Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions

The microwave properties of epoxy composites filled with 30 wt.% of BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> (0.1 ≤ <i>x</i> ≤ 1.2) and with 1 wt.% of multi-walled carbon nanotubes (CNTs) were investigated i...

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Main Authors: Olena S. Yakovenko, Lyudmila Yu. Matzui, Ludmila L. Vovchenko, Victor V. Oliynyk, Volodymyr V. Zagorodnii, Sergei V. Trukhanov, Alex V. Trukhanov
Format: Article
Language:English
Published: MDPI AG 2021-10-01
Series:Nanomaterials
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Online Access:https://www.mdpi.com/2079-4991/11/11/2873
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author Olena S. Yakovenko
Lyudmila Yu. Matzui
Ludmila L. Vovchenko
Victor V. Oliynyk
Volodymyr V. Zagorodnii
Sergei V. Trukhanov
Alex V. Trukhanov
author_facet Olena S. Yakovenko
Lyudmila Yu. Matzui
Ludmila L. Vovchenko
Victor V. Oliynyk
Volodymyr V. Zagorodnii
Sergei V. Trukhanov
Alex V. Trukhanov
author_sort Olena S. Yakovenko
collection DOAJ
description The microwave properties of epoxy composites filled with 30 wt.% of BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> (0.1 ≤ <i>x</i> ≤ 1.2) and with 1 wt.% of multi-walled carbon nanotubes (CNTs) were investigated in the frequency range 36–55 GHz. A sufficient increase in the microwave shielding efficiency was found for ternary 1 wt.%CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites compared with binary 1% CNT/epoxy and 30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy due to the complementary contributions of dielectric and magnetic losses. Thus, the addition of only 1 wt.% of CNTs along with 30 wt.% of barium hexaferrite into epoxy resin increased the frequency range where electromagnetic radiation is intensely attenuated. A correlation between the cation Ga<sup>3+</sup> concentration in the BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> filler and amplitude–frequency characteristics of the natural ferromagnetic resonance (NFMR) in 1 wt.%CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites was determined. Higher values of the resonance frequency <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> (51.8–52.4 GHz) and weaker dependence of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> on the Ga<sup>3+</sup> concentration were observed compared with pressed polycrystalline BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> = 49.6–50.4 GHz). An increase in the NFMR amplitude on the applied magnetic field for both random and aligned 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites was found. The frequency of NFMR was approximately constant in the range of the applied magnetic field, H = 0–5 kOe, for the random 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composite, and it slightly increased for the aligned 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composite.
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spelling doaj.art-99e23e8a44454ad5af4b136eb9714bda2023-11-23T00:39:42ZengMDPI AGNanomaterials2079-49912021-10-011111287310.3390/nano11112873Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler DistributionsOlena S. Yakovenko0Lyudmila Yu. Matzui1Ludmila L. Vovchenko2Victor V. Oliynyk3Volodymyr V. Zagorodnii4Sergei V. Trukhanov5Alex V. Trukhanov6Physics Department, Taras Shevchenko National University of Kyiv, Volodymyrska Str. 64/13, 01601 Kyiv, UkrainePhysics Department, Taras Shevchenko National University of Kyiv, Volodymyrska Str. 64/13, 01601 Kyiv, UkrainePhysics Department, Taras Shevchenko National University of Kyiv, Volodymyrska Str. 64/13, 01601 Kyiv, UkrainePhysics Department, Taras Shevchenko National University of Kyiv, Volodymyrska Str. 64/13, 01601 Kyiv, UkrainePhysics Department, Taras Shevchenko National University of Kyiv, Volodymyrska Str. 64/13, 01601 Kyiv, UkraineDepartment of Technology of Electronics Materials, National University of Science and Technology “MISiS”, Leninskii av., 4119049 Moscow, RussiaDepartment of Technology of Electronics Materials, National University of Science and Technology “MISiS”, Leninskii av., 4119049 Moscow, RussiaThe microwave properties of epoxy composites filled with 30 wt.% of BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> (0.1 ≤ <i>x</i> ≤ 1.2) and with 1 wt.% of multi-walled carbon nanotubes (CNTs) were investigated in the frequency range 36–55 GHz. A sufficient increase in the microwave shielding efficiency was found for ternary 1 wt.%CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites compared with binary 1% CNT/epoxy and 30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy due to the complementary contributions of dielectric and magnetic losses. Thus, the addition of only 1 wt.% of CNTs along with 30 wt.% of barium hexaferrite into epoxy resin increased the frequency range where electromagnetic radiation is intensely attenuated. A correlation between the cation Ga<sup>3+</sup> concentration in the BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> filler and amplitude–frequency characteristics of the natural ferromagnetic resonance (NFMR) in 1 wt.%CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites was determined. Higher values of the resonance frequency <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> (51.8–52.4 GHz) and weaker dependence of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> on the Ga<sup>3+</sup> concentration were observed compared with pressed polycrystalline BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub> (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>f</mi><mrow><mi>r</mi><mi>e</mi><mi>s</mi></mrow></msub></mrow></semantics></math></inline-formula> = 49.6–50.4 GHz). An increase in the NFMR amplitude on the applied magnetic field for both random and aligned 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composites was found. The frequency of NFMR was approximately constant in the range of the applied magnetic field, H = 0–5 kOe, for the random 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composite, and it slightly increased for the aligned 1 wt.% CNT/30 wt.% BaFe<sub>12–<i>x</i></sub>Ga<i><sub>x</sub></i>O<sub>19</sub>/epoxy composite.https://www.mdpi.com/2079-4991/11/11/2873doped M-type hexaferritescarbon-based magnetodielectric nanocompositesmicrowave propertiesnatural ferromagnetic resonanceresonance frequency
spellingShingle Olena S. Yakovenko
Lyudmila Yu. Matzui
Ludmila L. Vovchenko
Victor V. Oliynyk
Volodymyr V. Zagorodnii
Sergei V. Trukhanov
Alex V. Trukhanov
Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
Nanomaterials
doped M-type hexaferrites
carbon-based magnetodielectric nanocomposites
microwave properties
natural ferromagnetic resonance
resonance frequency
title Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
title_full Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
title_fullStr Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
title_full_unstemmed Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
title_short Electromagnetic Properties of Carbon Nanotube/BaFe<sub>12−x</sub>Ga<sub>x</sub>O<sub>19</sub>/Epoxy Composites with Random and Oriented Filler Distributions
title_sort electromagnetic properties of carbon nanotube bafe sub 12 x sub ga sub x sub o sub 19 sub epoxy composites with random and oriented filler distributions
topic doped M-type hexaferrites
carbon-based magnetodielectric nanocomposites
microwave properties
natural ferromagnetic resonance
resonance frequency
url https://www.mdpi.com/2079-4991/11/11/2873
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