Controllable Preparation of Fe3O4@RF and Its Evolution to Yolk–Shell-Structured Fe@C Composite Microspheres with High Microwave Absorbing Performance

Abstract

Fe3O4@RF microspheres with different phenolic (RF) layer thicknesses are prepared by adjusting the polymerization time. With the prepared Fe3O4@RF as the precursor, Fe@C composite microspheres with rattle-like morphology are obtained through one-step controlled carbonization. This method simplifies the preparation of rattle-shaped microspheres from sandwich microspheres. Fe@C microspheres exhibit excellent microwave absorbing properties. The morphology and composition of the product are investigated depending on the effects of carbonization temperature, time and thickness of the RF layer. When the carbonization temperature is 700 °C, the carbonization time is 12 h and the polymer shell thickness is 62 nm, the inner hollow Fe3O4 is completely reduced to Fe. The absorption properties of the materials are compared before and after the reduction of Fe3O4. Both Fe@C-12 and Fe3O4@C-700 show excellent absorbing properties. When the filler content is 50%, the maximum reflection loss (RLmax) of the rattle-shaped Fe@C microspheres is −50.15 dB, and the corresponding matching thickness is 3.5 mm. At a thickness of 1.7 mm, the RLmax of Fe3O4@C-700 is −44.42 dB, which is slightly worse than that of Fe@C-12. Both dielectric loss and magnetic loss play a vital role in electromagnetic wave absorption. This work prepares rattle-shaped absorbing materials in a simple way, which has significance for guiding the construction of rattle-shaped materials.

Flexible MWCNT/PVA/Mn Ferrite/AC Metacomposites with Tunable Negative Permittivity for Low-Frequency Reflectors and Optical Sensors

“…The reflection loss (RL) value can be used to assess the reflectance qualities of metacomposites. According to the transmission line theory, the RLs of the metacomposites were calculated from the measured relative complex permittivity and permeability values by the following equations − RL = 20 nobreak0em0.1em⁡ log | ( Z in − Z 0 ) ( Z in + Z 0 ) | Z in = Z 0 μ r / ε r nobreak0em0.1em⁡ tan nobreak0em0.25em⁡ normalh [ j false( 2 π italicfd / c false) μ normalr ε normalr ] where Z in is the input impedance of the absorber, μ r and ε r are relative complex permeability and permittivity, respectively, c is the velocity of light in vacuum, f is the frequency of electromagnetic wave, and d is the thickness of the reflector. In Figure , the calculated RL for the metacomposites at a thickness of 1 mm is displayed.…”

Tunable Negative Permittivity Derived From Flexible MWCNT/PVA/Mn Ferrite/AC Metacomposites

“…According to the transmission line theory, the RL of the metacomposites were calculated from the measured relative complex permittivity and permeability values by the following equations [50][51][52]:…”

MWCNT/CuO/Fe3O4/Polyaniline Nanocomposites with Remarkable Microwave Attenuation and Broad Frequency Band by Tuned Composition

“…ε values of all samples of nanocomposites, almost are the same. In our composite, ε was resulted from several factors: (i) charge accumulation created at the interface of CuO and Fe 3 O 4 in hybrid form, CuO or Fe 3 O 4 single form, and polyaniline, CuO/Fe 3 O 4 and polyaniline, polyaniline and CNT [33,34]. Dispersion of nanoparticles within the polymer leads greatly to increase joint surface of the nanoparticles with the polymer.…”