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COMSOL Inc 2d electrostatic model
2d Electrostatic 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/2d+comsol+simulation/2d+electrostatic+simulation/pmc09205313-144-0-7
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2d electrostatic model - by Bioz Stars, 2026-10
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Article Title: Assembly of Shape-Tunable Colloidal Dimers in a Dielectrophoretic Field
Article Snippet: The shape of colloid particles plays an important role in directing the structure of their assemblies.. Anisotropic colloids can adopt more complex structures than can their spherical counterparts, illustrated here by organosilica dimers fabricated with precise control of particle shape.. Dielectrophoretic fields were used to coerce the assembly of 19 uniquely shaped dimers, which allowed direct visualization of the assembly process as well as the structure, symmetry, and long-range order (or lack thereof) of the final state.

Article Title: Flexible electronic-photonic 3D integration from ultrathin polymer chiplets
Article Snippet: Electrostatic analysis for the shielding effect A 2D electrostatics model was established in COMSOL Multiphysics to investigate shielding effects between the LED and electrode layers.

Article Title: GLIDER-A pulsed-current generator for laboratory astrophysics x-ray absorption experiments.
Article Snippet: In the field of pulse-power, there has always been an interest on small and medium size pulsed-current generators (≤2 MA) which are affordable and of low maintenance.. We developed the GLIDER, a compact and modular generator, that drives a gas-puff z-pinch load as a soft x-ray source (0.1–1 keV) for laboratory astrophysics absorption experiments.. It comprises 48 bricks, tightly packed in a 1.7 m × 3.5 m × 0.8 m transformer oil container.

Article Title: New local electrical diagnostic tool for dielectric barrier discharge (DBD).
Article Snippet: A new diagnostic tool to study dielectric barrier discharges (DBDs) at atmospheric pressure by local electrical measurements is introduced.. The square ground electrode is divided into 64 square segments (3.44 mm side length) so as to measure the discharge currents and gas voltages with spatial resolutions, which allows a 2D mapping.. The electrical measurement results are validated by a comparison with short exposure time photographs taken from the top view of the discharge cell.

Article Title: Ambulatory Cardiovascular Monitoring Via a Machine-Learning-Assisted Textile Triboelectric Sensor
Article Snippet: Electricity Generation Simulation: 2D electrostatic model in COMSOL Multiphysics was used to simulate electricity generation and output performance of the hierarchical and plane structured devices.

Article Title: Controlled Formation of Conduction Channels in Memristive Devices Observed by X-ray Multimodal Imaging.
Article Snippet: This was done for the 2D electrostatics simulation and Joule heating simulation using COMSOL software.

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Article Title: Bioinspired Electron Polarization of Nanozymes with a Human Self-Generated Electric Field for Cancer Catalytic Therapy.
Article Snippet: S. Yao, X. Zhao, X. Wang, T. Huang, Y. Ding, J. Zhang, Z. Zhang, Z. L. Wang, L. Li Beijing Institute of Nanoenergy and Nanosystems Chinese Academy of Sciences Beijing 101400, P. R. China E-mail: lilinlin@binn.cas.cn S. Yao, J. Zhang, Z. L. Wang, L. Li School of Nanoscience and Technology University of Chinese Academy of Sciences Beijing 101400, P. R. China T. Huang, Y. Ding, Z. Zhang, Z. L. Wang, L. Li Center on Nanoenergy Research Guangxi University Nanning 530004, China Z. L. Wang School of Materials Science and Engineering Georgia Institute of Technology Atlanta, GA 30332-0245, USA E-mail: zhong.wang@mse.gatech.edu The ORCID identification number(s) for the author(s) of this article can be found under https://doi.org/10.1002/adma.202109568.



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(a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
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(a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
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(a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
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COMSOL Inc 2d flow velocity and 3d electrical field simulations comsol multiphysics v5.4
(a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL <t>Multiphysics,</t> this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.
2d Flow Velocity And 3d Electrical Field Simulations Comsol Multiphysics V5.4, 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): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL Multiphysics, this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.

Journal: Scientific Reports

Article Title: Inverse designed aperiodic multilayer perfect absorbers for mid infrared enable tunability switchability and angular robustness

doi: 10.1038/s41598-025-99995-6

Figure Lengend Snippet: (a): Simulated using the finite-difference time-domain (FDTD) method, this plot shows the normalized electric field intensity along the z-direction for multiple values of graphene chemical potential (µc = 0 to 1 eV). The simulation domain includes the air region above the structure, which allows visualization of both external and internal field behavior. At µc = 0.0 eV, where the structure is optimized for maximum absorption, the electric field in the air remains nearly constant, exhibiting an almost flat profile. This behavior indicates excellent impedance matching at the air-absorber interface, with negligible reflection—a hallmark of perfect absorption. As µc increases, the field confinement inside the multilayer weakens, confirming the switchable nature of the absorber.(b): Simulated using COMSOL Multiphysics, this panel shows the spatial distribution of the electric field inside the structure for two states: µc = 0 eV, with strong field localization, and µc = 1 eV, where the internal field intensity is significantly reduced. This independently confirms the tunable suppression of absorption and the modulation of plasmonic resonances in the multilayer stack.

Article Snippet: To further validate these findings, Fig. (b) presents 2D electric field maps simulated using COMSOL Multiphysics for two representative chemical potentials: μc = 0 eV (top) and μc = 1 eV (bottom).

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