Published at : 21 Apr 2020
Volume : IJtech
Vol 11, No 2 (2020)
DOI : https://doi.org/10.14716/ijtech.v11i2.2988
Erlina Yustanti | Department of Metallurgical Engineering, Faculty of Engineering, Sultan Ageng Tirtayasa University, Jl. Jenderal Sudirman KM 03 Cilegon, Banten 42435, Indonesia |
Adhitya Trenggono | Department of Metallurgical Engineering, Faculty of Engineering, Sultan Ageng Tirtayasa University, Jl. Jenderal Sudirman KM 03 Cilegon, Banten 42435, Indonesia |
Azwar Manaf | Department of Physics, Faculty of Mathematics and Natural Science, Universitas Indonesia, Kampus UI Depok, Depok 16424, Indonesia |
Barium hexaferrite (BHF) with the chemical
formula BaFe12O19 is a well-known permanent magnet and is
still primarily used in various electrical devices. Because of its excellent
magnetic properties, BHF is potentially one of the best candidates as a
microwave absorber. For this investigation, the magnetic and microwave
absorption characteristics of nanostructured BHF and BaFe9Mn1.5Ti1.5O19
were study. The high coercivity of BHF was substantially reduced through
Mn-Ti partial substitution for Fe atoms with a minor reduction of its
saturation magnetization. Nanostructured Mn-Ti–doped BHF was obtained through
particle size reduction with high-powered ultrasonic irradiation. After 12 h of ultrasonic irradiation, the mean
particle of BHF reduced to 61 nm from 380 nm, and the Mn-Ti–doped BHF reduced
from 545 nm to 95 nm. The mean crystallite size of the two samples was 15 and
18 nm, respectively. Hence, the particles of both samples contained only a few
crystallites. The characterization of reflection loss revealed that the highest
absorption value achieved by the nanostructured BaFe9Mn1.5Ti1.5O19 sample was 19.75 dB at 13.6 GHz, and approximately 90% of the intensity
of incoming electromagnetic waves was reduced by the material.
Barium hexaferrite; Mechanical alloying; Reflection loss; Ultrasonic irradiation
Barium hexaferrite (BHF) is a permanent magnetic material characterized by high values of coercivity, saturation magnetization, magnetic transition temperature, and corrosion resistance (Kerschl et al., 2002). The high value of saturation magnetization in BHF provides an opportunity for employing it in microwave absorption applications. However, its high coercivity must be reduced to some extent to facilitate the interaction between the magnetic field of electromagnetic waves and the magnetization of BHF. The reduced coercivity of Mn-Ti–substituted BHF was shown to increase microwave absorption (Manaf et al., 2017). Studies have shown that BaFe12-yMnyTiyO19 (y = 0.0; 0.5; 1.0; 1.5) with y = 1.5 was the best absorption up to a 40 dB reflection loss in 1–5 GHz (Priyono and Manaf, 2009). BHF as an electromagnetic wave absorber is widely used in many applications like information, communication using electronics components, and radar-absorbing material (Priyono and Manaf, 2009; Adi et al., 2017; Fitriana et al., 2017; Manaf et al., 2017).
Mechanical
alloying is a simple tool for the preparation of crystalline materials.
Mn-Ti–substituted BHF has been employed by several researchers to prepare
microwave absorption materials. Large crystallites resulting from mechanical
alloying can be further fragmented to smaller sizes of crystallites by means of
high-powered ultrasonic irradiation. There have been several methods available
for the fabrication of nanoparticles, including salt-assisted ultrasonic spray
pyrolysis (Hwan An et al., 2014), microwave-induced
combustion (Fu et al., 2003), ceramic
routing (Hessien et al., 2007),
microwave-hydrothermal (Sadhana et al., 2012),
and citrate sol–gel combustion routing (Sözeri et
al., 2012). Mechanical alloying has some advantages: it is a simple
technique, produces waste-free material, and can be implemented on a large
scale.
In terms of magnetic properties, remanence and
coercivity are affected by crystallite size. Magnetic materials with
nanostructures allow the grain exchange interaction effect, resulting in
enhanced remanence and reduced coercivity (Manaf et
al., 1993). The effect is further beneficial for microwave absorption
applications since nanoscale crystallites have become a center for
electromagnetic wave scattering due to a high density of surfaces in the
material. A combination of high remanence and nanostructure would be a
potentially powerful source for electromagnetic wave absorption.
In
this work, we explored the potential of BHF and its physical effects on its
magnetic properties and microwave absorption characteristics. BHF-based
magnetic materials were fabricated through mechanical alloying combined with
high-powered ultrasonic irradiation. The material under study is BaFe9Mn1.5Ti1.5O19,
a selected composition from the BaFe12-yMnyTiyO19
(y = 0.0, 0.5, 1.0, and 1.5) series, which has been previously studied (Priyono and Manaf, 2009; Repi and Manaf, 2012; Manawan
et al., 2014). However, the focus of the current work of this
composition is to further explore its excellent absorption characteristics.
Ultrasonic irradiation treatment to the mechanically
alloyed BHF and BFMTO powders for 12 h resulted in monocrystalline powders with
mean sizes of 15 and 18 nm, respectively. The BHF sample with a mean
crystallite size of 15 nm allowed inter-grain exchange interaction, leading to
a remanence-to-saturation ratio value of greater than 0.5. The BFMTOU12 sample
with the mean crystallite size of 18 nm was characterized by a high RL value,
where almost 90% of the incoming EM wave intensity was absorbed by the
material.
Research work was funded by Sultan Ageng Tirtayasa
University. The authors are
grateful to the support of the Physics Department, Universitas Indonesia, for
the research facilities.
Filename | Description |
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R1-MME-2988-20200303231416.png | Figure 1(a) Diffraction pattern of BaO.6Fe2-xMnx2Tix2O3 x = 0 |
R1-MME-2988-20200303231613.png | Figure 1(b) Diffraction pattern of BaO.6Fe2-xMnx2Tix2O3 x = 0.5 |
R1-MME-2988-20200303231656.png | Figure 2 Shifting of XRD diffraction peaks due to Mn-Ti substitution |
R1-MME-2988-20200303231722.png | Figure 3(a) The particle size distribution of BHF after ultrasonic irradiation for 3 hours |
R1-MME-2988-20200303231752.png | Figure 3(b) The particle size distribution of BFMTO after ultrasonic irradiation for 3 hours |
R1-MME-2988-20200303231828.png | Figure 4(a) Effect of ultrasonic time on the reduction of particle size BHF |
R1-MME-2988-20200303231853.png | Figure 4(b) Effect of ultrasonic time on the reduction of particle size BFMTO |
R1-MME-2988-20200303232749.png | Figure 5 (a) SEM-FEI before ultrasonic irradiation |
R1-MME-2988-20200303232923.png | Figure 5 (b) TEM after 12 hours of ultrasonic irradiation |
R1-MME-2988-20200303233016.png | Figure 6(a) The loop hysteresis of BHF and BFMTO |
R1-MME-2988-20200303233042.png | Figure 6(b) Reflection loss value of BHF and BFMTO U12 in the frequency range 8-20 GHz |
R1-MME-2988-20200303233154.png | Figure 7 Schematic illustration of nanoparticle synthesis through mechanical milling and ultrasonic irradiation |
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