Abstract:Mechanically flexible butyl rubber–SrTiO3 composites were prepared through sigma mixing followed by hot pressing. Tensile tests established the mechanical flexibility of the composites. Swelling tests revealed the degree of matrix–filler interactions. The effect of SrTiO3 ceramic filler on the dielectric properties of the composites was studied at 1 MHz and 5 GHz using an LCR meter and a Split Post Dielectric Resonator, respectively. The relative permittivity of the composites increased with filler loading whi… Show more
“…Today elastomer-ceramic composites found applications ranging from ultrathin health monitoring to advanced imaging devices. Recently, we have reported the microwave dielectric properties of butyl rubber composites with SrTiO 3 ,SiO 2 , Ba(Zn 1/3 Ta 2/3 )O 3 and Sr 2 Ce 2 Ti 5 O 16 composites [13][14][15]. In the present paper we report the preparation, mechanical, thermal and microwave dielectric properties of butyl rubber with micron and nano barium titanate composites.…”
Butyl rubber-micron barium titanate (BR/BT) and butyl rubber-nano barium titanate (BR/nBT) composites were prepared by sigma mixing followed by hot pressing. The tensile tests show that both the composites were mechanically flexible. The microwave dielectric properties of both BR/BT and BR/nBT composites were investigated as a function of ceramic loading and were found to be improved with filler content. The butyl rubber has a relative permittivity (e r ) of 2.4 and loss tangent (tan d) of 0.0017 at 5 GHz. At a filler loading of 0.24 volume fraction (v f ) of micron sized barium titanate (BaTiO 3 ) powder loading, the composite attained a e r of 7 and tan d of 0.014 and for the same filler content of nano BaTiO 3 the composite have e r of 8.9 and tan d of 0.019 at 5 GHz. The thermal and mechanical properties of both the composites were investigated. The experimental values of e r of both BR/BT and BR/nBT composites for different volume fractions were compared with theoretical models.
“…Today elastomer-ceramic composites found applications ranging from ultrathin health monitoring to advanced imaging devices. Recently, we have reported the microwave dielectric properties of butyl rubber composites with SrTiO 3 ,SiO 2 , Ba(Zn 1/3 Ta 2/3 )O 3 and Sr 2 Ce 2 Ti 5 O 16 composites [13][14][15]. In the present paper we report the preparation, mechanical, thermal and microwave dielectric properties of butyl rubber with micron and nano barium titanate composites.…”
Butyl rubber-micron barium titanate (BR/BT) and butyl rubber-nano barium titanate (BR/nBT) composites were prepared by sigma mixing followed by hot pressing. The tensile tests show that both the composites were mechanically flexible. The microwave dielectric properties of both BR/BT and BR/nBT composites were investigated as a function of ceramic loading and were found to be improved with filler content. The butyl rubber has a relative permittivity (e r ) of 2.4 and loss tangent (tan d) of 0.0017 at 5 GHz. At a filler loading of 0.24 volume fraction (v f ) of micron sized barium titanate (BaTiO 3 ) powder loading, the composite attained a e r of 7 and tan d of 0.014 and for the same filler content of nano BaTiO 3 the composite have e r of 8.9 and tan d of 0.019 at 5 GHz. The thermal and mechanical properties of both the composites were investigated. The experimental values of e r of both BR/BT and BR/nBT composites for different volume fractions were compared with theoretical models.
“…SrTiO 3 , BaTiO 3 and CaTiO 3 ) have been extensively researched owning to their potential applications, such as capacitor, photo-corrosion, solar cell, sensor, superconductor and so on [9][10][11]. In particular, SrTiO 3 , as a member of perovskite structure materials family, has attracted increasing interest in dielectric properties and microwave absorption properties owing to its adjustable dielectric loss, low cost, and excellent temperature stability [12][13][14]. The most concerning advantage of such SrTiO 3 perovskite material is the exible chemical composition by A-or B-site doping, by which one can adjust the electronic states.…”
xAl 2 O 3-(1-x)Sr 0.85 Gd 0.15 TiO 3 (x=0.2, 0.3, 0.4, 0.5) ceramics were fabricated by hot-press sintering. Their morphology, phase composition, conductivity, dielectric properties as well as microwave absorption performance were examined by scanning electron microscopy (SEM), X-ray diffraction (XRD), multifunction digital four-probe meter and vector network analysis, respectively. The microwave absorption of as-prepared xAl 2 O 3-(1-x)Sr 0.85 Gd 0.15 TiO 3 ceramics demonstrates excellent microwave absorbability. It is unexpectedly found that with a thickness of only 0.346 mm, xAl 2 O 3-(1x)Sr 0.85 Gd 0.15 TiO 3 (x=0.2) ceramic exhibits an absorption bandwidth of 3.7 GHz (8.7-12.4 GHz), being consequential to re ection loss less than-10 dB (over 90% of microwave absorption). It is as well discovered that the minimum re ection loss and absorption peak frequency of xAl 2 O 3-(1x)Sr 0.85 Gd 0.15 TiO 3 (x=0.3) with a thickness of 0.436 mm were-45.43 dB and 11.3 GHz, respectively. The prominent microwave absorption performance of the ceramic with such a thin thickness can be attributed to strong interfacial polarization, dielectric frequency dispersion, and good electromagnetic impedance matching. It indicates that the xAl 2 O 3-(1-x)Sr 0.85 Gd 0.15 TiO 3 ceramics with appropriate Al 2 O 3 mass fraction and thickness showing good potential for effective microwave absorbing materials.
“…SrTiO 3 , BaTiO 3 and CaTiO 3 ) have been extensively researched owning to their potential applications, such as capacitor, photo-corrosion, solar cell, sensor, superconductor and so on [9][10][11]. In particular, SrTiO 3 , as a member of perovskite structure materials family, has attracted increasing interest in dielectric properties and microwave absorption properties owing to its adjustable dielectric loss, low cost, and excellent temperature stability [12][13][14]. The most concerning advantage of such SrTiO 3 perovskite material is the exible chemical composition by A-or B-site doping, by which one can adjust the electronic states.…”
xAl2O3-(1-x)Sr0.85Gd0.15TiO3(x=0.2, 0.3, 0.4, 0.5) ceramics were fabricated by hot-press sintering. Their morphology, phase composition, conductivity, dielectric properties as well as microwave absorption performance were examined by scanning electron microscopy (SEM), X-ray diffraction (XRD), multifunction digital four-probe meter and vector network analysis, respectively. The microwave absorption of as-prepared xAl2O3-(1-x)Sr0.85Gd0.15TiO3 ceramics demonstrates excellent microwave absorbability. It is unexpectedly found that with a thickness of only 0.346 mm, xAl2O3-(1-x)Sr0.85Gd0.15TiO3 (x=0.2) ceramic exhibits an absorption bandwidth of 3.7 GHz (8.7-12.4 GHz), being consequential to reflection loss less than -10 dB (over 90% of microwave absorption). It is as well discovered that the minimum reflection loss and absorption peak frequency of xAl2O3-(1-x)Sr0.85Gd0.15TiO3 (x=0.3) with a thickness of 0.436 mm were -45.43 dB and 11.3 GHz, respectively. The prominent microwave absorption performance of the ceramic with such a thin thickness can be attributed to strong interfacial polarization, dielectric frequency dispersion, and good electromagnetic impedance matching. It indicates that the xAl2O3-(1-x)Sr0.85Gd0.15TiO3 ceramics with appropriate Al2O3 mass fraction and thickness showing good potential for effective microwave absorbing materials.
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