Semi-analytical modeling of ultrasonic fields in solids with internal anomalies immersed in a fluid

Modeling of ultrasonic fields in presence of cracks, inclusions and delaminations in materials is of great interest to the researchers in the field of real time non-destructive evaluation (NDE) and structural health monitoring (SHM). Ultrasonic fields generated by finite size transducers in various structures with cracks and inclusions simulating actual experiments have been studied by numerical and semi-analytical techniques. However, many of the semi-analytical techniques lack simple implementation for complex structure geometries and numerical techniques often suffer from accuracy problems at high frequencies. Several attempts to compute the ultrasonic fields inside solid media have been made based on approximate paraxial methods such as the classical ray-tracing and multi-Gaussian beam models. These approximate methods have several limitations. A new semi-analytical method is adopted in this paper to model elastic wave fields in half-space and plate structures with internal anomalies generated by finite size transducers. A general formulation good for both isotropic and anisotropic solids is presented in this paper. No simplifying assumption has been made on the geometry of the anomalies. Therefore, the formulation presented in this paper can be applied to anomalies with any geometry.

[1]  Tribikram Kundu,et al.  Advanced Applications of Distributed Point Source Method – Ultrasonic Field Modeling in Solid Media , 2006 .

[2]  Sourav Banerjee,et al.  Elastic Wave Propagation in Corrugated Wave Guides , 2005 .

[3]  George D. Manolis,et al.  Elastodynamic fundamental solutions for certain families of 2d inhomogeneous anisotropic domains: basic derivations , 2005 .

[4]  Ch. Hafner MMP calculations of guided waves , 1985 .

[5]  Dominique Placko,et al.  Theoretical computation of acoustic pressure generated by ultrasonic sensors in the presence of an interface , 2002, Smart Structures and Materials + Nondestructive Evaluation and Health Monitoring.

[6]  Gerald R. Harris,et al.  Review of transient field theory for a baffled planar piston , 1981 .

[7]  Bill D. Cook,et al.  Theoretical Investigation of the Integrated Optical Effect Produced by Sound Fields Radiated from Plane Piston Transducers , 1969 .

[8]  R. Burridge,et al.  Fundamental elastodynamic solutions for anisotropic media with ellipsoidal slowness surfaces , 1993, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[9]  Lester W. Schmerr,et al.  Ultrasonic beam models: An edge element approach , 1998 .

[10]  Matthias G. Imhof,et al.  Computing the elastic scattering from inclusions using the multiple multipoles method in three dimensions , 2004 .

[11]  Theodor Tamir,et al.  Unified theory of Rayleigh-angle phenomena for acoustic beams at liquid-solid interfaces , 1973 .

[12]  K. Sung,et al.  Effect of spatial sampling in the calculation of ultrasonic fields generated by piston radiators , 1992 .

[13]  V. Vavryčuk Elastodynamic and elastostatic Green tensors for homogeneous weak transversely isotropic media , 1997 .

[14]  Tribikram Kundu,et al.  Elastic wave propagation in sinusoidally corrugated waveguides. , 2006, Journal of the Acoustical Society of America.

[15]  F. John Plane Waves and Spherical Means: Applied To Partial Differential Equations , 1981 .

[16]  Sohichi Hirose,et al.  MODELING OF IMMERSION ULTRASONIC TESTING AND SIMULATION OF SCATTERED WAVES BY FLAWS , 2006 .

[17]  M. Imhof Multiple multipole expansions for elastic scattering , 1995 .

[18]  M. Spies,et al.  Elastic wave propagation in transversely isotropic media. II. The generalized Rayleigh function and an integral representation for the transducer field. Theory , 1995 .

[19]  C. Y. Wang,et al.  Elastodynamic fundamental solutions for anisotropic solids , 1994 .

[20]  M. Spies Analytical methods for modeling of ultrasonic nondestructive testing of anisotropic media. , 2004, Ultrasonics.

[21]  Ryo Nishimura,et al.  Determining the arrangement of fictitious charges in charge simulation method using genetic algorithms , 2000 .

[22]  Developments in boundary element methods—1 , 1980 .

[23]  Woon-Seng Gan,et al.  A complex virtual source approach for calculating the diffraction beam field generated by a rectangular planar source. , 2003, IEEE transactions on ultrasonics, ferroelectrics, and frequency control.

[24]  Elfgard Kühnicke,et al.  Three‐dimensional waves in layered media with nonparallel and curved interfaces: A theoretical approach , 1996 .

[25]  A. Tverdokhlebov,et al.  On Green's functions for elastic waves in anisotropic media , 1988 .

[26]  Kaname Amano,et al.  Numerical conformal mappings of bounded multiply connected domains by the charge simulation method , 2003 .

[27]  J. Raamachandran,et al.  Bending of anisotropic plates by charge simulation method , 1999 .

[28]  L. W. Schmerr,et al.  A multigaussian ultrasonic beam model for high performance simulations on a personal computer , 2000 .

[29]  L. Schmerr,et al.  MULTI-GAUSSIA N ULTRASONIC BEAM MODELING , 2003 .

[30]  Byron Newberry,et al.  A paraxial theory for the propagation of ultrasonic beams in anisotropic solids , 1989 .

[31]  N. Wakatsuki,et al.  Electrical impedance evaluation in a conductive–dielectric half space by the charge simulation method , 2002 .

[32]  Dominique Placko,et al.  Ultrasonic field computation in the presence of a scatterer of finite dimension , 2003, SPIE Smart Structures and Materials + Nondestructive Evaluation and Health Monitoring.

[33]  Two-dimensional anisotropic elastic waves emanating from a point source , 1971 .

[34]  R. Wolfe,et al.  NEGATIVE THERMOELECTRIC FIGURE OF MERIT IN A MAGNETIC FIELD , 1963 .

[35]  P. Stepanishen Transient Radiation from Pistons in an Infinite Planar Baffle , 1970 .

[36]  Dominique Placko,et al.  Ultrasonic Field Modeling in Multilayered Fluid Structures Using the Distributed Point Source Method Technique , 2006 .

[37]  Martin Spies,et al.  Transducer field modeling in anisotropic media by superposition of Gaussian base functions , 1999 .

[38]  C. Hafner,et al.  The multiple multipole method in electro- and magnetostatic problems , 1983 .

[39]  M. A. Breazeale,et al.  A diffraction beam field expressed as the superposition of Gaussian beams , 1988 .

[40]  Dominique Placko,et al.  Modeling of phased array transducers. , 2005, The Journal of the Acoustical Society of America.

[41]  G. Duff,et al.  The Cauchy problem for elastic waves in an anisotropic medium , 1960, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[42]  Tribikram Kundu,et al.  Ultrasonic Nondestructive Evaluation : Engineering and Biological Material Characterization , 2003 .

[43]  Richard Paul Shaw Boundary integral equation methods applied to wave problems , 1979 .

[44]  J. Jensen,et al.  Calculation of pressure fields from arbitrarily shaped, apodized, and excited ultrasound transducers , 1992, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[45]  Dominique Placko,et al.  Theoretical study of magnetic and ultrasonic sensors: dependence of magnetic potential and acoustic pressure on the sensor geometry , 2001, SPIE Smart Structures and Materials + Nondestructive Evaluation and Health Monitoring.