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finite element time domain (fetd)-based simulation software comsol multiphysics  (COMSOL Inc)

 
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    COMSOL Inc finite element time domain (fetd)-based simulation software comsol multiphysics
    Finite Element Time Domain (Fetd) Based Simulation Software Comsol Multiphysics, 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/finite+element+method+calculation+software+comsol+multiphysics/finite+element+time+domain++fetd++based+simulation+software+comsol+multiphysics/pm37297068-52-11-18
    Average 90 stars, based on 1 article reviews
    finite element time domain (fetd)-based simulation software comsol multiphysics - by Bioz Stars, 2026-11
    90/100 stars

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    Article Title: Towards High-Efficiency Photon Trapping in Thin-Film Perovskite Solar Cells Using Etched Fractal Metadevices
    Article Snippet: The considered structures are simulated and investigated using a commercially available Finite Element Time Domain (FETD)-based simulation software (Comsol Multiphysics).

    Article Title: Towards High-Efficiency Photon Trapping in Thin-Film Perovskite Solar Cells Using Etched Fractal Metadevices.
    Article Snippet: The considered structures are simulated and investigated using a commercially available Finite Element Time Domain (FETD)-based simulation software (Comsol Multiphysics).

    Article Title: A Comparative Investigation of Presaturated Core Fault Current Limiters Biased by DC Current and Permanent Magnet
    Article Snippet: In this paper, the dc biasing magnetomotive force (mmf) in presaturated core fault current limiter (PCFCL) is replaced with permanent magnet (PM) to overcome the well-known drawbacks of the dc biased PCFCLs.. These drawbacks are excessively induced voltage across the terminals of the dc coil during fault condition and high total power losses during the steady-state condition.. The novel contributions of this paper are the introduction of the selection criteria of PM material and its representation by actual nonlinear B-H hysteresis loop of Jiles-Atherton method, and the use of PM alone as an equivalent to the dc biasing coils for three-phase fault current limiter (FCL), contrary to work reported in earlier papers.

    Article Title: Non-Layered Gold-Silicon and All-Silicon Frequency-Selective Metasurfaces for Potential Mid-Infrared Sensing Applications
    Article Snippet: In terms of simulation conditions, all simulations were performed using a commercial Finite Element Time Domain (FETD)-based simulation medium—COMSOL Multiphysics, Radio Frequency (RF) interface.



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    ( A ) Schematic images of a cell that first invades the scaffold (1), builds up initial force in the process (2), and is later stretched by the scaffold (3). ( B ) Linear relationship of changes in displacement and changes in cellular traction forces, obtained by numerical calculations in COMSOL <t>Multiphysics.</t> Negative displacements are defined to point toward the center of the scaffold. ( C ) Exemplary images of displacements from numerical calculations before (left) and after (right) the swelling of the hydrogel. ( D ) Reaction of an exemplary cell in a scaffold as a function of time after addition of trypsin at minute 17. The black data points depict the displacement change, and the blue data points depict the change in traction force. ( E ) Optical micrographs of a cell before, during, and after addition of trypsin. The blue arrows indicate the displacement of the individual beams scaled by a factor of 10. The images below show a magnification of the left beam, with the green dashed line denoting the beam position of the initial frame and the blue dashed line denoting the position of the current frame. The numbers next to the arrow show the cellular reaction as a change in displacement and traction force relative to the first image. ( F ) Quantification of initial forces in the scaffolds for U2OS and NIH 3T3 cells. Each data point corresponds to one cell in a scaffold.
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    ( A ) Schematic images of a cell that first invades the scaffold (1), builds up initial force in the process (2), and is later stretched by the scaffold (3). ( B ) Linear relationship of changes in displacement and changes in cellular traction forces, obtained by numerical calculations in COMSOL Multiphysics. Negative displacements are defined to point toward the center of the scaffold. ( C ) Exemplary images of displacements from numerical calculations before (left) and after (right) the swelling of the hydrogel. ( D ) Reaction of an exemplary cell in a scaffold as a function of time after addition of trypsin at minute 17. The black data points depict the displacement change, and the blue data points depict the change in traction force. ( E ) Optical micrographs of a cell before, during, and after addition of trypsin. The blue arrows indicate the displacement of the individual beams scaled by a factor of 10. The images below show a magnification of the left beam, with the green dashed line denoting the beam position of the initial frame and the blue dashed line denoting the position of the current frame. The numbers next to the arrow show the cellular reaction as a change in displacement and traction force relative to the first image. ( F ) Quantification of initial forces in the scaffolds for U2OS and NIH 3T3 cells. Each data point corresponds to one cell in a scaffold.

    Journal: Science Advances

    Article Title: Mechanical stimulation of single cells by reversible host-guest interactions in 3D microscaffolds

    doi: 10.1126/sciadv.abc2648

    Figure Lengend Snippet: ( A ) Schematic images of a cell that first invades the scaffold (1), builds up initial force in the process (2), and is later stretched by the scaffold (3). ( B ) Linear relationship of changes in displacement and changes in cellular traction forces, obtained by numerical calculations in COMSOL Multiphysics. Negative displacements are defined to point toward the center of the scaffold. ( C ) Exemplary images of displacements from numerical calculations before (left) and after (right) the swelling of the hydrogel. ( D ) Reaction of an exemplary cell in a scaffold as a function of time after addition of trypsin at minute 17. The black data points depict the displacement change, and the blue data points depict the change in traction force. ( E ) Optical micrographs of a cell before, during, and after addition of trypsin. The blue arrows indicate the displacement of the individual beams scaled by a factor of 10. The images below show a magnification of the left beam, with the green dashed line denoting the beam position of the initial frame and the blue dashed line denoting the position of the current frame. The numbers next to the arrow show the cellular reaction as a change in displacement and traction force relative to the first image. ( F ) Quantification of initial forces in the scaffolds for U2OS and NIH 3T3 cells. Each data point corresponds to one cell in a scaffold.

    Article Snippet: Therefore, we used numerical finite element method calculations using the commercial software COMSOL Multiphysics.

    Techniques: