Acoustic Crosstalk Reduction Method for CMUT Arrays
Transkript
Acoustic Crosstalk Reduction Method for CMUT Arrays
Acoustic Crosstalk Reduction Method for CMUT Arrays Baris Bayram, Goksen G. Yaralioglu, Mario Kupnik, and Butrus T. Khuri-Yakub Ginzton Laboratory, Stanford University, CA 2006 IEEE Ultrasonics Symposium, Vancouver, Canada Khuri-Yakub Group, Ginzton Lab, Stanford University Bayram© Outline Motivation Finite element (FE) analysis of a 1-D CMUT array Experimental verification A new method to reduce crosstalk Conclusion Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Motivation To accurately model the crosstalk in CMUT arrays in “linear” and nonlinear operation regimes using time-domain, finite element method (FEM) To reduce the crosstalk between array elements using FEM to explore novel methods Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University 1-D CMUT Array Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Finite Element Model of the Array Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Features of the FE Analysis Explicit, time-domain solver of a commercially available software (LS-DYNA 970) – 3-D modeling of an actual CMUT array in detail – Memory-efficient, faster calculations for large million-node models Electrostatic-structural coupling – Electromechanical transducer modeling of the CMUT Robust contact implementation – CMUT modeling in collapsed and collapse-snapback nonlinear operation modes Fast, initial biasing of the CMUT array – 40 times faster results in biasing conventional or collapsed modes for a 20-element model Verification with interferometer measurement results for an identical CMUT array – Accurate and reliable FE results Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Displacement across Neighbors Conventional mode Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Pressure across Neighbors Conventional mode Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Pressure Waves on the Surface Conventional mode Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Pressure Waves on the Surface Collapsed mode Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Experimental Verification Experiment Collapsed Conventional Simulation Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Dispersive Guided Modes Frequency Collapsed Conventional Time Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Modified CMUT Regular CMUT Crosstalk Reduction Method Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Modified CMUT Regular CMUT Reduced Crosstalk for the Modified CMUT Bayram© Pressure Displacement Khuri-Yakub Group, Ginzton Lab, Stanford University Modified CMUT Regular CMUT Reduced Crosstalk for the Modified CMUT Bayram© Pressure Displacement Khuri-Yakub Group, Ginzton Lab, Stanford University Reduced Crosstalk for the Modified CMUT Pressure Displacement Crosstalk level is improved by approximately 10 dB for the modified CMUT array. Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University Conclusion Crosstalk in 1-D CMUT arrays is modeled using LS-DYNA in both conventional and collapsed modes. Finite element results are verified with the interferometer measurements. Dispersive guided mode is the main crosstalk mechanism. A powerful method based on the acoustic band gap is presented to reduce the crosstalk without loss of the pressure of the transmitter element. Bayram© Khuri-Yakub Group, Ginzton Lab, Stanford University
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