3 edition of **Solution of the three-dimensional Helmholtz equation with nonlocal boundary conditions** found in the catalog.

Solution of the three-dimensional Helmholtz equation with nonlocal boundary conditions

- 115 Want to read
- 19 Currently reading

Published
**1995** by National Aeronautics and Space Administration, Langley Research Center, National Technical Information Service, distributor in Hampton, Va, [Springfield, Va .

Written in English

- Boundary conditions.,
- Ducted flow.,
- Helmholtz equations.,
- Linear systems.,
- Point sources.,
- Sound generators.,
- Three dimensional flow.

**Edition Notes**

Other titles | Solution of the three dimensional Helmholtz equation with nonlocal boundary conditions. |

Statement | Steve Hodge, William E. Zorumski, and Willie R. Watson. |

Series | NASA technical memorandum -- 110174. |

Contributions | Zorumski, W. E., Watson, Willie R., Langley Research Center. |

The Physical Object | |
---|---|

Format | Microform |

Pagination | 1 v. |

ID Numbers | |

Open Library | OL18081616M |

of various elliptic problems with classical boundary conditions using RBF-based meshless methods. The RBF-based meshless methods for the solution of PDEs with nonlocal boundary conditions have been applied in a few papers. We can mention works [44–47] where such methods where used for the solution . Mathematics Stack Exchange is a question and answer site for people studying math at any level and professionals in related fields. Two dimensional Helmholtz equation and complex function theory. Ask Question Asked 3 Helmholtz equation in a circle with nonhomogeneous boundary conditions. 8 (Fundamental) Solution of the Helmholtz.

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The Helmholtz equation is solv ed within a three-dimensional rectangular duct with a sound source at the duct en trance plane, lo cal admittance conditions on the side w alls, and a. The Helmholtz equation is solved within a three-dimensional rectangular duct with a sound source at the duct entrance plane, local admittance conditions on the side walls, and a new, nonlocal radiation boundary condition at the duct exit plane.

Get this from a library. Solution of the three-dimensional Helmholtz equation with nonlocal boundary conditions. [Steve L Hodge; W E Zorumski; Willie R Watson; Langley Research.

The Helmholtz equation is solved within a three-dimensional rectangular duct with a sound source at the duct entrance plane, local admittance conditions on the side walls, and a new, nonlocal radiation boundary condition at the duct exit plane.

The formulation employs a truncation of an infinite matrix, the generalized modal admittance tensor. The Helmholtz equation is solved within a three-dimensional rectangular duct with a sound source at the duct entrance plane, local admittance conditions on the side walls, and new, nonlocal radiation boundary condition at the duct exit plane.

In nonlocal elasticity theory, Galerkin approach has some problems with free boundary conditions and in three-dimensional analysis of any plate, top and bottom surfaces are considered as free boundaries. It is noted that solutions to Helmholtz three-dimensional differential equations in Cartesian coordinates have a hyperbolic-trigonometric Cited by: 5.

The numerical solution of the Helmholtz equation subject to nonlocal radiation boundary conditions is studied. The specific problem is the propagation of hydroacoustic waves in a two-dimensional curvilinear duct. The problem is discretized with a second-order accurate finite difference method, resulting in a linear system of by: HELMHOLTZ EQUATION WITH ARTIFICIAL BOUNDARY CONDITIONS IN A TWO-DIMENSIONAL WAVEQUIDE D.A.

MITSOUDIS yx, CH. MAKRIDAKIS zx, AND M. PLEXOUSAKIS Abstract. We consider a time-harmonic acoustic wave propagation problem File Size: KB.

Consequently, any combination of boundary conditions can be imposed along x = 0, x = i, without affecting the solution, as long as () and () are satisfied on ^(x) and ^(x), respectively. In particular, separable boundary conditions can be imposed, so that eigenvalues and eigenfunction solutions can be obtained for ().Cited by: Wave equation reduces to Helmholtz Equation Fundamental solution of u k2u = 0 in R3 G k(x;y) = 1 4ˇ eikjx yj jx yj x 6= y also 1 4ˇ e ik jx y jx yj is a fundamental solution - justify our.

In [G. Fibich, S. Tsynkov, High-order two-way artificial boundary conditions for nonlinear wave propagation with backscattering, J. Comput. Phys., () ] and [G. Fibich, S. Tsynkov, Numerical solution of the nonlinear Helmholtz equation. Stack Exchange network consists of Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their.

of solution is the point-matching or collocation method, whereby an exact solution of the Helmholtz equation is made to satisfy the boundary conditions approximately.

5 The TE (Neumann) and TM (Dirichlet) modes 6 of the regions of Fig. 6 (Chapter 3 File Size: KB. • One way wave equations • Solution via characteristic curves • Solution via separation of variables • Helmholtz’ equation • Classiﬁcation of second order, linear PDEs • Hyperbolic equations and the wave equation 2.

Lecture Two: Solutions to PDEs with boundary conditions and initial conditions • Boundary and initial conditionsCited by: 2.

This volume in the Elsevier Series in Electromagnetism presents a detailed, in-depth and self-contained treatment of the Fast Multipole Method and its applications to the solution of the Helmholtz equation Cited by: The nonlocal boundary condition on B is determined for equations of the type 2u + k2u = 0 in a separable coordinate system, and compared with two methods in which the boundary condition.

Exact Solutions > Linear Partial Differential Equations > Second-Order Elliptic Partial Differential Equations > Helmholtz Equation. Helmholtz Equation ¢w + ‚w = –'(x) Many problems related to steady-state oscillations (mechanical, acoustical, thermal File Size: 68KB. the logarithmic boundary condition is odd, which led me to believe that the solution X(x) is expandable to a sine column.

the boundary condition [itex]E_z(y\rightarrow-\infty)=0 [/itex] together with the logarithmic boundary condition. In this document we discuss the ﬁnite-element-based solution of the Helmholtz equation, an elliptic PDE that de- scribes time-harmonic wave propagation problems.

