a Driven Electron Plasma Wave 驱动电子等离子体波的非线性包络方程和非线性朗道阻尼率
Pub Date : 2009-10-28 DOI: 10.1080/00411450.2011.604568
D. B'enisti, O. Morice, L. Gremillet, D. Strozzi
In this article, we provide a theoretical description and calculate the nonlinear frequency shift, group velocity, and collionless damping rate, ν, of a driven electron plasma wave (EPW). All these quantities, whose physical content will be discussed, are identified as terms of an envelope equation allowing one to predict how efficiently an EPW may be externally driven. This envelope equation is derived directly from Gauss’ law and from the investigation of the nonlinear electron motion, provided that the time and space rates of variation of the EPW amplitude, , are small compared to the plasma frequency or the inverse of the Debye length. ν arises within the EPW envelope equation as a more complicated operator than a plain damping rate and may only be viewed as such because [] remains nearly constant before abruptly dropping to zero. We provide a practical analytic formula for ν and show, without resorting to complex contour deformation, that in the limit 0, ν is nothing but the Landau damping rate. We then term ν the “nonlinear Landau damping rate” of the driven plasma wave. As for the nonlinear frequency shift of the driven EPW, it is also derived theoretically and found to assume values significantly different from previously published ones, which were obtained by assuming that the wave was freely propagating. Moreover, we find no limitation in , being the plasma wavenumber and the Debye length, for a solution to the dispertion relation to exist, and want to stress here the importance of specifying how an EPW is generated to discuss its properties. Our theoretical predictions are in excellent agreement with results inferred from Vlasov simulations of stimulated Raman scattering (SRS), and an application of our theory to the study of SRS is presented.
本文给出了一个理论描述,并计算了驱动电子等离子体波(EPW)的非线性频移、群速度和无柱阻尼率ν。所有这些物理量,其物理内容将被讨论,被确定为包络方程的项,允许人们预测外部驱动EPW的效率。这个包络方程是直接从高斯定律和对非线性电子运动的研究中推导出来的,前提是EPW振幅的时间和空间变化率与等离子体频率或德拜长度的倒数相比都很小。ν出现在EPW包络方程中,是一个比普通阻尼率更复杂的算符,可能只是因为[]在突然降为零之前几乎保持不变。我们提供了一个实用的解析公式,并证明在极限0下,ν只是朗道阻尼率,而不需要复杂的轮廓变形。然后我们将ν命名为驱动等离子体波的“非线性朗道阻尼率”。对于驱动EPW的非线性频移,也进行了理论推导,发现其假设值与先前发表的假设值有很大不同,这些假设值是在波自由传播的情况下得到的。此外,我们发现,当等离子体波数和德拜长度存在时,色散关系的解没有限制,并且想在这里强调说明如何产生EPW以讨论其性质的重要性。我们的理论预测与受激拉曼散射(SRS)的Vlasov模拟结果非常一致,并提出了我们的理论在SRS研究中的应用。
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引用次数: 5
Radial Orbit Instability: Review and Perspectives 径向轨道不稳定性:回顾与展望
Pub Date : 2009-10-27 DOI: 10.1080/00411450.2011.654750
L. Marechal, Julien Perez
This article presents elements about the radial orbit instability, which occurs in spherical self-gravitating systems with a strong anisotropy in the radial velocity direction. It contains an overview on the history of radial orbit instability. We also present the symplectic method we use to explore stability of equilibrium states directly related to the dissipation induced instability mechanism well known in theoretical mechanics and plasma physics.
本文给出了在径向速度方向上具有较强各向异性的球形自重力系统的径向轨道不稳定性的基本原理。它概述了径向轨道不稳定性的历史。我们还提出了我们用来探索与理论力学和等离子体物理学中众所周知的耗散诱导不稳定机制直接相关的平衡态稳定性的辛方法。
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引用次数: 10
Modeling Error in L1 for a Hierarchy of 1-D Discrete Velocity Models 一维离散速度模型层次的L1建模误差
Pub Date : 2009-10-20 DOI: 10.1080/00411450903238665
K. C. Assi, M. Laforest
We consider the spatial difference in L 1 between solutions to two different discrete velocity models in one space dimension. We assume that the second (fine) model is obtained by adding new velocities to the first (coarse) model, although the collision operators can be completely different. The 1-D discrete velocity models studied here include projections of n-D models, as described by Beale. This work adapts the nonlinear and decreasing interaction functional of Ha and Tzavaras for discrete velocity models in 1-D in order to measure the distance in L 1 . The resulting functional increases by a term proportional to the residual of the modeling error for the coarse model. The modeling error can therefore be computed a posteriori and can be used to determine which discrete velocity model within a hierarchy satisfies a prescribed accuracy.
