2006
DOI: 10.1002/nme.1852
|View full text |Cite
|
Sign up to set email alerts
|

A boundary condition in Padé series for frequency‐domain solution of wave propagation in unbounded domains

Abstract: SUMMARYA boundary condition satisfying the radiation condition at infinity is frequently required in the numerical simulation of wave propagation in an unbounded domain. In a frequency domain analysis using finite elements, this boundary condition can be represented by the dynamic stiffness matrix of the unbounded domain defined on its boundary. A method for determining a Padé series of the dynamic stiffness matrix is proposed in this paper. This method starts from the scaled boundary finite-element equation, … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

1
18
0

Year Published

2007
2007
2014
2014

Publication Types

Select...
6
1

Relationship

3
4

Authors

Journals

citations
Cited by 32 publications
(19 citation statements)
references
References 52 publications
1
18
0
Order By: Relevance
“…Figure 4 shows the pressure distribution along the dam height acting on the rigid dam, in which the pressure p = − with fluid density , = H /c and the magnitude of pressure | p| is normalized by a 0 H . Analytical solutions [25] and solutions from Equation (1) in the full matrix form are marked with circles and rectangles, respectively, while solutions from the diagonal Equation (20) are plotted by solid line. The three results are exactly the same.…”
Section: Numerical Examplesmentioning
confidence: 99%
See 1 more Smart Citation
“…Figure 4 shows the pressure distribution along the dam height acting on the rigid dam, in which the pressure p = − with fluid density , = H /c and the magnitude of pressure | p| is normalized by a 0 H . Analytical solutions [25] and solutions from Equation (1) in the full matrix form are marked with circles and rectangles, respectively, while solutions from the diagonal Equation (20) are plotted by solid line. The three results are exactly the same.…”
Section: Numerical Examplesmentioning
confidence: 99%
“…In numerical methods, dams are often discretized into solid finite elements by using finite element method (FEM), while the reservoir is either directly modeled by boundary 598 S. M. LI methods were used to evaluate the dynamic stiffness matrix, which avoid evaluating integral convolution equations, but evaluation errors increased with frequency increasing so that results at high frequencies were not acceptable [19]. To evaluate accurately high frequencies behaviors of the dynamic stiffness matrix, a Pade series was presented to analyze out-of-plane motion of circular cavity embedded in full-plane through using the SBFEM alone [20]. Good results were obtained at high frequencies, but results at low frequencies were inferior even if a high-order Pade series was used.…”
Section: Introductionmentioning
confidence: 99%
“…Bazyar and Song extended the SBFEM to model time‐harmonic and transient response of non‐homogeneous elastic unbounded domains. They later developed new techniques to enhance the solution procedures for modeling unbounded domains in frequency and time domains . The method was later employed to model steady‐state seepage problems .…”
Section: Introductionmentioning
confidence: 99%
“…Alternative procedures, which aim at avoiding the convolution integral altogether by developing the SBFEM directly in the time domain, have been proposed recently. Song and Bazyar presented a Padé approximation of the dynamic stiffness matrix of an unbounded medium in the frequency‐domain, which has a large range and a high rate of convergence. Bazyar and Song then developed a high‐order local transmitting boundary based on a continued‐fraction solution of the dynamic stiffness matrix and applied it to two‐dimensional problems.…”
Section: Introductionmentioning
confidence: 99%