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本文根据年龄理论,考虑下列问题:二介质由球面r=a分开,球面外的介质一直延伸到无限,球面内的介质中在r=R处放有壳形单能快中子源;要求二介质中由此引起的中子慢化密度的空间分布。求解时应用了拉氏变换的方法。求出了适用於(τ1)1/2≤α情形的展开式,这里τ1是中子在球面内介质中的年龄、物理上出现的实际情形多半满足(τ1)1/2?α的条件,这时展开式收敛很快。对於二介质是重水和石墨的一个实例;我们算出了热能处中子慢化密度的数值结果(假定快中子源的能量为2兆电子伏),并和用通常二群近似方法求得的结果进行了比较。 相似文献
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本文分析了中子平面晶体谱仪的分辨宽度,给出它的近似表示式为:△θ=((α12α22+α12β2+α22β2)/(α12+4β2+α22))1/2;同时对几种常见情况也作了简略的讨论。为了确定计算参量△θ,又给出了晶体摇动曲线半宽度的近似表示式为:△γ=1/2(α12+4β2+α22)1/2。以上两式中的α1,α2是第一、第二准直器的散开角;β是晶体单色器嵌镶结构(mosaic)分布半宽度。最后,依据上述结果,计算了我们仪器的分辨宽度,另外从该仪器测量的中子共振截面估计了它的分辨宽度,并作了比较。 相似文献
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本文报告了在En=13.6—14.8MeV中子能区用活化法以27Al(n,α)24Na截面为中子注量标准测得的62Ni(n,α)59Fe的反应截面.在En为 13.64,13.79,14.00,14.05,14.33,14.60和14.80MeV处的截面分别为17.4±1.1,19.5±1.5,21.9±1.9,22.4±1.6,25.4±1.4,26.1±1.1和26.0±1.1mb.在文章中还列举了所能收集到的一些作者的数据以作比较.中子能量是用铌锆截面比法测定的. 相似文献
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本文讨论了在三层平板介质波导中TM0模的传播问题.三层介质的芯区是一层各向异性的Kerr型介质,上下两层则是线性介质.本文将利用Ex2 >> Ex2这一性质,求解非线性方程组,给出零级近似和1级近似的解析解. 相似文献
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本文报告了En=13.6—14.8MeV中子能区用活化法以27Al(n,α)24Na截面为中子注量标准得的60Ni(n,p)60Co的反应截面.在En为 13.64,13.79,14.03,14.33,14.60,14.80MeV处的截面分别为184.4±12.2,178.8±10.5,171.4±10.3,161.9±9.6,157.0±9.3,147.5±8.9mb.在文章中还列举了所能收集的一些作者的数据以作比较.中子能量是用铌锆截面比法则定的. 相似文献
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Michael F. Modest Jun Yang 《Journal of Quantitative Spectroscopy & Radiative Transfer》2008,109(9):1641-1666
The inherent complexity of the radiative transfer equation makes the exact treatment of radiative heat transfer impossible even for idealized situations and simple boundary conditions. Therefore, a wide variety of efficient solution methods have been developed for the RTE. Among these solution methods the spherical harmonics method, the moment method, and the discrete ordinates method provide means to obtain higher-order approximate solutions to the equation of radiative transfer. Although the assembly of the governing equations for the spherical harmonics method requires tedious algebra, their final form promises great accuracy for any given order, since it is a spectral method (rather than finite difference/finite volume in the case of discrete ordinates). In this study, a new methodology outlined in a previous paper on the spherical harmonics method (PN) is further developed. The new methodology employs successive elimination of spherical harmonic tensors, thus reducing the number of first-order partial differential equations needed to be solved simultaneously by previous PN approximations (=(N+1)2). The result is a relatively small set (=N(N+1)/2) of second-order, elliptic partial differential equations, which can be solved with standard PDE solution packages. General boundary conditions and supplementary conditions using rotation of spherical harmonics in terms of local coordinates are formulated for the general PN approximation for arbitrary three-dimensional geometries. Accuracy of the PN approximation can be further improved by applying the “modified differential approximation” approach first developed for the P1-approximation. Numerical computations are carried out with the P3 approximation for several new two-dimensional problems with emitting, absorbing, and scattering media. Results are compared to Monte Carlo solutions and discrete ordinates simulations and a discussion of ray effects and false scattering is provided. 相似文献
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Mahesh Ravishankar Maathangi Sankar 《Journal of Quantitative Spectroscopy & Radiative Transfer》2010,111(14):2052-7001
The first-order spherical harmonics method (or P1 approximation) has found prolific usage for approximate solution of the radiative transfer equation (RTE) in participating media. However, the accuracy of the P1 approximation deteriorates as the optical thickness of the medium is decreased. The modified differential approximation (MDA) was originally proposed to remove the shortcomings of the P1 approximation in optically thin situations. This article presents algorithms to apply the MDA to arbitrary geometry—in particular, geometry with obstructions, and inhomogeneous media. The wall-emitted component of the intensity was computed using a combined view-factor and ray-tracing approach. The Helmholtz equation, arising out of the medium-emitted component, was solved using an unstructured finite-volume procedure. The general procedure was validated for both two-dimensional (2D) and three-dimensional (3D) geometries against benchmark Monte Carlo results. The accuracy of MDA was found to be superior to the P1 approximation for all optical thicknesses. Its accuracy, when compared with the discrete ordinates method (both S6 and S8), was found to be clearly superior in optically thin situations, but problem dependent in optically intermediate and thick situations. For 3D geometries, calculation and storage of the view-factor matrix was found to be a major shortcoming of the MDA. In addition, for inhomogeneous media, calculation of optical distances requires a ray-tracing procedure, which was found to be a bottleneck from a computational efficiency standpoint. Several strategies to reduce both memory and computational time are discussed and demonstrated. 相似文献