We start by reviewing File Size: KB. The numerical solution of the Helmholtz equation subject to nonlocal radiation boundary conditions is studied. The specific problem is the propagation of hydroacoustic waves in a two-dimensional curvilinear duct.

The problem is discretized with a second-order accurate finitedifference method, resulting in a linear system of equations. Neumann or a Robin condition. For boundary value problems associated with ODEs, we derived general for-mulas (equations and in Section ) for Green’s functions.

This was File Size: KB. uniformly in with, where the vertical bars denote the Euclidean norm. With this condition, the solution to the inhomogeneous Helmholtz equation is the convolution (notice this integral is. FEM solution for the two-dimensional Helmholtz equation.

Finite element methods (FEM), initially developed for structural mechanics [70], are widely used for numerical simulations of. Solution of Helmholtz equation by Trefftz method. Cheung. A simple Trefftz method for solving the Cauchy problems of three-dimensional Helmholtz equation, Engineering Analysis with Boundary Elements, 63,Effectiveness of nonsingular solutions of the boundary.

Bin-Mohsin, B. and Lesnic, D. () The method of fundamental solutions for Helmholtz-type equations in composite materials, Computers and Mathe- with two- or three-dimensional Helmholtz-type equations.

Inverse problems have unknows are determined by imposing the available boundary conditions. Two dimensional invisibility cloaking for Helmholtz equation and non-local boundary conditions Article in Mathematical Research Letters 18(3) November with 34 Reads.

We consider a time-harmonic acoustic wave propagation problem in a two-dimensional water waveguide confined between a horizontal surface and a locally varying bottom. We formulate a model based on the Helmholtz equation coupled with nonlocal Dirichlet-to-Neumann boundary conditions Cited by: 5.

In [G. Fibich, S. Tsynkov, High-order two-way artiﬁcial boundary conditions for nonlinear wave propagation with backscattering, J.

Comput. Phys., () –] and [G. Fibich, S. Tsynkov, Numerical solution of the nonlinear Helmholtz equation. Transformation optics constructions have allowed the design of cloaking devices that steer electromagnetic, acoustic and quantum waves around a region without penetrating it, so that.

Helmholtz Equation and High Frequency Approximations 1 The Helmholtz equation TheHelmholtzequation, u(x) + n(x)2!2u(x) = f(x); x2Rd; (1) is a time-independent linear partial diﬀerential equation. The interpretation of the unknown u(x) and the parameters n(x),!and f(x) depends on what the equation File Size: KB.

The Dirichlet Problem for the Helmholtz Equation 2. A Representation Theorem In this section we first adopt notation and record some definitions, then state and prove an important representation theorem.

Let B be the boundary. Green's Function for the Up: Green's Functions for the Previous: Poisson Equation Contents Green's Function for the Helmholtz Equation. If we fourier transform the wave equation, or alternatively attempt to find solutions.

The study of boundary-value problems for linear differential equations was initiated by many authors. The formulae of Green's functions for many problems with classical boundary conditions are presented in [].In this book, Green's functions are constructed for regular and singular boundary-value problems for ODEs, the Helmholtz equation, and linear nonstationary by: ing boundary condition using partitioned low rank matrices.

The result, modulo a precomputation, is a fast and memory-e cient compression scheme of an absorbing boundary condition for the Helmholtz equation File Size: 2MB. Solution of Inhomogeneous Helmholtz Equation the three-dimensional delta function can be written () It follows that () Let us expand the Green's function in the form () Substitution of this expression into Equation yields () The appropriate boundary conditions.

Unfortunately the direct solution of equation requires the inversion of a multi-dimensional convolutional with Poisson's equation above, the application of helical boundary conditions. We propose an analytic perturbative scheme in the spirit of Lord Rayleigh's work for determining the eigenvalues of the Helmholtz equation in three dimensions inside an arbitrary boundary where the eigenfunction satisfies either the Dirichlet boundary condition or the Neumann boundary condition Author: S.

Panda, S. Panda, G. Hazra. These drawbacks have been widely discussed within the framework of beam theory. 5, 14, 52, 55 Polyanin and Manzhirov 52 showed that, in order that the solution of the differential equation be also a solution of the integral equation, the stress must satisfy some specific boundary conditions which, together with the equilibrium equations.

conditions are presented in 1. In this book, Green’s functions are constructed for regular and singular boundary-value problems for ODEs, the Helmholtz equation, and linear nonstationary equations.

The investigation of semilinear problems with Nonlocal Boundary Conditions NBCs and the existence of their positive solutions Cited by: Mixed Boundary Value Problems for the Helmholtz Equation in a Quadrant L. Castro, F.-O. Speck and F. Teixeira Dedicated to the memory of Ernst Lu¨neburg Abstract.

The main objective is the study of a class of boundary value prob-lems in weak formulation where two boundary conditions. The wave equation is an important second-order linear partial differential equation for the description of waves—as they occur in classical physics—such as mechanical waves (e.g.

.The Helmholtz equation, named for Hermann von Helmholtz, is the elliptic partial differential equation: (abla^2 + k^2) A = 0 where abla^2 is the Laplacian, k is a constant, and the unknown function A=A(x, y, z) is defined on "n"-dimensional Euclidean space R "n" (typically "n" = 1, 2, or 3, when the solution to this equation .A rigorous but accessible introduction to the mathematical theory of the three-dimensional Navier–Stokes equations, this book provides self-contained proofs of someof the most Cited by: