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finite element electromagnetic simulation comsol multiphysics 5.4  (COMSOL Inc)

 
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    COMSOL Inc finite element electromagnetic simulation comsol multiphysics 5.4
    Schematics of the (A) single-metalized (without photoexcitation) and (B) double-metalized (with photoexcitation) waveguides. (C) Dispersion curves of transverse magnetic (TM) and transverse <t>electromagnetic</t> (TEM) modes in the single- and double-metalized waveguides. In this analysis, the thickness of the waveguide is d = 100 μm, and the relative permittivity of GaAs is ɛ s = 12.96. The input and output frequencies observed in the experiment are plotted using red and black markers, respectively; the circles, squares, and triangles correspond to the frequency conversion for input frequencies of 0.35, 0.42, and 0.48 THz, respectively. (D) Energy efficiency of the frequency conversion T l from the lowest TM mode in the single-metalized waveguide to the TEM ( l = 0) and TM ( l = 1) modes in the double-metalized waveguide.
    Finite Element Electromagnetic Simulation Comsol Multiphysics 5.4, 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
    https://www.bioz.com/product/multiphysics+finite+element+simulation+program+comsol+multiphysics/pmc11501523-182-22-25?v=COMSOL+Inc
    Average 90 stars, based on 1 article reviews
    finite element electromagnetic simulation comsol multiphysics 5.4 - by Bioz Stars, 2026-06
    90/100 stars

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    1) Product Images from "Frequency down-conversion of terahertz waves at optically induced temporal boundaries in GaAs waveguides"

    Article Title: Frequency down-conversion of terahertz waves at optically induced temporal boundaries in GaAs waveguides

    Journal: Nanophotonics

    doi: 10.1515/nanoph-2024-0010

    Schematics of the (A) single-metalized (without photoexcitation) and (B) double-metalized (with photoexcitation) waveguides. (C) Dispersion curves of transverse magnetic (TM) and transverse electromagnetic (TEM) modes in the single- and double-metalized waveguides. In this analysis, the thickness of the waveguide is d = 100 μm, and the relative permittivity of GaAs is ɛ s = 12.96. The input and output frequencies observed in the experiment are plotted using red and black markers, respectively; the circles, squares, and triangles correspond to the frequency conversion for input frequencies of 0.35, 0.42, and 0.48 THz, respectively. (D) Energy efficiency of the frequency conversion T l from the lowest TM mode in the single-metalized waveguide to the TEM ( l = 0) and TM ( l = 1) modes in the double-metalized waveguide.
    Figure Legend Snippet: Schematics of the (A) single-metalized (without photoexcitation) and (B) double-metalized (with photoexcitation) waveguides. (C) Dispersion curves of transverse magnetic (TM) and transverse electromagnetic (TEM) modes in the single- and double-metalized waveguides. In this analysis, the thickness of the waveguide is d = 100 μm, and the relative permittivity of GaAs is ɛ s = 12.96. The input and output frequencies observed in the experiment are plotted using red and black markers, respectively; the circles, squares, and triangles correspond to the frequency conversion for input frequencies of 0.35, 0.42, and 0.48 THz, respectively. (D) Energy efficiency of the frequency conversion T l from the lowest TM mode in the single-metalized waveguide to the TEM ( l = 0) and TM ( l = 1) modes in the double-metalized waveguide.

    Techniques Used: Dispersion



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    <t>Finite</t> <t>element</t> <t>simulation</t> results of the sensor operation. ( a ) Stress imposed on the bladder by the sensor with different Young’s modulus; ( b ) Maximum gap distance between two electrodes to form an electric contact when the volume changes from 800 mL to 400 mL.
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    Finite element simulation results of the sensor operation. ( a ) Stress imposed on the bladder by the sensor with different Young’s modulus; ( b ) Maximum gap distance between two electrodes to form an electric contact when the volume changes from 800 mL to 400 mL.

    Journal: Sensors (Basel, Switzerland)

    Article Title: Polypyrrole/Agarose Hydrogel-Based Bladder Volume Sensor with a Resistor Ladder Structure

    doi: 10.3390/s18072288

    Figure Lengend Snippet: Finite element simulation results of the sensor operation. ( a ) Stress imposed on the bladder by the sensor with different Young’s modulus; ( b ) Maximum gap distance between two electrodes to form an electric contact when the volume changes from 800 mL to 400 mL.

    Article Snippet: To investigate the effects of various design parameters, we simulated the operation of the proposed structure using a commercial finite element simulation program (COMSOL Multiphysics ® , Burlington, MA, USA).

    Techniques: