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saw modes and acoustic pressure comsol simulation results of the multilayer structure  (COMSOL Inc)

 
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    COMSOL Inc saw modes and acoustic pressure comsol simulation results of the multilayer structure
    Saw Modes And Acoustic Pressure Comsol Simulation Results Of The Multilayer Structure, 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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    Average 90 stars, based on 1 article reviews
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    COMSOL Inc saw modes and acoustic pressure comsol simulation results of the multilayer structure
    a The model constructed for molecular dynamic simulations featuring PEI polymer wetted by Al 2 O 3 layers (left), and the corresponding diffusion coefficient ( D ) of PEI polymer chains at different positions from the bottom to top Al 2 O 3 surfaces. b The diffusion coefficient of PEI polymer chains as a function of temperature. c Variation of T g for confined PEI with different film thicknesses, the thickness of the Al 2 O 3 layers is fixed at 28 nm. The error bars (±1 °C) represent the inherent error due to the fitting of the data required to obtain T g . d , e Variations of d Young’s modulus and e resistivity for PEI-Al 2 O 3 <t>nanolaminates</t> with different PEI thicknesses at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm. f Dependency of breakdown strength on PEI film thickness for PEI-Al 2 O 3 nanolaminates at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm.
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    a The model constructed for molecular dynamic simulations featuring PEI polymer wetted by Al 2 O 3 layers (left), and the corresponding diffusion coefficient ( D ) of PEI polymer chains at different positions from the bottom to top Al 2 O 3 surfaces. b The diffusion coefficient of PEI polymer chains as a function of temperature. c Variation of T g for confined PEI with different film thicknesses, the thickness of the Al 2 O 3 layers is fixed at 28 nm. The error bars (±1 °C) represent the inherent error due to the fitting of the data required to obtain T g . d , e Variations of d Young’s modulus and e resistivity for PEI-Al 2 O 3 nanolaminates with different PEI thicknesses at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm. f Dependency of breakdown strength on PEI film thickness for PEI-Al 2 O 3 nanolaminates at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm.

    Journal: Nature Communications

    Article Title: High-temperature capacitive energy stroage in polymer nanocomposites through nanoconfinement

    doi: 10.1038/s41467-024-51052-y

    Figure Lengend Snippet: a The model constructed for molecular dynamic simulations featuring PEI polymer wetted by Al 2 O 3 layers (left), and the corresponding diffusion coefficient ( D ) of PEI polymer chains at different positions from the bottom to top Al 2 O 3 surfaces. b The diffusion coefficient of PEI polymer chains as a function of temperature. c Variation of T g for confined PEI with different film thicknesses, the thickness of the Al 2 O 3 layers is fixed at 28 nm. The error bars (±1 °C) represent the inherent error due to the fitting of the data required to obtain T g . d , e Variations of d Young’s modulus and e resistivity for PEI-Al 2 O 3 nanolaminates with different PEI thicknesses at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm. f Dependency of breakdown strength on PEI film thickness for PEI-Al 2 O 3 nanolaminates at various temperatures, the thickness of the Al 2 O 3 layers is fixed at 28 nm.

    Article Snippet: The cross-sectional morphology of multilayer structured nanolaminates was characterized with scanning electron microscopy (JSM-7610FPlus, JEOL, Japan).

    Techniques: Construct, Polymer, Diffusion-based Assay

    a Cross-section SEM images of nanolaminates with varying layers and interlayer PEI thickness of 10 nm. The pink region represents Al 2 O 3 , and the blue region represents PEI. The scale bar is 50 nm for all. b Leakage current densities of nanolaminates with varying layers as a function of an electric field at 200 °C. c KPFM maps of the normalized contact potential difference (CPD) of nanolaminates with varying layers. From top to bottom, ~30 s, ~1 min, ~2 min, ~3 min, ~4 min, ~5 min, ~7 min, ~9 min, ~11 min after applying a 20 V voltage at the surface of the samples. The scale bar is 1 μm. d Simulated evolution of volume fraction of breakdown phase for different multilayered nanolaminates. e Failure probability of breakdown strength deduced from Weibull distribution for nanolaminates with varying layers at 25, 150, and 200 °C, respectively.

    Journal: Nature Communications

    Article Title: High-temperature capacitive energy stroage in polymer nanocomposites through nanoconfinement

    doi: 10.1038/s41467-024-51052-y

    Figure Lengend Snippet: a Cross-section SEM images of nanolaminates with varying layers and interlayer PEI thickness of 10 nm. The pink region represents Al 2 O 3 , and the blue region represents PEI. The scale bar is 50 nm for all. b Leakage current densities of nanolaminates with varying layers as a function of an electric field at 200 °C. c KPFM maps of the normalized contact potential difference (CPD) of nanolaminates with varying layers. From top to bottom, ~30 s, ~1 min, ~2 min, ~3 min, ~4 min, ~5 min, ~7 min, ~9 min, ~11 min after applying a 20 V voltage at the surface of the samples. The scale bar is 1 μm. d Simulated evolution of volume fraction of breakdown phase for different multilayered nanolaminates. e Failure probability of breakdown strength deduced from Weibull distribution for nanolaminates with varying layers at 25, 150, and 200 °C, respectively.

    Article Snippet: The cross-sectional morphology of multilayer structured nanolaminates was characterized with scanning electron microscopy (JSM-7610FPlus, JEOL, Japan).

    Techniques:

    a Discharged energy density and efficiency of nanolaminates with varying layers at temperatures of 150, 200, and 250 °C. b Comparison of maximum discharged energy density achieved at above 90% efficiency in this work and previously reported values at different temperatures. c Cyclic stability of energy density and energy efficiency for 7-layered nanolaminate under 700 kV/mm at various temperatures.

    Journal: Nature Communications

    Article Title: High-temperature capacitive energy stroage in polymer nanocomposites through nanoconfinement

    doi: 10.1038/s41467-024-51052-y

    Figure Lengend Snippet: a Discharged energy density and efficiency of nanolaminates with varying layers at temperatures of 150, 200, and 250 °C. b Comparison of maximum discharged energy density achieved at above 90% efficiency in this work and previously reported values at different temperatures. c Cyclic stability of energy density and energy efficiency for 7-layered nanolaminate under 700 kV/mm at various temperatures.

    Article Snippet: The cross-sectional morphology of multilayer structured nanolaminates was characterized with scanning electron microscopy (JSM-7610FPlus, JEOL, Japan).

    Techniques: Comparison