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2d comsol simulations  (COMSOL Inc)

 
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    COMSOL Inc 2d comsol simulations
    2d Comsol Simulations, 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/comsol+multiphysics/10__1016_slash_j__snr__2024__100273-170-3-4
    Average 90 stars, based on 1 article reviews
    2d comsol simulations - by Bioz Stars, 2026-09
    90/100 stars

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    Related Articles

    Polymer:

    Article Title: Mechanistic computational modeling of implantable, bioresorbable, drug release systems.
    Article Snippet: .. The predicted drug release from the 2D COMSOL simulation (Figure 4i, solid grey line) and the stochastic 1D Python simulation (Figure 4i, solid blue line), both in the absence of polymer degradation, are compared to experimental data (Figure 4i, black markers) [16]. ..

    other:

    Article Title: Detection and identification of single ribonucleotide monophosphates using a dual in-plane nanopore sensor made in a thermoplastic via replication
    Article Snippet: As seen from , 3% of the fluidic circuit voltage drop occurred in the microchannels while 97% of the voltage drop occurred in the dual in-plane nanosensor region of this chip based on the physical dimensions of this chip (see Table S1 ). provides a 2D COMSOL simulation (see Table S1 for COMSOL variables) of the relative voltage drop around the nanopore.

    Article Title: Modeling of a Nonlinear Coupled Compliant Mechanism via Developed Kinematics-integrated Neural Network Algorithm
    Article Snippet: In order to collect the input-output data of the designed nanopositioner, a 2D COMSOL simulation has been created, where the parameter sweep method is adopted to have various data sets.

    Concentration Assay:

    Article Title: Non-contact photoacoustic imaging with a silicon photonics-based Laser Doppler Vibrometer
    Article Snippet: .. Fig. 4 2D COMSOL simulation of acoustic propagation in a geometry similar to Fig. e for an initial pressure distribution with increased pressure inside the tube filled with a water-based solution surrounded by PDMS at ( a ) \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t=0~\mu s$$\end{document} t = 0 μ s , ( b ) \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t=5~\mu s$$\end{document} t = 5 μ s and ( c ) \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$t=9~\mu s$$\end{document} t = 9 μ s . While the results from Fig. were obtained using a 1 % ink concentration, resulting in an absorption coefficient well above the physiological range, Fig. a demonstrates the dependence of the amplitude of the photoacoustic signals on the absorption of the ink solution. ..



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    Image Search Results


    (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).

    Techniques: