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 共查询到17条相似文献,搜索用时 140 毫秒
1.
尤云祥  缪国平  刘应中 《物理学报》2001,50(6):1103-1109
提出了用点声源散射场的近场信息来可视化多个三维障碍物的一种简单快速算法,它是通过利用一个线性方程组的解的三维等值线图来实现这种可视化的.这个算法的一个特别吸引人的性质是,它避开了迭代技术的应用,而且不需要关于障碍物的任何几何和物理的先验信息.此外,它只需要散射场在测量表面的某个有限范围中若干个观测点处的近场测量信息,就能得到障碍物的一个很理想的可视化.数值算例保证了这个可视化算法是有效和实用的 关键词: 声散射 反问题 物形反演  相似文献   

2.
研究用声传播远场分布信息成像海洋波导环境中三维散射目标的反问题,提出一种指示器样本成像方法,在不需要预先知道散射目标的任何声学和几何特性的情况下,可以快速得到其位置、形状等几何信息的一个理想的像.数值试验表明,该方法对成像海洋波导中三维散射目标是有效的,即使在有限孔径测量方式和具有噪声测量数据时,也能够得到散射目标的一个理想成像,表明海洋波导边界的多重反射效应对成像效果具有一定的正面影响.  相似文献   

3.
研究了从声散射场的远场分布的信息来再现半空间三维目标几何特征信息的反问题,提出了求解这种非线性不适定问题的一种简单快速算法。该方法的一个特别的性质是只需要通过一个不适定的线性方程组求解,即可简单快速地得到半空间中三维目标几何特征信息的一个清晰的像,而且目标的个数和边界条件的类型等几何与物理的先验信息在本算法中都是不需要的。数值算例保证了本算法的有效性。  相似文献   

4.
阻抗障碍物声散射的反问题   总被引:1,自引:0,他引:1       下载免费PDF全文
尤云祥  缪国平 《物理学报》2002,51(2):270-278
研究了从声散射场的远场分布的信息来再现声阻抗障碍物形状的反问题,建立了求解这类反问题的一种非线性最优化模型,并提出了数值实现该非线性最优化模型的一种两步调整迭代算法.两步过程的应用使在确定未知障碍物形状的非线性最优化步中未知函数的个数达到了最少,而在调整迭代过程中,通过利用前一迭代步所得重构信息,使重构精度得到了相当大的改进.所建立的反演算法的一个特别吸引人的性质是,只需要远场分布的一个Fourier系数即可对未知声阻抗障碍物作几何物形的设别.对大量具有各种几何形状的二维障碍物的数值算例保证了本算法是实用和有效的.  相似文献   

5.
阻抗障碍物声散射的反问题   总被引:4,自引:2,他引:2       下载免费PDF全文
尤云祥  缪国平 《物理学报》2002,51(2):270-278
研究了从声散射场的远场分布的信息来再现声阻抗障碍物形状的反问题,建立了求解这类反问题的一种非线性最优化模型,并提出了数值实现该非线性最优化模型的一种两步调整迭代算法.两步过程的应用使在确定未知障碍物形状的非线性最优化步中未知函数的个数达到了最少,而在调整迭代过程中,通过利用前一迭代步所得重构信息,使重构精度得到了相当大的改进.所建立的反演算法的一个特别吸引人的性质是,只需要远场分布的一个Fourier系数即可对未知声阻抗障碍物作几何物形的设别.对大量具有各种几何形状的二维障碍物的数值算例保证了本算法是实用和有效的.  相似文献   

6.
三维障碍物形状反演问题的一种简单算法   总被引:2,自引:0,他引:2  
研究了从声散射场的远场分布的信息,再现三维物体形状的反问题.基于将在有限个测量方向上的远场数据作加权合成的思想,提出了求解这类反问题的一种简单快速算法.在这个算法中,既不需预先知道散射体的边界类型,也不需预先知道散射体个数的信息.对有限孔径远场数据的数值算例表明了这一方法是实用和有效的.  相似文献   

7.
在电磁场积分方程方法框架下,应用等效原理求解了半空间背景下目标的电磁散射问题,可针对目标仅处于半空间界面单侧及目标跨越半空间界面处于半空间两侧的几何相对位置。与传统的半空间格林函数计算方法不同的是,这一方法使用的是各自介质的自由空间格林函数,因此可以回避索墨菲积分并且可以很方便与快速算法(如多层快速多级子)相结合,并对求解临近半空间界面的目标获得较好的收敛性。在等效原理方法中需要用有限的界面等效无限大半空间界面,因此采用了锥形入射波以降低开放边界引起的边缘效应。不同于一般目标的远场雷达散射截面表达,在该模型下,半空间电磁散射的远场描述需要用差场雷达散射截面。给出的算例能与现有文献以及仿真软件很好的吻合,并可作为实用工具分析半空间背景对目标远场响应的影响。  相似文献   

8.
选择谐波函数作为散射源的表征基函数,利用随机矩阵进行观测,实现了对散射源的稀疏表征,最后通过正交匹配追踪算法解算出表面散射源.利用压缩感知—正交匹配追踪算法与直接求解矩阵方程所得到的散射远场分布一致.  相似文献   

9.
张培珍  李秀坤  范军  王斌  林芳 《声学学报》2021,46(6):950-960
提出逆向运用傅里叶衍射定理预报水下弱散射目标三维声散射指向分布的快速计算方法。依据目标形状、周围介质的密度和声速构建三维声场图像模型,建立散射远场积分结果与图像频域幅值的关系式,提取频域中半径为水中波数k;的球型表面上的幅值,获得精细化的宽带、全方位散射声压指向特性。数值计算表明:将傅里叶衍射定理逆向运用于解决声学正问题,适用于分层的、不均匀的、非规则及多体弱散射目标散射声场的求解。通过插值提取频域样本获得远场声压的方法,避免了有限元法(3D-FEM)所必须的大规模的网格划分和迭代运算,可以有效地减少计算成本并拓展散射频率响应的带宽。在水池中完成两种具有不同声学参数和形状目标指向性测试实验,得到散射声压指向性幅度函数与理论预报相一致。   相似文献   

10.
 首先讨论了自由空间中一维周期结构近-远场外推的Floquet模方法,即对FDTD计算所得散射近场中输出边界上散射场进行级数展开,求出各阶Floquet模的复数幅值,再求得远区场。接着介绍了求解一维周期结构远区散射场的周期Green函数方法,即根据FDTD计算所得散射近场中输出边界上散射场,求得等效面电磁流后,再借助周期Green函数进行外推得到远区场。两种方法均仅用一个周期单元内的散射近场进行外推。计算结果验证了上述两种方法外推的有效性。  相似文献   

11.
This work is concerned with the reconstruction, from measured (synthetic or real) data, of a 2D penetrable fluid-like object of arbitrary cross-section embedded in a fluid of infinite extent and insonified by a plane acoustic wave. Green's theorem is used to provide a domain integral representation of the scattered field. The introduction therein of the Born approximation gives rise to a linearized form of the inverse problem. The actual inversion is carried out by two methods. The first diffraction tomography (DT), exhibits the contrast function very conveniently and explicitly in the form of a wave number/incident angle Fourier transform of the far backscattered field and thus requires measurements of this field for incident waves all around the object and at all frequencies. The second discretized domain integral equation with Born approximation method, is numerically more intensive, but enables a wider choice of configurations and requires less measurements (one or several frequencies, one or several incident waves, choice of measurement points) than the DT method. A comparison of the two methods is carried out by inversion of both simulated and experimental scattered field data.  相似文献   

12.
A numerically efficient technique is presented for computing the field radiated or scattered from three-dimensional objects embedded within layered acoustic media. The distance between the receivers and the object of interest is supposed to be large compared to the acoustic wavelength. The method requires the pressure and normal particle displacement on the surface of the object or on an arbitrary circumscribing surface, as an input, together with a knowledge of the layered medium Green's functions. The numerical integration of the full wave number spectral representation of the Green's functions is avoided by employing approximate formulas which are available in terms of elementary functions. The pressure and normal particle displacement on the surface of the object of interest, on the other hand, may be known by analytical or numerical means or from experiments. No restrictions are placed on the location of the object, which may lie above, below, or across the interface between the fluid media. The proposed technique is verified through numerical examples, for which the near field pressure and the particle displacement are computed via a finite-element method. The results are compared to validated reference models, which are based on the full wave number spectral integral Green's function.  相似文献   

13.
在基于目标回光的激光瞄准系统和目标在回路(TIL)系统中都要使用目标照明漫反射回光作为系统工作的基础.数值仿真在研究光波传输特性的过程中一直发挥着重要作用.由于漫反射光场发散角很大,给数值计算带来困难.一般的处理方法是进行分段空间域滤波,但这会大大增加计算量.提出一种计算漫反射光传榆的频率域滤波方法.频域滤波基本不增加...  相似文献   

14.
The ensemble-averaged field scattered by a smooth, bounded, elastic object near a penetrable surface with small-scale random roughness is formulated. The formulation consists of combining a perturbative solution for modeling propagation through the rough surface with a transition (T-) matrix solution for scattering by the object near a planar surface. All media bounding the rough surface are assumed to be fluids. By applying the results to a spherical steel shell buried within a rough sediment bottom, it is demonstrated that the ensemble-averaged "incoherent" intensity backscattered by buried objects illuminated with shallow-grazing-angle acoustic sources can be well enhanced at high frequencies over field predictions based on scattering models where all environmental surfaces are planar. However, this intensity must compete with the incoherent intensity scattered back from the interface itself, which can defeat detection attempts. The averaged "coherent" component of the field maintains the strong evanescent spectral decay exhibited by flat interface predictions of shallow-angle measurements but with small deviations. Nevertheless, bistatic calculations of the coherent field suggest useful strategies for improving long-range detection and identification of buried objects.  相似文献   

15.
Abstract

The finite element method (FEM) of Monte Carlo simulations of random rough surface scattering is extended to penetrable rough surface scattering. The attraction of the method is the banded nature of the resulting matrix equation. The method yields a system of linear algebraic equations which is solved by a direct sparse symmetric matrix inversion. Convergence and accuracy of the method is demonstrated and established by varying various input parameters such as the number of evanescent waves, the number of sampling points and the surface lengths. Results with incident plane wave TE polarization are presented for both the mean reflected scattered intensity and the mean transmitted scattered intensity as a function of surface parameters such as RMS surface heights and correlation lengths. The numerical results are compared against the tapered wave integral equation (TWIE) method. The results of a tapered wave solution of the integral equation averaging over many realizations are in good numerical agreement with FEM if large surface lengths are used in the integral equation method. It is found that a large surface length is required in the TWIE method to have a narrow incident angular spectlum to accurateiy predict the transmitted scattered intensity, whereas a relatively small surface length is sufficient in the FEM. The total CPU time and memory storage requirements for the FEM are much less than that of the TWIE method for eases when the number of horizontal sampling points is much larger than the number of vertical sampling points in the region of discretization. The percentage error in conservation of energy for the FEM is shown to be less than 0.4% for all the examples presented. The total CPU time, memory storage requirements and the percentage error comparisons between the FEM and the TWIE are presented.  相似文献   

16.
In this paper, a new heuristic approach based on chaos genetic algorithm and modified transfer matrix method is presented to demodulate the fiber Bragg grating strain sensors. To facilitate accurate calculation of the grating reflected intensity spectrum, the modified transfer matrix approach is applied. The motivation for using the spline smooth function scheme is to provide nice approximation of strain profiles from a scattered data set and overcome the difficulty of calculating the strain gradients in local period function of the modified T-matrix formulation for the piecewise constant strain field assumption. The chaos genetic algorithm is developed to improve the performance of GA and optimize the data of control nodes of the spline smooth function, and more valuably, the reconstructed strain profile is continuous with discretionary spatial resolution. The proposed method is verified through numerical example reconstructions of Bragg grating sensor simulated strain profile cases.  相似文献   

17.
The finite element method (FEM) of Monte Carlo simulations of random rough surface scattering is extended to penetrable rough surface scattering. The attraction of the method is the banded nature of the resulting matrix equation. The method yields a system of linear algebraic equations which is solved by a direct sparse symmetric matrix inversion. Convergence and accuracy of the method is demonstrated and established by varying various input parameters such as the number of evanescent waves, the number of sampling points and the surface lengths. Results with incident plane wave TE polarization are presented for both the mean reflected scattered intensity and the mean transmitted scattered intensity as a function of surface parameters such as RMS surface heights and correlation lengths. The numerical results are compared against the tapered wave integral equation (TWIE) method. The results of a tapered wave solution of the integral equation averaging over many realizations are in good numerical agreement with FEM if large surface lengths are used in the integral equation method. It is found that a large surface length is required in the TWIE method to have a narrow incident angular spectlum to accurateiy predict the transmitted scattered intensity, whereas a relatively small surface length is sufficient in the FEM. The total CPU time and memory storage requirements for the FEM are much less than that of the TWIE method for eases when the number of horizontal sampling points is much larger than the number of vertical sampling points in the region of discretization. The percentage error in conservation of energy for the FEM is shown to be less than 0.4% for all the examples presented. The total CPU time, memory storage requirements and the percentage error comparisons between the FEM and the TWIE are presented.  相似文献   

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