2011
DOI: 10.1142/s0218396x11004286
|View full text |Cite
|
Sign up to set email alerts
|

Computational Acoustics in Multi-Field Problems

MANFRED KALTENBACHER

Abstract: We present physical/mathematical models base on partial differential equations (PDEs) and efficient numerical simulation schemes based on the Finite Element (FE) method for multi-field problems, where the acoustic field is the field of main interest. Acoustics, the theory of sound, is an emerging scientific field including disciplines from physics over engineering to medical science. We concentrate on the following three topics: vibro-acoustics, aero-acoustics and high intensity focused ultrasound. For each to… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
8
0

Year Published

2011
2011
2023
2023

Publication Types

Select...
5
2
1

Relationship

1
7

Authors

Journals

citations
Cited by 10 publications
(8 citation statements)
references
References 60 publications
0
8
0
Order By: Relevance
“…For the following remarks, it is assumed that the wave propagation direction is perpendicular to the interface. In this case, the reflection coefficient R and the transmission coefficient T can be expressed in terms of acoustic impedances for a wave travelling from medium Z i into the adjacent medium Z i+1 , respectively (Bergman, 2018;Kaltenbacher, 2018;Rose, 2014)…”
Section: Theory On Acoustic Impedance Matchingmentioning
confidence: 99%
“…For the following remarks, it is assumed that the wave propagation direction is perpendicular to the interface. In this case, the reflection coefficient R and the transmission coefficient T can be expressed in terms of acoustic impedances for a wave travelling from medium Z i into the adjacent medium Z i+1 , respectively (Bergman, 2018;Kaltenbacher, 2018;Rose, 2014)…”
Section: Theory On Acoustic Impedance Matchingmentioning
confidence: 99%
“…This can be described recording to Refs. [18–20] with the reflection coefficient R and the transmission coefficient T as functions of acoustic impedances of a wave that propagates from material Zi$Z_i$ into material Zi+1$Z_{i+1}$: R=Zi+1ZiZi+1+Zi,$$\begin{align} R = \frac{Z_{i+1} - Z_{i}}{Z_{i+1} + Z_{i}}, \end{align}$$ T=2Zi+1Zi+1+Zi.$$\begin{align} T = \frac{2 Z_{i+1}}{Z_{i+1} + Z_{i}}. \end{align}$$…”
Section: Theory On Acoustic Impedance Matchingmentioning
confidence: 99%
“…This can be described recording to Refs. [18][19][20] with the reflection coefficient 𝑅 and the transmission coefficient 𝑇 as functions of acoustic impedances of a wave that propagates from material 𝑍 𝑖 into material 𝑍 𝑖+1 :…”
Section: Theory On Acoustic Impedance Matchingmentioning
confidence: 99%
“…All these propagation environments constitute a large number of inputs for a numerical acoustic propagation model, such as bellhop [4]. Using this software across all oceanographic results completes our oceanographic dataset from an acoustic point of view, providing signal arrival times via the ray tracing method [8], [9]. The amplitudes of the paths are also calculated, and knowledge of the position of the floats and sources over time also gives us access to their relative velocities and hence Doppler compression factor.…”
Section: B An Oceano-acoustic Datasetmentioning
confidence: 99%