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.2018 Oct 8;3(10):12813-12823.
doi: 10.1021/acsomega.8b01477. eCollection 2018 Oct 31.

Dielectric Properties for Nanocomposites Comparing Commercial and Synthetic Ni- and Fe3O4-Loaded Polystyrene

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Dielectric Properties for Nanocomposites Comparing Commercial and Synthetic Ni- and Fe3O4-Loaded Polystyrene

Parth N Vakil et al. ACS Omega..

Abstract

Nanomaterial-loaded thermoplastics are attractive for applications in adaptive printing methods, as the physical properties of the printed materials are dependent on the nanomaterial type and degree of dispersion. This study compares the dispersion and the impact on the dielectric properties of two common nanoparticles, nickel and iron oxide, loaded into polystyrene. Comparisons between commercial and synthetically prepared samples indicate that well-passivated synthetically prepared nanomaterials are dispersed and minimize the impact on the dielectric properties of the host polymer by limiting particle-particle contacts. Commercial samples were observed to phase-segregate, leading to the loss of the low-k performance of polystyrene. The change in the real and imaginary dielectric was systematically studied in two earth abundant nanoparticles at the concentration between 0 and 13 vol % (0-50 wt %). By varying the volume percentage of fillers in the matrix, it is shown that one can increase the magnetic properties of the materials while minimizing unwanted contributions to the dielectric constant and dielectric loss. The well-dispersed nanoparticle systems were successfully modeled through the Looyenga dielectric theory, thus giving one a predictive ability for the dielectric properties. The current experimental work coupled with modeling could facilitate future material choices and guide design rules for printable polymer composite systems.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1
Figure 1
TEM sizeand size distribution of (A) com-Fe3O4, (B)com-Ni, (C) syn-Fe3O4, and (D) syn-Ninanoparticles. A disk of the formed composite used in dielectric spectroscopyis shown (inset).
Figure 2
Figure 2
I vsq SAXS data for the (A)lowest loading of Fe3O4 (com vs syn), (B) highestloading of Fe3O4 (com vs syn), (C) lowest loadingof Ni (com vs syn), and (D) highest loading of Ni (com vs syn).
Figure 3
Figure 3
Fe Kα SEM–EDS map and line profilescans of nanocompositedisks in various regions for (A) com-Fe3O4 and(B) syn-Fe3O4. Dashed white lines at the edgesindicate the boundaries of the samples.
Figure 4
Figure 4
Ni Kα SEM–EDS map and line profile scans of pressednanocomposite samples for all volume fractions of (A) com-Ni and (B)syn-Ni obtained using EDS analysis. Dashed white lines at the edgesindicate the boundaries of the samples.
Figure 5
Figure 5
Frequency-dependent dielectric measurements (0.1 Hz to 1 MHz) ofthe real permittivity (ε′) of (A) com-Fe3O4, (B) syn-Fe3O4, (C) com-Ni, and (D)syn-Ni nanocomposites at different particle loadings.
Figure 6
Figure 6
Real permittivity (ε′) of different nanocompositesamples as a function of volume fraction of particles (vf). Experimental data are the solid symbols, whereas thedashed lines are fits of the Looyenga model to the data. (A) com-Fe3O4, (B) syn-Fe3O4, (C) com-Ni,and (D) syn-Ni nanocomposites.
Figure 7
Figure 7
Frequency-dependent (0.1 Hz to 1 MHz) dielectric loss tangent (tanδε) of (A) com-Fe3O4,(B) syn-Fe3O4, (C) com-Ni, and (D) syn-Ni nanocomposites.
Figure 8
Figure 8
Photographs, BSE images,and EDS mapping of (A) com-Ni and (B)syn-Ni nanocomposite filaments.
See this image and copyright information in PMC

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