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M.P. Mengüç R. Viskanta 《Journal of Quantitative Spectroscopy & Radiative Transfer》1983,29(5):381-394
We examine critically the accuracy of the two-flux, spherical harmonics and discrete ordinates methods for predicting radiative transfer in a planar, highly-forward scattering and absorbing medium. Numerical results for the radiative fluxes show that the two-flux and P3-approximations yield accurate results compared to solutions based on the FN-method. Indeed, these approximate methods are relatively simple and have potential for generalization to predict radiative transfer in multidimensional systems, as long as an appropriate simplification of the phase function is utilized. 相似文献
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Spherical harmonics are often used to solve multi-scatter transport problems. For a collimated incident beam, we describe a technique similar to the familiar PN approximation except that we manage the infinite set of coupled equations in a novel way that permits the use of hundreds of harmonics to represent very pointed angular distributions. We split some equations into two approximate ones that depend on the angle of incidence. For plane slab geometry, the harmonics of low degree are solved in a coordinate system aligned to the boundary while the high harmonics use coordinates pointed at the source. We illustrate the technique with an extreme example: a scattering function having an integrable singularity in the forward direction. We give a time-dependent example along with several time-independent ones. 相似文献
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Effective response in nonlinear spherical coated composites under external AC and DC electric field
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By using the perturbation method, effective nonlinear direct current (DC) and alternating current (AC) responses of nonlinear composites with spherical coated inclusions randomly embedded in a host medium are studied under the action of external electric field Ea =E0 +E1 sin ωt+E3 sin 3ωt with different amplitudes and frequencies. The local potentials of composites at all harmonics are given in the inclusion particles and the host regions. All effective nonlinear responses to composites and the relationship between the effective nonlinear responses at all harmonics are also deduced for the spherical coated inclusions in a dilute limit. 相似文献
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We present a novel application of filters to the spherical harmonics (PN) expansion for radiative transfer problems in the high-energy-density regime. The filter we use is based on non-oscillatory spherical splines and a filter strength chosen to (i) preserve the equilibrium diffusion limit and (ii) vanish as the expansion order tends to infinity. Our implementation is based on modified equations that are derived by applying the filter after every time step in a simple first-order time integration scheme. The method is readily applied to existing codes that solve the PN equations. Numerical results demonstrate that the solution to the filtered PN equations are (i) more robust and less oscillatory than standard PN solutions and (ii) more accurate than discrete ordinates solutions of comparable order. In particular, the filtered P7 solution demonstrates comparable accuracy to an implicit Monte Carlo solution for a benchmark hohlraum problem in 2D Cartesian geometry. 相似文献
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Jonathan Dimock 《Communications in Mathematical Physics》1974,35(4):347-356
In theP(φ)2 model it is proved that the perturbation series for the infinite volume Schwinger functionsS(λ) are asymptotic in the limit as the coupling constant λ goes to zero. We also give conditions which imply smoothness ofS(λ) at arbitrary λ. 相似文献
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M.P. Mengüç R. Viskanta 《Journal of Quantitative Spectroscopy & Radiative Transfer》1985,33(6):533-549
Radiative transfer in a three-dimensional rectangular enclosure containing radiatively participating gases and particles is studied using the first- and third-order spherical harmonics approximations. Inhomogeneities in the radiative properties of the medium, as well as in the radiation characteristics of the boundaries, are allowed for. The scattering phase function is represented by the delta-Eddington approximation, and it is assumed to be a function of the location in order to account for density variation of the particles in the medium. Numerical solutions of the model equations are obtained using a finite difference scheme. For the purpose of validating the P3-approximation, the results are compared with those based on Hottel's zonal method. 相似文献