我们考虑在一维空间中两个不同离散速度模型的解在L 1中的空间差异。我们假设第二个(精细)模型是通过向第一个(粗糙)模型添加新的速度而获得的,尽管碰撞算子可能完全不同。这里研究的一维离散速度模型包括Beale所描述的n-D模型的投影。本文将Ha和Tzavaras的非线性递减相互作用泛函用于1- d离散速度模型,以测量L - 1中的距离。所得到的函数增加一项,与粗模型的建模误差残差成正比。因此,建模误差可以后验计算,并可用于确定层次结构中哪个离散速度模型满足规定的精度。
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引用次数: 2
Some Benchmark Results in Spherical Media Radiative Transfer Problems 球面介质辐射传递问题的一些基准结果
Pub Date : 2009-10-20 DOI: 10.1080/00411450903238707
A. Yilmazer, C. Kocar
This study is aimed at demonstrating the numerical convergency of spectral polynomial approximations to the radiative transfer equation in spherical media. To this end, T N method is employed as a representative of classical polynomial approximations to the corresponding pseudo-slab problem of spherical media radiative transfer equation. The method is used to calculate the albedo and density for isotropic scattering in a homogeneous spherical medium. Spherical harmonics or P N method is also applied to the same problem for comparison purposes. Benchmark results of both methods for an absorbing and scattering spherical medium transfer problem are reported. The results contribute remarkable improvements to the previously reported data in the literature. More importantly, on contrary to some literature works, numerical divergence of spherical harmonics method in spherical media transfer problems is illustrated to be unsound provided that arbitrary precision arithmetic is available when considering higher order approximations.
本研究旨在证明谱多项式近似在球形介质中辐射传递方程的数值收敛性。为此,采用tn法作为经典多项式近似的代表,求解球形介质辐射传递方程的拟板问题。用该方法计算了均匀球面介质中各向同性散射的反照率和密度。为了便于比较,球面谐波法或pn法也适用于同一问题。本文报道了两种方法对吸收散射球形介质传输问题的基准结果。该结果对先前文献中报道的数据作出了显著的改进。更重要的是,与一些文献相反,在考虑高阶近似时,在任意精度算法可用的情况下,说明球面介质传递问题中球谐波方法的数值散度是不完善的。
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引用次数: 3
New Trace Theorems for Neutronic Function Spaces 中子函数空间的新迹定理
Pub Date : 2009-09-16 DOI: 10.1080/00411450903196228
M. Boulanouar
This article deals with new trace theorems for neutronic function spaces.
本文讨论了中子函数空间的新迹定理。
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引用次数: 11
W N Approximations Of Neutron Transport Equation 中子输运方程的W - N近似
Pub Date : 2009-09-16 DOI: 10.1080/00411450903192938
L. Bourhrara
In this article, we propose new approximations of the neutron transport equation based on the transport variational formulations presented in Bourhrara (2004). These approximations are solutions of associated variational problems. We give an error estimate between the angular flux, exact solution of the transport equation, and the approximate solutions. We also derive variational formulations for even- and odd- parity fluxes as approximations of the neutron transport equation.
在本文中,我们基于Bourhrara(2004)提出的输运变分公式提出了中子输运方程的新近似。这些近似是相关变分问题的解。给出了输运方程的角通量、精确解和近似解之间的误差估计。我们也推导出偶宇称和奇宇称通量的变分公式作为中子输运方程的近似。
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引用次数: 1
Landau and Non-Landau Linear Damping: Physics of the Dissipation 朗道和非朗道线性阻尼:耗散的物理学
Pub Date : 2009-09-11 DOI: 10.1080/00411450.2011.651055
G. Belmont, T. Chust, F. Mottez, S. Hess
The linear Landau effect is revisited by the means of numerical simulations and analytical calculations. The existence of non-Landau solutions to the Vlasov-Poisson system is emphasized and the consistency of these solutions with respect to the arguments based on energy is investigated. The present article briefly summarizes the content of two articles already published on the subject and introduces a discussion based on the exchanges that occurred at Marseille during the Vlasovia meeting.
