Construction of Ti

To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by v...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Wang, Zhenjun [verfasserIn] Xu, Zhiwang [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth

Übergeordnetes Werk:	Enthalten in: Journal of industrial and engineering chemistry - Seoul : KSIEC, 1995, 116, Seite 257-267
Übergeordnetes Werk:	volume:116 ; pages:257-267

DOI / URN:	10.1016/j.jiec.2022.09.016

Katalog-ID:	ELV008663246

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520			\|a To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material.
650		4	\|a Electromagnetic wave absorption
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773	0	8	\|i Enthalten in \|t Journal of industrial and engineering chemistry \|d Seoul : KSIEC, 1995 \|g 116, Seite 257-267 \|w (DE-627)391337238 \|w (DE-600)2152565-1 \|w (DE-576)28474784X \|x 1226-086X \|7 nnns
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publishDate	2022
allfields	10.1016/j.jiec.2022.09.016 doi (DE-627)ELV008663246 (ELSEVIER)S1226-086X(22)00500-7 DE-627 ger DE-627 rda eng 600 540 DE-600 Wang, Zhenjun verfasserin aut Construction of Ti 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material. Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth Xu, Zhiwang verfasserin aut Enthalten in Journal of industrial and engineering chemistry Seoul : KSIEC, 1995 116, Seite 257-267 (DE-627)391337238 (DE-600)2152565-1 (DE-576)28474784X 1226-086X nnns volume:116 pages:257-267 GBV_USEFLAG_U SYSFLAG_U GBV_ELV SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 AR 116 257-267
spelling	10.1016/j.jiec.2022.09.016 doi (DE-627)ELV008663246 (ELSEVIER)S1226-086X(22)00500-7 DE-627 ger DE-627 rda eng 600 540 DE-600 Wang, Zhenjun verfasserin aut Construction of Ti 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material. Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth Xu, Zhiwang verfasserin aut Enthalten in Journal of industrial and engineering chemistry Seoul : KSIEC, 1995 116, Seite 257-267 (DE-627)391337238 (DE-600)2152565-1 (DE-576)28474784X 1226-086X nnns volume:116 pages:257-267 GBV_USEFLAG_U SYSFLAG_U GBV_ELV SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 AR 116 257-267
allfields_unstemmed	10.1016/j.jiec.2022.09.016 doi (DE-627)ELV008663246 (ELSEVIER)S1226-086X(22)00500-7 DE-627 ger DE-627 rda eng 600 540 DE-600 Wang, Zhenjun verfasserin aut Construction of Ti 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material. Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth Xu, Zhiwang verfasserin aut Enthalten in Journal of industrial and engineering chemistry Seoul : KSIEC, 1995 116, Seite 257-267 (DE-627)391337238 (DE-600)2152565-1 (DE-576)28474784X 1226-086X nnns volume:116 pages:257-267 GBV_USEFLAG_U SYSFLAG_U GBV_ELV SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 AR 116 257-267
allfieldsGer	10.1016/j.jiec.2022.09.016 doi (DE-627)ELV008663246 (ELSEVIER)S1226-086X(22)00500-7 DE-627 ger DE-627 rda eng 600 540 DE-600 Wang, Zhenjun verfasserin aut Construction of Ti 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material. Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth Xu, Zhiwang verfasserin aut Enthalten in Journal of industrial and engineering chemistry Seoul : KSIEC, 1995 116, Seite 257-267 (DE-627)391337238 (DE-600)2152565-1 (DE-576)28474784X 1226-086X nnns volume:116 pages:257-267 GBV_USEFLAG_U SYSFLAG_U GBV_ELV SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 AR 116 257-267
allfieldsSound	10.1016/j.jiec.2022.09.016 doi (DE-627)ELV008663246 (ELSEVIER)S1226-086X(22)00500-7 DE-627 ger DE-627 rda eng 600 540 DE-600 Wang, Zhenjun verfasserin aut Construction of Ti 2022 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material. Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth Xu, Zhiwang verfasserin aut Enthalten in Journal of industrial and engineering chemistry Seoul : KSIEC, 1995 116, Seite 257-267 (DE-627)391337238 (DE-600)2152565-1 (DE-576)28474784X 1226-086X nnns volume:116 pages:257-267 GBV_USEFLAG_U SYSFLAG_U GBV_ELV SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 AR 116 257-267
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author	Wang, Zhenjun
spellingShingle	Wang, Zhenjun ddc 600 misc Electromagnetic wave absorption misc Nanocomposite misc Effective absorption bandwidth Construction of Ti
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topic_title	600 540 DE-600 Construction of Ti Electromagnetic wave absorption Nanocomposite Effective absorption bandwidth
topic	ddc 600 misc Electromagnetic wave absorption misc Nanocomposite misc Effective absorption bandwidth
topic_unstemmed	ddc 600 misc Electromagnetic wave absorption misc Nanocomposite misc Effective absorption bandwidth
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title	Construction of Ti
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title_full	Construction of Ti
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doi_str_mv	10.1016/j.jiec.2022.09.016
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title_sort	construction of ti
title_auth	Construction of Ti
abstract	To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material.
abstractGer	To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material.
abstract_unstemmed	To obtain the high-efficiency electromagnetic (EM) wave absorber, two-dimensional layered Ti3C2Tx/Co spheres/TiO2 nanocomposite powders were prepared by heat treatment, and the samples were characterized and analyzed by SEM, XRD and XPS. The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. It was proved that Ti3C2Tx/Co sphere/TiO2 nanocomposite is a very promising electromagnetic wave absorbing material.
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title_short	Construction of Ti
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doi_str	10.1016/j.jiec.2022.09.016
up_date	2024-07-06T20:28:25.760Z
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The electromagnetic parameters of the samples were tested by vector network analyzer and the reflection loss values (RL) of the samples were simulated and calculated at different coating thicknesses. The results showed that the mass content of TiO2 in the samples increased with the increase of heat treatment temperature; when the heat treatment temperature is 400 °C, the RL of the sample reaches −45.7 dB at 7 GHz with a coating thickness of 3 mm, and the effective absorption bandwidth is as high as 10 GHz (3 ∼ 5 GHz, 10 ∼ 18 GHz) at 4 mm. Finally,electromagnetic wave absorption mechanism of Ti3C2Tx/Co spheres/TiO2 nanocomposites was analyzed. 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