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2d axisymmetric model in comsol multiphysics 5.6  (COMSOL Inc)

 
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    COMSOL Inc 2d axisymmetric model in comsol multiphysics 5.6
    2d Axisymmetric Model In Comsol Multiphysics 5.6, 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+multiphysics/2d+axisymmetric+model+in+comsol+multiphysics+5+6/pm40649531-69-11-11
    Average 90 stars, based on 1 article reviews
    2d axisymmetric model in comsol multiphysics 5.6 - by Bioz Stars, 2026-10
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    Related Articles

    Diffusion-based Assay:

    Article Title: Biocompatible Core-Shell Microneedle Sensor Filled with Zwitterionic Polymer Hydrogel for Rapid Continuous Transdermal Monitoring.
    Article Snippet: .. Numerical simulation on glucose diffusion using COMSOL. (a) Three 2Daxisymmetric models used to simulate three hydrogel-assembly designs of off-skin, on MN, and in MN. (b) Set the initial concentration value to 0 and fix the bottom boundary concentration to 1mM. ..

    Concentration Assay:

    Article Title: Biocompatible Core-Shell Microneedle Sensor Filled with Zwitterionic Polymer Hydrogel for Rapid Continuous Transdermal Monitoring.
    Article Snippet: .. Numerical simulation on glucose diffusion using COMSOL. (a) Three 2Daxisymmetric models used to simulate three hydrogel-assembly designs of off-skin, on MN, and in MN. (b) Set the initial concentration value to 0 and fix the bottom boundary concentration to 1mM. ..

    other:

    Article Title: Programming Tactic Behaviors of Active Colloids via Surface Charge
    Article Snippet: To simulate the self-diffusiophoresis of Pt@SiO 2 in H 2 O 2 , we built a 2D axis-symmetric COMSOL model where one Janus particle, with 5 μm in diameter, is placed at the center of a cubic box with sides setting 100 μm.

    Article Title: Multi-Response Optimization of Aluminum Laser Spot Welding with Sinusoidal and Cosinusoidal Power Profiles Based on Taguchi-Grey Relational Analysis.
    Article Snippet: Laser spot welding was simulated using a 2D axisymmetric model in COMSOL Multiphysics 5.6, justified by the rotational symmetry of the stationary laser beam around the vertical z-axis.

    Article Title: Microwave Ablation Therapy for Hepatocellular Carcinoma: The Effect of Metabolic Heat on Temperature Distribution
    Article Snippet: Hepatocellular carcinoma is the main cause of liver cancer and one of the most occurring cancers worldwide.. Microwave Ablation (MWA) is a method to destroy cancer cells by heating tumours above 50°C.. Cancerous tissues can have high metabolic heat rates and affect temperature gain and distribution in thermal therapies.

    Emulsion:

    Article Title: A study of electrochemiluminescence mechanism of Rubrene/TPrA system in an aqueous solution via stochastic collision electrochemistry in an emulsion reactor.
    Article Snippet: • A new ECL mechanism of Rub/TPrA emulsion in an aqueous was raised and

    Formulation:

    Article Title: Numerical simulation of dynamic loss and total loss in the REBCO tapes under perpendicular AC magnetic fields up to 8 T at 20 K and 50 K
    Article Snippet: .. The 2D T‐A formulation finite element model is used to calculate Qm, Rdyn, and Qtotal of the REBCO tapes in COMSOL Multiphysics. ..



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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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    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: