The invention relates to nanoparticles for use in permanent magnets, for example in electric motors or generators.
Permanently energized motors and generators present great demands on the magnetic properties of the permanent magnets used. In a conventional construction, these are achieved merely with anisotropic sintered rare earth magnetic materials based on neodymium-iron-boron or samarium-cobalt. The reduction in access to rare earth elements has led to an intensification of the search for new permanently magnetic, in particular rare earth-free, magnetic materials. This has been stimulated in particular by nanotechnology. This is due to the fact that permanent magnetic properties, in addition to the high magnetization (magnetic polarization) due to a suitable atomic and crystallographic structure, are greatly dependent on magnetization processes at the mesoscopic scale. Permanent magnetic properties are promoted by the micro-structural construction as nanoscale single-domain particles, as known in the context of the rapid-solidification technique.
However, the synthetic construction of permanent magnetic materials made of nanoparticles having high spontaneous magnetization is prevented by the increasing sensitivity to oxidation in nanoparticles. Thus, even favored transition metal alloys of Co and Fe are easily oxidized.
The coercive field strengths which can be achieved by what is referred to as shape anisotropy cannot be achieved experimentally at the same time.
While, in current rare earth-based permanent magnets (e.g. SmCo or NdFeB), high magnetocrystalline anisotropy in microcrystalline, metallurgically produced microstructures generates a coercive field strength which is sufficiently strong for almost all current applications, the remanent magnetization in these systems remains limited to the spontaneous magnetization of the magnetically hard phase (e.g. Nd2Fe14B of 1.61 T).
Nanotechnological synthesis methods can be used, by virtue of the shaping possibility, to produce magnetically single-domain nanoparticles. The nanoparticles can also take the form of elongate ellipsoids, nanowires or nanorods and can be arranged in oriented ensembles. Ferromagnetic materials such as NiFe and CoFe, originally known as magnetically soft metals and alloys, are used on account of the shape anisotropy to create a permanently magnetic material having substantial magnetic reversal stability. In that context, the anisotropy field as an upper limit for the coercive field is limited, for infinitely elongate particle geometries, to 2Pi*Ms (saturation magnetization). Due to influences from the ensemble, but also on account of the fact that the coercive field is reduced by defects on the surface of the nanoparticles and by corners and edges (μH=alpha*μHa−Neff*Js), it has not been clear to date whether this limit value can be achieved in the ensemble of particles, or whether additionally other magnetic reversal modes (curling, fanning) emerge that likewise result in a reduced coercive field.
A common maximum value for a coercive field in FeCo nanowires is approximately 5.5 kOe and is thus too low for high energy densities. This can once again be remedied conventionally by means of what is termed the core-shell method, that is to say depositing a second magnetically hard material onto the outer surface of the shape-anisotropic nanoparticle. A magnetically hard shell can then be deposited areally onto the nanoparticle and can completely cover the nanoparticle. DE 10 2012 204 083.8 discloses such an arrangement.
DE 10 2012 204 083.8 discloses a nanoparticle having at least one elongate core which is formed with at least one first, magnetizable and/or magnetized material and with a shell, surrounding the core, which is formed with at least one second material having magnetocrystalline anisotropy.
This concept of two-phase magnets, referred to as exchange spring magnets, has been investigated in metallurgical methods—in particular what is called the rapid quenching process. However, limited control with respect to shaping and distribution of the two phases with respect one another leads to a sharp drop in the coercive field strength and thus to reduced permanent magnetic properties.
One embodiment provides nanoparticles, having an elongate core extending from a first end to a second end along a longitudinal axis, which core is made using at least one first, magnetizable and/or magnetized material; wherein, on the core, a first covering is formed at the first end and a second covering is formed at the second end, which coverings have a second material having magnetocrystalline anisotropy, wherein the core is not covered thereby between the first covering and the second covering over a distance greater than zero along the longitudinal axis.
In a further embodiment, the first covering and the second covering cover surface regions of the core that extend transversely with respect to the longitudinal axis.
In a further embodiment, the first covering and the second covering completely cover the surface regions of the core that extend transversely with respect to the longitudinal axis.
In a further embodiment, the first covering and the second covering cover surface regions of the core that extend along the longitudinal axis.
In a further embodiment, the first covering entirely coats the first end and the second covering entirely coats the second end.
In a further embodiment, the second material consists of second nanoparticles whose volumes are in each case smaller than that of the core.
In a further embodiment, the volume of the second nanoparticles is 1 to 20% of the volume of the core.
In a further embodiment, the second nanoparticles are spherical.
In a further embodiment, the distance between the first covering and the second covering is at least 50%, in particular 80%, of the length of the core along the longitudinal axis.
In a further embodiment, the nanoparticle is formed as a nanorod and the core is cylindrical with a length and a radius.
In a further embodiment, the first covering and the second covering are in each case in the form of a cylinder, a hollow cylinder, a hollow cylinder having a base cylinder, or a pebble bed.
In a further embodiment, the first covering and the second covering have a thickness.
In a further embodiment, the distance is the length of the core plus twice the thickness and minus the extent of the first covering and of the second covering along the longitudinal axis.
In a further embodiment, an outer protective layer for protection from corrosion, in particular oxidation, is formed.
In a further embodiment, the first covering and the second covering form part of the protective layer.
Another embodiment provides a method for coating a nanoparticle with a first covering and a second covering as disclosed above, wherein the core on one hand and the first covering and the second covering on the other hand are synthesized separately from one another and subsequently chemical or physical deposition of the second material onto the first material is carried out.
Another embodiment provides a permanent magnet comprising a multiplicity of nanoparticles as disclosed above.
In a further embodiment, the nanoparticles are arranged such that the orientations of the longest dimensions of the nanoparticles have a preferred direction.
Another embodiment provides an electric motor or generator having at least one permanent magnet as disclosed above, and a rotor (e.g., arranged radially inward from the at least one permanent magnet) configured to rotate relative to the at least one permanent magnet.
Example embodiments and aspects of the invention are described in more detail below with reference to the figures, in which:
Embodiments of the invention provide an improved nanoparticle. For example, the nanoparticle may be used to create an improved permanently magnetic material. Other embodiments provide an improved permanent magnet and an improved electric motor and an improved generator. New concepts for synthetic permanent magnets are also disclosed. An effective increase in the energy density may be achieved. Sensitivity to oxidation may be reduced and achievable coercive field strengths may be increased.
Some embodiments provide a nanoparticle having an elongate core extending from a first end to a second end along a longitudinal axis, which core is made using at least one first, magnetizable and/or magnetized material, wherein, on the core, a first covering is formed at the first end and a second covering is formed at the second end, which coverings have a second material having magnetocrystalline anisotropy, wherein the core is not covered thereby between the first covering and the second covering over a distance >0 along the longitudinal axis.
In that context, and within the meaning of this invention, a nanoparticle is to be understood as a particle having a diameter of less than 1000 nm. In particular, the nanoparticle has a diameter of less than 300 nm.
An elongate core is to be understood, within the meaning of this invention, as a core having an aspect ratio—that is to say the ratio of the longitudinal dimension to the transverse dimension—of at least 1.5. The aspect ratio is suitably at least 5, ideally at least 10.
Elongated particles having a core-covering nanostructure, in which at least two material systems participate, may provide high permanent magnetic performance, e.g., high remanence, a high coercive field and a high energy product as well as to long-term stability; also disclosed is the combination of these magnet components to give ensembles.
One of the components, specifically the core phase, has a higher volume fraction and carries high magnetization.
A second phase, in this case the covering phase, has high magnetocrystalline anisotropy. This magnetically stabilizes the surface or the interface. In addition, the choice of core size, core diameter and covering thickness and optimized contact achieves a magnetic exchange coupling which leads to a single-phase magnetic reversal behavior and thus promotes homogeneous rotation in the case of high coercive fields.
It has been recognized, according to the invention, that the magnetic reversal process begins at the ends of the core phase or of the core. According to the invention, the second phase is deposited at the ends of the core phase. It has been recognized, according to the invention, that this permits an improvement in the magnetic properties while at the same time reducing the volume fraction of the second phase (the coating of the core) when compared to a closed phase.
The reduction of the total volume of the second phase, or of the second material, advantageously raises the magnetization of the nanoparticle when compared to complete encapsulation of the core. Reducing the fraction of the second phase advantageously reduces the price per magnet component since a large number of the materials used having high magnetocrystalline anisotropy are very expensive elements such as Pt, Pd or rare earths.
Other embodiments provide a method for coating a nanoparticle with a first covering and a second covering, wherein the core on one hand and the first covering and the second covering on the other hand are synthesized separately from one another and subsequently chemical or physical deposition of the second material onto the first material is carried out.
Further advantages arise in the synthesis of the magnet components in particular from the use of nanoparticles as the second phase or as the second material. Generally, homogeneous coating of a nanoparticle with a second layer is a great challenge, such that partial coating is advantageously simpler to carry out. Due to the magnetic interaction between the first and second phases, or between the first and second materials, it is advantageously favored to accumulate the second phase at the ends of the nanoparticles of the first phase. Synthesis can be carried out either in one step or separately. Separate synthesis makes it possible to use the optimum formation conditions for both phases. In many cases, and in particular for forming the hard phase, a thermal treatment may be required which exceeds the thermal stability of the first phase. For example, temperatures of approximately 1000° C. may be necessary for the formation of hard ferrites and temperatures above 600° C. may be required for converting FePt into the magnetically hard tetragonal structure. In addition, the conditions for forming the second phase can have a negative effect on the first phase, such as oxidation of the first phase. This can advantageously be prevented by means of separate synthesis. Deposition of the second phase can be carried out equally by means of chemical or physical methods.
By constructing according to the invention, a high coercive field is provided in a simple manner via the combination of high shape anisotropy with stabilization of the surface by magnetocrystalline anisotropy.
According to one embodiment, the first covering and the second covering can cover surface regions of the core that extend transversely with respect to the longitudinal axis.
According to another embodiment, the first covering and the second covering can completely cover the surface regions of the core that extend transversely with respect to the longitudinal axis.
According to another embodiment, the first covering and the second covering can cover surface regions of the core that extend along the longitudinal axis.
According to another embodiment, the first covering can entirely coat the first end and the second covering can entirely coat the second end.
According to another embodiment, the second material can consist of second nanoparticles whose volumes are in each case smaller than that of the core.
According to another embodiment, the total volume of the second nanoparticles can be 1 to 20% of the volume of the core.
According to another embodiment, the second nanoparticle can be spherical or the second nanoparticles can be spherical.
According to another embodiment, the distance between the first covering and the second covering can be at least 50%, in particular 80%, of the length of the core along the longitudinal axis.
According to another embodiment, the nanoparticle can be formed as a nanorod and the core can be cylindrical with a length and a radius.
According to another embodiment, the first covering and the second covering can in each case be in the form of a cylinder, a hollow cylinder, a hollow cylinder having a base cylinder, or a pebble bed.
According to another embodiment, the first covering and the second covering can have a thickness.
According to another embodiment, the distance can be the length of the core plus twice the thickness and minus the extent of the first covering and of the second covering along the longitudinal axis.
According to another embodiment, an outer protective layer for protection from corrosion, in particular oxidation, can be formed.
According to another embodiment, the first covering and the second covering can form part of the protective layer.
Other embodiments provide a permanent magnet comprising a multiplicity of the disclosed nanoparticles, wherein the nanoparticles are arranged such that the orientations of the longest dimensions along the longitudinal axis of the nanoparticles have a preferred direction.
According to another embodiment, permanent magnets according to the invention can be used in electric motors or generators.
exampleexampleexampleexampleexampleexampleexample
Such coverings 20a and 20b can also be termed caps. In this case, the second phase takes the form of caps, and specifically the form of coverings of the end face and parts of the end face of the first phase. In comparison to the embodiment as shown in
An example calculation using the following values r=10 nm, L=200 nm, s=2 nm and t=50 nm makes it advantageously possible to show the amount of second material saved by virtue of the invention. It has been shown that, for a so-called sarcophagus configuration as shown in
The invention makes it possible to save second material with respect to the generated coercive field strength. It is accordingly possible to propose cost-saving solutions for permanent magnets.
Number | Date | Country | Kind |
---|---|---|---|
10 2013 221 828.1 | Oct 2013 | DE | national |
This application is a U.S. National Stage Application of International Application No. PCT/EP2014/067619 filed Aug. 19, 2014, which designates the United States of America, and claims priority to DE application No. 10 2013 221 828.1 filed Oct. 28, 2013, the contents of which are hereby incorporated by reference in their entirety.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/EP2014/067619 | 8/19/2014 | WO | 00 |