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Journal of Magnetism and Magnetic Materials
journal homepage: www.elsevier.com/locate/jmmm
Magnetic and microstructural properties of Fe
3
O
4
-coated Fe powder soft
magnetic composites
Katie Jo Sunday
a
, Francis G. Hanejko
b
, Mitra L. Taheri
a,
⁎
a
Department of Materials Science and Engineering, Drexel University, Philadelphia, PA19104, United States
b
Hoeganaes Corporation, Cinnaminson, NJ08077, United States
ARTICLE INFO
Keywords:
Soft magnetic composites
Core loss
Inorganic coating
Magnetic properties
ABSTRACT
Soft magnetic composites (SMCs) comprised of ferrite-coated ferrous powder permit isotropic magnetic flux
capabilities, lower core losses, and complex designs through the use of traditional powder metallurgy
techniques. Current coating materials and methods are vastly limited by the nonmagnetic properties of organic
and some inorganic coatings and their inability to withstand high heat treatments for proper stress relief of core
powder after compaction. Ferrite-based coatings are ferrimagnetic, highly resistive, and possess high melting
temperatures, thus providing adequate electrical barriers between metallic particles. In this work, iron powder
was coated with Fe
3
O
4
particles via mechanical milling, then compacted and cured in an inert gas environment.
We find density and coercivity to improve with increasing temperatures; however, core loss greatly increases,
which is attributed to the formation of a more conductive iron-oxide phase and less resistive Fe volume. Our
work begins to exemplify the unique qualities and potential for ferrite-based coatings using traditional powder
metallurgy techniques and higher curing temperatures for electromagnetic devices.
1. Introduction
The continuous development of SMCs is crucial to electromagnetic
device potential application at high applied frequencies, nominally
400 Hz. SMCs incorporate electrically insulated particles with the
capability of high magnetic permeability and low core losses depending
on material selection, processing, and curing temperature. Utilizing
powder material all for several worthy advantages of SMCs, which
include three-dimensional magnetic flux carrying capabilities, lower
core losses, and structural freedom for complex designs [1–3]. In
addition, manufacturing cost and waste material can be reduced since
minimal processing steps are required and subtractive methods are not
necessary. The limiting factor in current SMC designs is the thermal
instability of the coating material at high curing temperatures, which
leads to large eddy current paths and potential failure from overheating
[4]. The coating material needs to be electrically resistive, thermally
stable, and compressible at low compaction pressures and iron stress-
relieving temperatures (570–775 °C). Several groups have studied
organic coatings such as epoxy resins or silicone polymers, which
cannot withstand heating above 450 °C before they begin to degrade
[5,6]. Organic coatings are thus not viable for applications requiring
low coercivity because the internal strain and dislocations brought on
by compaction cannot be relieved via curing below 500 °C [7–10].
Therefore, inorganic coatings (mostly oxides) are more suitable due to
higher thermal stability and improved soft magnetic properties if
minimal coating material is applied or ferrimagnetic material is used
[11–14]. Ceramic materials have high melting points and are electri-
cally insulating, corrosive and wear resistant, making them good
coating selections [12]. These materials, however, are dia- or anti-
ferromagnetic which decrease magnetic permeability considerably by
decreasing the overall magnetic volume [15]. Therefore materials that
exhibit ferro- or ferrimagnetism are optimal for soft magnetic applica-
tions as core and coating materials.
These two types of magnetic materials have limited frequency
ranges because of their electrical resistivity, which ultimately affects
the core loss and overall performance. Ferromagnetic materials (iron-,
nickel-, cobalt-alloys) are applicable at low frequencies ( < 2 kHz)
because of their high electrical conductivity, while ferrimagnetic
materials (ceramic oxides or soft ferrites) are applicable at much
higher frequencies [16]. The frequency range at which each material
is applicable vastly depends on eddy current loss and thus electrical
resistivity. NiZn-ferrites can be employed at UHF (ultra-high fre-
quency) between 300 MHz and 3 GHz because of a high electrical
resistivity (ρ) of ∼10 Ω·cm
6
at room temperature [17]. Likewise, MnZn-
ferrites (ρ ∼ 10 Ω·cm
2
) are limited to below VHF (very high frequency)
between 30 and 300 MHz because of more ferrous ions present
http://dx.doi.org/10.1016/j.jmmm.2016.09.024
Received 3 June 2016; Received in revised form 25 August 2016; Accepted 2 September 2016
⁎
Corresponding author.
E-mail address: mtaheri@coe.drexel.edu (M.L. Taheri).
Journal of Magnetism and Magnetic Materials 423 (2017) 164–170
0304-8853/ © 2016 Elsevier B.V. All rights reserved.
Available online 15 September 2016
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