Ultrasonic Field Modeling: A Comparison of Analytical, Semi-Analytical, and Numerical Techniques

被引:52
|
作者
Kundu, Tribikram [1 ,2 ]
Placko, Dominique [3 ]
Rahani, Ehsan Kabiri [1 ]
Yanagita, Tamaki [2 ]
Dao, Cac Minh [1 ]
机构
[1] Univ Arizona, Dept Civil Engn & Engn Mech, Tucson, AZ 85721 USA
[2] Univ Arizona, Dept Aerosp & Mech Engn, Tucson, AZ 85721 USA
[3] Ecole Normale Super, Syst Applicat Informat Technol & Energy Lab SATIE, Dept Elect Engn, Cachan, France
关键词
RESILIENT DISK; GUIDED-WAVES; SOUND FIELD; BEAM MODELS; RADIATION; TRANSDUCERS; PROPAGATION; DIFFRACTION; SIMULATION; LENS;
D O I
10.1109/TUFFC.2010.1753
中图分类号
O42 [声学];
学科分类号
070206 ; 082403 ;
摘要
Modeling ultrasonic fields in front of a transducer in the presence and absence of a scatterer is a fundamental problem that has been attempted by different techniques: analytical, semi-analytical, and numerical. However, a comprehensive comparison study among these techniques is currently missing in the literature. The objective of this paper is to make this comparison for different ultrasonic field modeling problems with various degrees of difficulty. Four fundamental problems are considered: a flat circular transducer, a flat square transducer, a circular concave transducer, and a point focused transducer (concave lens) in the presence of a cavity. The ultrasonic field in front of a finite-sized transducer can be obtained by Huygens-Fresnel superposition principle that integrates the contributions of several point sources distributed on the transducer face. This integral which is also known as the Rayleigh integral or Rayleigh-Sommerfeld integral (RSI) can be evaluated analytically for obtaining the pressure field variation along the central axis of the transducer for simple geometries, such as a flat circular transducer. The semi-analytical solution is a newly developed mesh-free technique called the distributed point source method (DPSM). The numerical solution is obtained from finite element analysis. Note that the first three problems study the effect of the transducer size and shape, whereas the fourth problem computes the field in presence of a scatterer.
引用
收藏
页码:2795 / 2807
页数:13
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