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multiphysics finite element simulation results of the capacitor model  (COMSOL Inc)

 
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    Structured Review

    COMSOL Inc multiphysics finite element simulation results of the capacitor model
    Multiphysics Finite Element Simulation Results Of The Capacitor Model, 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
    https://www.bioz.com/product/model+simulation+results/parallel+plate+capacitor+model/pm39716837-139-47-39
    Average 90 stars, based on 1 article reviews
    multiphysics finite element simulation results of the capacitor model - by Bioz Stars, 2026-11
    90/100 stars

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    Related Articles

    Comparison:

    Article Title: Optimization Design and Simulation of Light Broadband Multilayer Composite Absorber
    Article Snippet: .. Fig. 7 shows the comparison between the theoretical calculation and model simulation results in COMSOL. ..

    Produced:

    Article Title: Nanosecond shock wave-induced surface acoustic waves and dynamic fracture at fluid-solid boundaries
    Article Snippet: .. Moreover, while the mean radius of the ring cracks normalized by S d remains almost unchanged, the number of shocks (NS) required to initiate a ring crack decreases significantly with the incident pressure ( P i ) on the solid boundary [ ]. fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 5. caption a7 (a) A representative example of the initiation and progression of ringlike fractures produced at S d = 1.5mm ( R 1 , R 2 : the first and second ring fractures; E 1 , E 2 : the extension of the first and second ring fractures underneath the surface). (b) Optical microscopy images of ring fractures produced at various S d (the zoom in window shows a confocal microscopy of the sample at S d = 0.5mm, demonstrating the formation of multiple ring fractures). fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 6. caption a7 (a) Equivalent radius of the ring fractures produced at various S d ; the red line indicates the locations of the maximum tensile stress ( θ T, max ); the blue line indicates the location of the maximum of stress integral (SI) calculated based on the Tuler-Butcher criterion using the COMSOL model simulation results; the black dash lines delineate the lower and upper range in the radius of the ring fractures observed in the experiments. (b) the relationship between ring crack radius normalized by S d (left), the number of shocks, NS, (right) and the incident pressure on the solid boundary ( P i ) normalized by the Young’s modulus ( E ) of borosilicate glass. ..

    Microscopy:

    Article Title: Nanosecond shock wave-induced surface acoustic waves and dynamic fracture at fluid-solid boundaries
    Article Snippet: .. Moreover, while the mean radius of the ring cracks normalized by S d remains almost unchanged, the number of shocks (NS) required to initiate a ring crack decreases significantly with the incident pressure ( P i ) on the solid boundary [ ]. fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 5. caption a7 (a) A representative example of the initiation and progression of ringlike fractures produced at S d = 1.5mm ( R 1 , R 2 : the first and second ring fractures; E 1 , E 2 : the extension of the first and second ring fractures underneath the surface). (b) Optical microscopy images of ring fractures produced at various S d (the zoom in window shows a confocal microscopy of the sample at S d = 0.5mm, demonstrating the formation of multiple ring fractures). fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 6. caption a7 (a) Equivalent radius of the ring fractures produced at various S d ; the red line indicates the locations of the maximum tensile stress ( θ T, max ); the blue line indicates the location of the maximum of stress integral (SI) calculated based on the Tuler-Butcher criterion using the COMSOL model simulation results; the black dash lines delineate the lower and upper range in the radius of the ring fractures observed in the experiments. (b) the relationship between ring crack radius normalized by S d (left), the number of shocks, NS, (right) and the incident pressure on the solid boundary ( P i ) normalized by the Young’s modulus ( E ) of borosilicate glass. ..

    Confocal Microscopy:

