Polymer -bonded magnets produced by laser powder bed fusion Influence of powder morphology filler fraction and energy input on the magn etic and mechanical properties Kilian Schäfera Tobias Brauna Stefan Riegga Jens Musekampb Oliver Gutfleischa

2025-05-02 0 0 2.27MB 41 页 10玖币
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Polymer-bonded magnets produced by laser powder bed fusion: Influence of powder morphology, filler
fraction and energy input on the magnetic and mechanical properties
Kilian Schäfera, Tobias Brauna, Stefan Riegga, Jens Musekampb, Oliver Gutfleischa
a Functional Materials, Institute of Materials Science, Technical University of Darmstadt, 64287 Darmstadt,
Germany
bInstitute for Materials Technology (IfW), Technical University of Darmstadt, Grafenstraße 2, 64283
Darmstadt, Germany
Keywords:
Additive manufacturing
Laser powder bed fusion
Bonded permanent magnets
Particle alignment
Abstract
Bonded permanent magnets are key components in many energy conversion, sensor and actuator devices.
These applications require high magnetic performance and freedom of shape. With additive
manufacturing processes, for example laser powder bed fusion (LPBF), it is possible to produce bonded
magnets with customized stray field distribution. Up to now, most studies use spherical powders as
magnetic fillers due to their good flowability. Here, the behavior of large SmFeN platelets with a high
aspect ratio as filler material and its influence on the arrangement and the resulting magnetic properties
are examined in comparison to a spherical magnetic filler. The 3D distribution and orientation of the
magnetic filler was studied by computed tomography and digital image analysis. The platelet-shaped
particles align themselves perpendicular to the buildup direction during the process, which offers a new
and cost-effective way of producing composites by LPBF with anisotropic structural and functional
properties. The influence of LPBF parameters on the properties of the composites is investigated. Highest
filling fractions are required for high magnetic remanence, however the powder itself limits this maximum
due to particle shape and required minimal polymer fraction to form mechanically stable magnets. The
coercivity decreases for higher filling fractions, which is attributed to increased rotation of insufficiently
embedded magnetic particles in the matrix. It is discussed how filler morphology influences the observed
change in coercivity since the rotation of spherical particles in comparison to platelet-shaped particles
requires less energy. Our work shows the challenges and opportunities of large platelet shaped fillers used
in LPBF for the production of anisotropic functional and structural composites.
1. Introduction:
Bonded permanent magnets are key components for many energy conversion devices including sensor
and actuator applications [1]. These applications require high magnetic performance, customized stray
field distribution and shapeability for complex geometries. Bonded magnets consist of magnetic particles
within a polymer matrix and are conventionally processed via injection or compression molding [2]. The
drawbacks of molding processes are the high price and limited shapes of tooling dies, which makes it
economically only viable for large batch sizes and a reduced degree of freedom of shaping.
Additive manufacturing (AM) can overcome the limitations of conventional bonded magnets
manufacturing techniques [35]. AM also brings the potential for manufacturing magnets with specific
stray field distributions for sensor applications and improving them by the combination of soft and hard
magnetic materials [6,7]. In addition, AM is ideal for net-shape production allowing the processing of
magnets in a resource-efficient way due to the omission of additional subtractive machining. For lower
volume parts the resource criticality of the rare-earth elements present in high-performance magnets can
be addressed efficiently by AM [8].
To optimize the magnetic performance, the remanence Jr (which scales to the square for the energy
density (BH)max) and the coercivity Hc must be maximized [1]. A high remanence in bonded magnets can
be achieved with a high magnetic filling fraction. However, the mechanical stability of polymer composites
is reduced for high filling fractions [9] which is detrimental for applications with mechanical loads like
motors or generators. Similar behavior can be observed in AM of bonded magnets [10]. Literature shows
that the morphology of the filler has an influence on the magnetic, microstructural and mechanical
properties of the resulting composites [11,12]. Fim et al. investigated the influence of laser parameters on
the densification of bonded magnets [13]. Moreover, it was shown by Fliegl et al. that the porosity of parts
