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COMSOL Inc finite element electric field simulation
Finite Element Electric Field Simulation, 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/simulated+electric+fields/finite+element+electrostatic+simulation/pm40501443-113-4-3
Average 90 stars, based on 1 article reviews
finite element electric field simulation - by Bioz Stars, 2026-09
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Article Title: Multi-Functional Additive with Triple Regulation Mechanisms for Long-Life Zinc-Ion Batteries.
Article Snippet: Aqueous zinc-ion batteries (ZIBs) have attracted significant interest due to their low cost and high safety.. The lifetime of ZIBs is highly associated with several critical factors, including dendrite growth, hydrogen evolution reactions (HER), and irreversible parasitic reactions.. Although the adoption of electrolyte additives can greatly mitigate such issues, the fundamental regulation mechanisms remain unclear.

Article Title: Interfacial charge transfer enhancement via formation of binary molecular assemblies on electronically corrugated boron nitride.
Article Snippet: An intriguing question remains to be addressed, i.e., why F16ZnPc molecules charge more in the binary superstructure than in its Fig. 3 Finite element electrostatic simulations using COMSOL. (a) 2D representation of the geometric setup of the simulation. (b) Schematic illustration of the charge state of F16ZnPc molecules in its pure layer (left) and the mixed binary blend (right), respectively. (c) Electrostatic potential energy for electrons is plotted from the image charge plane of the metal up to 100 angstroms directly above the ZnPc molecule near the center of the binary molecular assembly.

Article Title: Confinement Related Phenomena in MoS 2 Tubular Structures Grown from Vapour Phase
Article Snippet: The results were in good agreement with electrostatic finite element method simulations using COMSOL.

Article Title: Anisotropic resistance with a 90° twist in a ferromagnetic Weyl semimetal, Co 2 MnGa.
Article Snippet: A discussion of the approaches we adopted to understand the measured {Rij,kl} is given in Section F of the SI.We derived themost insights from finite-element electrostatic simulations using COMSOL.

Article Title: Electrically Controlled Spin Injection from Giant Rashba Spin–Orbit Conductor BiTeBr
Article Snippet: To verify, we performed finite element electrostatic simulations, using COMSOL, on a simplified geometric model of a BiTeBr/graphene device, presented in Fig. S3.

Article Title: Anisotropic resistance with a 90° twist in a ferromagnetic Weyl semimetal, Co 2 MnGa
Article Snippet: We derived the most insights from finite-element electrostatic simulations using COMSOL.

Micro-CT:

Article Title: Self-Limiting Electrospray Deposition for the Surface Modification of Additively Manufactured Parts.
Article Snippet: Electrospray deposition (ESD) is a spray coating process that utilizes a high voltage to atomize a flowing solution into charged microdroplets.. These self-repulsive droplets evaporate as they travel to a target substrate, depositing the solution solids.. Our previous research investigated the conditions necessary to minimize charge dissipation and deposit a thickness-limited film that grows in area over time through self-limiting electrospray deposition.

Produced:

Article Title: Atomic-like charge qubit in a carbon nanotube enabling electric and magnetic field nano-sensing
Article Snippet: .. We can determine the spatial distribution of the potential produced by each one of the gates,using finite element electrostatic simulations (Comsol) (Supplementary Fig. 4a). ..



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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 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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