    Article Title: Nanosecond shock wave-induced surface acoustic waves and dynamic fracture at fluid-solid boundaries
    Article Snippet: .. Moreover, while the mean radius of the ring cracks normalized by S d remains almost unchanged, the number of shocks (NS) required to initiate a ring crack decreases significantly with the incident pressure ( P i ) on the solid boundary [ ]. fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 5. caption a7 (a) A representative example of the initiation and progression of ringlike fractures produced at S d = 1.5mm ( R 1 , R 2 : the first and second ring fractures; E 1 , E 2 : the extension of the first and second ring fractures underneath the surface). (b) Optical microscopy images of ring fractures produced at various S d (the zoom in window shows a confocal microscopy of the sample at S d = 0.5mm, demonstrating the formation of multiple ring fractures). fig ft0 fig mode=article f1 fig/graphic|fig/alternatives/graphic mode="anchored" m1 Open in a separate window FIG. 6. caption a7 (a) Equivalent radius of the ring fractures produced at various S d ; the red line indicates the locations of the maximum tensile stress ( θ T, max ); the blue line indicates the location of the maximum of stress integral (SI) calculated based on the Tuler-Butcher criterion using the COMSOL model simulation results; the black dash lines delineate the lower and upper range in the radius of the ring fractures observed in the experiments. (b) the relationship between ring crack radius normalized by S d (left), the number of shocks, NS, (right) and the incident pressure on the solid boundary ( P i ) normalized by the Young’s modulus ( E ) of borosilicate glass. ..

    other:

    Article Title: An Apparatus for Measuring the Electron’s Electric Dipole Moment in Trapped ThF+
    Article Snippet: The COMSOL model simulation results are shown in Figure 3.12.



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    Image Search Results


    Overall design measuring the impact of uncertain sensitive attribute inference on bias mitigation algorithms.

    Journal: Frontiers in Artificial Intelligence

    Article Title: Impact on bias mitigation algorithms to variations in inferred sensitive attribute uncertainty

    doi: 10.3389/frai.2025.1520330

    Figure Lengend Snippet: Overall design measuring the impact of uncertain sensitive attribute inference on bias mitigation algorithms.

    Article Snippet: For the COMPAS and credit card client data sets, we use the simulated sensitive attribute inference model results with random misclassification at 0.75 balanced accuracy.

    Techniques:

    Gender  inference  accuracy using existing demographic  inference  models.

    Journal: Frontiers in Artificial Intelligence

    Article Title: Impact on bias mitigation algorithms to variations in inferred sensitive attribute uncertainty

    doi: 10.3389/frai.2025.1520330

    Figure Lengend Snippet: Gender inference accuracy using existing demographic inference models.

    Article Snippet: For the COMPAS and credit card client data sets, we use the simulated sensitive attribute inference model results with random misclassification at 0.75 balanced accuracy.

    Techniques:

    Balanced accuracy and fairness score of the outcome prediction  model  (using inferred  sensitive   attribute)  on Wikidata.

    Journal: Frontiers in Artificial Intelligence

    Article Title: Impact on bias mitigation algorithms to variations in inferred sensitive attribute uncertainty

    doi: 10.3389/frai.2025.1520330

    Figure Lengend Snippet: Balanced accuracy and fairness score of the outcome prediction model (using inferred sensitive attribute) on Wikidata.

    Article Snippet: For the COMPAS and credit card client data sets, we use the simulated sensitive attribute inference model results with random misclassification at 0.75 balanced accuracy.

    Techniques:

    Prediction model fairness difference using the ground truth sensitive attribute S and the inferred sensitive attribute S ′ with 0.75 balanced accuracy.

    Journal: Frontiers in Artificial Intelligence

    Article Title: Impact on bias mitigation algorithms to variations in inferred sensitive attribute uncertainty

    doi: 10.3389/frai.2025.1520330

    Figure Lengend Snippet: Prediction model fairness difference using the ground truth sensitive attribute S and the inferred sensitive attribute S ′ with 0.75 balanced accuracy.

    Article Snippet: For the COMPAS and credit card client data sets, we use the simulated sensitive attribute inference model results with random misclassification at 0.75 balanced accuracy.

    Techniques:

    Prediction model fairness difference between baseline model and bias mitigation methods using inferred sensitive attribute with 0.75 balanced accuracy.

    Journal: Frontiers in Artificial Intelligence

    Article Title: Impact on bias mitigation algorithms to variations in inferred sensitive attribute uncertainty

    doi: 10.3389/frai.2025.1520330

    Figure Lengend Snippet: Prediction model fairness difference between baseline model and bias mitigation methods using inferred sensitive attribute with 0.75 balanced accuracy.

    Article Snippet: For the COMPAS and credit card client data sets, we use the simulated sensitive attribute inference model results with random misclassification at 0.75 balanced accuracy.

    Techniques:

    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