produced with full metal laser powder bed fusion (LPBF) can vary across the powder bed depending on
the laser incident angle [14].
The relations between process parameters, filler fraction and morphology on the magnetic and mechanical
performance of bonded magnets produced by AM processes are the subject of current research but are
yet to be fully understood [3,12,13,15,16]. Due to its high flowability, which influences the processability
of the magnetic filler in LPBF, and its easy availability, the focus of previous research on AM of bonded
magnets has mostly been on the utilization of spherical, gas-atomized powders with particles sizes of
around 20 50 µm [3]. The behavior of large Sm2Fe17N3 platelets with a high aspect ratio as filler material,
its influence on the distribution and arrangement, as well as the resulting magnetic mechanical properties
has not been studied in detail yet. Up to now, similar studies used significantly smaller particle sizes for
the AM processes with platelet-shaped powders [12,16]. The Sm2Fe17N3 powder used in this manuscript
has median particle size of 91 µm.
The aim of this work is to investigate the trade-off between the magnetic and mechanical properties of
polymer composites produced by LPBF while studying in detail the differences caused by magnetic fillers
with significantly different morphologies. In this study, spherical NdFeB and significantly larger platelet-
shaped SmFeN particles with a high aspect ratio were utilized as filler materials to investigate the potential
of non-spherical particles in AM of bonded magnets. The influence of the laser energy density and
temperature distribution across the build volume on the magnetic and mechanical properties is studied
and compared to the performance of pure polymer polyamide 12 (PA12). Furthermore, the impact of an
increasing filler fraction on the microstructure, magnetic and mechanical properties for both types of
morphologies is explored. This paper also presents the potential of the different used morphologies for an
in situ alignment process of the magnetic filler. This alignment effect can offer new and cost-effective ways
of producing anisotropic bonded magnets by LPBF, which show higher magnetic performance in
comparison to isotropic bonded magnets. The alignment process can also be transferred to AM of other
functional composites produced by LPBF to specifically tune properties like electrical conductivity.
2. Experimental:
Bonded magnets were produced using PA 12 from Sintratec (Sintratec, Switzerland), in combination with
commercially available magnetically isotropic powders: MQP-S (MQP-S-11-9) which is Nd2Fe14B based
from Neo Magnequench (Singapore) and Sm2Fe17N3 (Daido Steel, Japan). The powders were used in
their as received, thermally demagnetized state from the manufacturer. PA12 provides a good
combination of flowability and good mechanical properties which qualifies it very well for the processing
of highly filled composites. Therefore, it is used as the matrix material for the LPBF process in this study.
The morphology of the magnetic powders is presented in Figure 1. The Scanning electron microscopy
(SEM) images show that the MQP-S consist of rounds particles, as produced by atomization, with an
average particle size of 35-55 µm [17]. On the other hand, the Sm2Fe17N3, which is produced by melt
spinning, consist of larger platelet shaped particles with an average size of 91 µm [18]. Latter will be further
referred to as SmFeN. The full hysteresis loops and initial magnetization curves of the two magnetic
powders, measured in a PPMS at 300K up to 4T for fixed powders, are presented in Figure 2. Both powders
are so called exchange-coupled magnetic materials [18,19] which can be seen by the ratio between
remanence polarization (Jr) and saturation (Js). This ratio is larger than 50% of Js. For isotropic magnetic
materials remanence is half of the saturation. In exchange coupled permanent magnets, the coupling
between a hard and soft magnetic phase leads to the stabilization of the soft magnetic phase by the high
coercive phase during the demagnetization process; for this the soft phase should be well-below 100nm
in size [19]. Due to the hindered switching of the soft magnetic phase, an increase of the remanence can
be observed [18]. The properties of the feedstock materials as given by the manufacturer are presented
in Table 1.
摘要:

Polymer-bondedmagnetsproducedbylaserpowderbedfusion:Influenceofpowdermorphology,fillerfractionandenergyinputonthemagneticandmechanicalpropertiesKilianSchäfera,TobiasBrauna,StefanRiegga,JensMusekampb,OliverGutfleischaaFunctionalMaterials,InstituteofMaterialsScience,TechnicalUniversityofDarmstadt,6428...

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