通过数值模拟和解析计算的方法,重新探讨了线性朗道效应。强调了Vlasov-Poisson系统的非朗道解的存在性,并研究了这些解与基于能量的参数的一致性。本文简要总结了已发表的两篇相关文章的内容,并介绍了在马赛举行的Vlasovia会议期间的讨论。
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引用次数: 10
A Fast-Forward Solver of Radiative Transfer Equation 辐射传递方程的快进求解器
Pub Date : 2009-09-04 DOI: 10.1080/00411450903187722
Haoyang Gao, Hongkai Zhao
In this article, we develop an efficient forward solver for steady-state or frequency-domain radiative transfer equation on 2D and 3D structured and unstructured meshes with vacuum boundary condition or reflection boundary condition. Although we emphasize applications in optical imaging, our method may be applied to more general radiative transfer equations, for example, other types of scattering function. Efficiency and accuracy of our algorithm is demonstrated by comparison with both analytical solutions and Monte Carlo solutions and with various numerical tests in optical imaging.
在本文中,我们开发了一种有效的二维和三维结构和非结构网格上具有真空边界条件或反射边界条件的稳态或频域辐射传递方程的正演求解器。虽然我们强调在光学成像中的应用,但我们的方法可以应用于更一般的辐射传递方程,例如,其他类型的散射函数。通过与解析解和蒙特卡罗解的比较以及光学成像中的各种数值测试,证明了该算法的有效性和准确性。
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引用次数: 111
Nonlinear Landau Damping 非线性朗道阻尼
Pub Date : 2009-08-20 DOI: 10.1080/00411450903081313
C. Lancellotti, J. Dorning
In this article, we report the mathematical details of a systematic analysis of the nonlinear Landau damping of longitudinal electrostatic waves propagating in a collisionless plasma. Many of the main results have been reported previously; unfortunately, major parts of the essential mathematical developments had to be omitted for various reasons, making it almost impossible for even the most well-prepared reader to follow the analysis. Sufficient details are provided here to remedy this situation. Some important results that have not been reported previously are also are included here. Most notably among these is the distinction between strong branches and weak branches of nonzero time-asymptotic electric field amplitudes that bifurcate from the zero-amplitude solution for the time-asymptotic electric field, and the results on the weak branches that had to be omitted in the earlier report of this research. Based on the decomposition of the electric field E into a transient part T and a time-asymptotic part A, we show that A is given by a finite superposition of wave modes, whose frequencies obey a Vlasov dispersion relation and whose amplitudes satisfy a set of nonlinear algebraic equations. These time-asymptotic mode amplitudes are calculated explicitly based on approximate solutions for the particle distribution functions obtained by linearizing only the term that contains T in the Vlasov equation for each particle species and then integrating the resulting equation along the nonlinear characteristics associated with A, which are obtained via Hamiltonian perturbation theory. For “linearly stable” initial Vlasov equilibria, we obtain a critical initial amplitude, separating the initial conditions that Landau damp to zero from those that lead to nonzero multiple-traveling-wave time-asymptotic states via nonlinear particle trapping. These theoretical results explain why in some cases experiments and large-scale numerical simulations have resulted in zero-field final states; whereas in other cases they have yielded nonzero multiple-traveling-wave final states because the theoretical results establish the existence of a “threshold” in the initial electric field below which the field damps to zero and above which it evolves to a finite-amplitude multiple-traveling-wave final state.
本文报道了在无碰撞等离子体中传播的纵向静电波的非线性朗道阻尼的系统分析的数学细节。许多主要结果以前已经报道过;不幸的是,由于各种原因,基本数学发展的主要部分不得不被省略,这使得即使是准备最充分的读者也几乎不可能理解分析。这里提供了足够的细节来纠正这种情况。一些以前没有报道过的重要结果也包括在这里。其中最值得注意的是,从时间渐近电场的零振幅解分叉的非零时间渐近电场振幅的强分支和弱分支的区分,以及在本研究的早期报告中不得不忽略的关于弱分支的结果。在将电场E分解为瞬态部分T和时间渐近部分a的基础上,我们证明了a是由频率服从Vlasov色散关系且振幅满足一组非线性代数方程的波模的有限叠加给出的。这些时间渐近模态振幅是根据粒子分布函数的近似解来显式计算的,这些近似解是通过对每个粒子种的Vlasov方程中仅包含T的项进行线性化,然后沿着与A相关的非线性特征对结果方程进行积分,这些非线性特征是通过哈密顿摄动理论得到的。对于“线性稳定”初始Vlasov平衡,我们获得了一个临界初始振幅,将朗道阻尼为零的初始条件与那些通过非线性粒子捕获导致非零多行波时间渐近状态的初始条件分开。这些理论结果解释了为什么在某些情况下,实验和大规模数值模拟会导致零场最终状态;然而,在其他情况下,他们已经产生了非零的多行波最终状态,因为理论结果确定了初始电场中存在一个“阈值”,低于该阈值,场衰减为零,高于该阈值,它演变为有限振幅的多行波最终状态。
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引用次数: 10
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Transport Theory and Statistical Physics
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