equivalent circuit model (eqc) simulation results Search Results


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COMSOL Inc equivalent circuit model (eqc) simulation results
a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model <t>(EQC)</t> <t>simulations,</t> <t>COMSOL</t> simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations
Equivalent Circuit Model (Eqc) Simulation Results, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model (EQC) simulations, COMSOL simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations

Journal: Microsystems & Nanoengineering

Article Title: A low-voltage-driven MEMS ultrasonic phased-array transducer for fast 3D volumetric imaging

doi: 10.1038/s41378-024-00755-9

Figure Lengend Snippet: a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model (EQC) simulations, COMSOL simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations

Article Snippet: Fig. 4 The vibration velocity and two-dimensional pressure field distribution of the single element. a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model (EQC) simulations, COMSOL simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations In acoustic output characterization of one single element, the axial pressures at 5 mm from the pMUT surface evaluated by the EQC model (Fig. d_i and D_ii) are consistent with the reference data acquired by hydrophone experiments (Fig. e_i and e_ii).

Techniques: Transmission Assay, Comparison

Results of the transmission and receiving experiments of a single element

Journal: Microsystems & Nanoengineering

Article Title: A low-voltage-driven MEMS ultrasonic phased-array transducer for fast 3D volumetric imaging

doi: 10.1038/s41378-024-00755-9

Figure Lengend Snippet: Results of the transmission and receiving experiments of a single element

Article Snippet: Fig. 4 The vibration velocity and two-dimensional pressure field distribution of the single element. a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model (EQC) simulations, COMSOL simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations In acoustic output characterization of one single element, the axial pressures at 5 mm from the pMUT surface evaluated by the EQC model (Fig. d_i and D_ii) are consistent with the reference data acquired by hydrophone experiments (Fig. e_i and e_ii).

Techniques: Transmission Assay

a , b Acoustic coupling effects from central excitation and edge excitation characterized by the equivalent circuit model (EQC) model and the FEM model. a Cross-talk analysis of the 3 × 3 array. ( i ) An array using central excitation at element D4, in which neighboring elements B1, B3, and C3 are characterized. ( ii ) An array using edge excitation at element A2, in which neighboring elements A1, A3, and B2 are characterized. ( iii ) Quantitative analysis results for the cross-talk degree (in dB) using the equivalent circuit model (EQC) model and the FEM model. b Cross-talk analysis of the 8 × 8 array. ( i ) An array actuated with central excitation D4, in which neighboring elements C4, E4, and D5 are characterized. ( ii ) An array actuated with edge excitation B1, in which neighboring elements A1, C1, and B2 are characterized. ( iii ). Quantitative analysis results for the cross-talk degree (in dB) using the equivalent circuit model (EQC) model and the FEM model. c – f Varied focusing intensities of the 8 × 8 MEMS phased-array transducer characterized by equivalent circuit model (EQC) simulations and experimental measurements. c Focused pressure at different depths: Comparison between the calculated results of the equivalent circuit (EQC) model and the experimental measurements. d Spatial pressure field distribution of the entire array calculated by the equivalent circuit (EQC) model. e Relationship between the excitation voltage amplitude set in the imaging platform and the focused pressure measured at 30 mm. f Relationship between the actual voltage amplitude on the device and the focused pressure measured at 30 mm

Journal: Microsystems & Nanoengineering

Article Title: A low-voltage-driven MEMS ultrasonic phased-array transducer for fast 3D volumetric imaging

doi: 10.1038/s41378-024-00755-9

Figure Lengend Snippet: a , b Acoustic coupling effects from central excitation and edge excitation characterized by the equivalent circuit model (EQC) model and the FEM model. a Cross-talk analysis of the 3 × 3 array. ( i ) An array using central excitation at element D4, in which neighboring elements B1, B3, and C3 are characterized. ( ii ) An array using edge excitation at element A2, in which neighboring elements A1, A3, and B2 are characterized. ( iii ) Quantitative analysis results for the cross-talk degree (in dB) using the equivalent circuit model (EQC) model and the FEM model. b Cross-talk analysis of the 8 × 8 array. ( i ) An array actuated with central excitation D4, in which neighboring elements C4, E4, and D5 are characterized. ( ii ) An array actuated with edge excitation B1, in which neighboring elements A1, C1, and B2 are characterized. ( iii ). Quantitative analysis results for the cross-talk degree (in dB) using the equivalent circuit model (EQC) model and the FEM model. c – f Varied focusing intensities of the 8 × 8 MEMS phased-array transducer characterized by equivalent circuit model (EQC) simulations and experimental measurements. c Focused pressure at different depths: Comparison between the calculated results of the equivalent circuit (EQC) model and the experimental measurements. d Spatial pressure field distribution of the entire array calculated by the equivalent circuit (EQC) model. e Relationship between the excitation voltage amplitude set in the imaging platform and the focused pressure measured at 30 mm. f Relationship between the actual voltage amplitude on the device and the focused pressure measured at 30 mm

Article Snippet: Fig. 4 The vibration velocity and two-dimensional pressure field distribution of the single element. a – c Normalized vibration velocities of all cells within one single element characterized by equivalent circuit model (EQC) simulations, COMSOL simulations and laser Doppler velocimetry (LDV) measurements. a Equivalent circuit model (EQC) simulation results. b Finite element method (FEM) simulation results. c Laser Doppler velocimetry (LDV) measurements. d Acoustic transmission efficiency characterized by equivalent circuit model (EQC) simulations. e Acoustic transmission efficiency characterized by hydrophone experiments. f Comparison of the 2D pressure field between the equivalent circuit model (EQC) and finite element method (FEM) simulations In acoustic output characterization of one single element, the axial pressures at 5 mm from the pMUT surface evaluated by the EQC model (Fig. d_i and D_ii) are consistent with the reference data acquired by hydrophone experiments (Fig. e_i and e_ii).

Techniques: Comparison, Imaging