Laser Treatment of Soft Magnetic Materials-Effect and Properties

The mechanical strength of Somaloy® 5P is with a value of 50-60 MPa after the heat treatment at temperature 550-650 °C under a protective atmosphere for magnetic applications. The strength of sintering iron alloys is > 300 MPa and can obtain 900 MPa for high performance iron alloys like PM materials Fe-NIMoCuC or FE-CrMoC. For this reason the technology of selective laser « sintering » without the addition of a foreign powder was experimented to evaluate the influence of this technology on the materialographical structure and on the mechanical and magnetic properties of the Somaloy® 5P. The goal is to obtain a densification layer with a high density poor porosity in the area of the surface without to change the pore distribution and the structure in the core. This paper investigates the effect of a selective laser « sintering » on the surface of a soft magnetic component and describes the final properties of component after the treatment. Finally, a proposal of an optimised process recommendation for the selective laser sintering of Somaloy® 5P components is made.


Introduction
The PM material Somaloy® [1][2][3][4][5] of the company Höganäs which is the considered Trademark for soft magnetic composite powders, was used for the experimental procedure for selective laser sintering. Somaloy® are pure iron, water atomized powder with an electrically insulating coating (Figure 1).
The insulating coating is one of the key factors to balance of good permeability, low core loss and good mechanical strength. The density of this material after the compacting under axial conditions DOI: 10.35840/2631-5076/9241 in space binding the material together to create a solid structure without the presence of pores. In single component powder, the laser melts only the outer surface of the particles (surface melting) fusing the solid no melting cores.

Experimental Procedure
The PM material Somaloy 5P Höganäs was used for the experimental procedure for selective laser sintering. The powder for the manufacturing of the toroid is a press-ready mix with particle size of about 250 µm. With ultra-high insulation suitable for higher permeability and low loss applications.
Toroids with an inner diameter of 45 mm, an outer diameter of 55 mm and a height of 5 mm were compacted under a high compaction pressure with a die temperature of about 80 °C to obtain a density of 7.2 g/cm 3 . The toroids were heat treated at 650 °C under pure nitrogen in a belt furnace. Heat treatment temperature, heat treatment time were chosen to avoid the de-terioration of the insulating layer. The coating will start to deteriorate at higher temperatures due to thermally activated diffusion processes, leading to decrease component resistivity. For this soft magnetic materials, the heat treatment temperature is lower that the conventionally sintering temperature for the iron or iron-alloys like Fe-CrMo, Fe-NiMoCu that is normally at 1120 °C or > 1120 °C under a protective atmosphere of a mixture of nitrogen-hydrogen.
Somaloy® 5P with a density of 7.2 g/cm 3 should be heat-treated in pure nitrogen atmosphere to avoid poor performance of the magnetic properties. The results are very logical because a component with low density -in this case 7.2 g/cm 3 has many open and large pores which will lead to oxygen deeply penetration inside the component. The oxidation will take place in the whole part.  Interparticles isolation can be seen as the grid separating particles from each other.
A scanning electron microscope (SEM) is a type of electron microscope that produces images of a sample by scanning the surface with a focused beam of electrons. The electrons interact with atoms in the sample, producing various signals that contain information about the surface topography and composition of the sample.
Under a scanning electron microscope the laser morphology surface was observed to determine the transformation of pores on the surface and compare to the reference sample in the heat treated state without the laser sintered process. If all pores at the surface are closed, the laser treatment can be considered as satisfied.
The SEM investigation ( Figure 5) of the fracture surface shows that the coating layer is not deteriorated and the formation of the sintering bridges on the powder particles cannot be seen.
These metallographical observations permit to conclude that the conditions of heat treatment are satisfied for the component made of Somaloy 5P.
After the heat treatment the toroids have been selective laser sintered under a protective gas (Argon without and with addition of hy-not show a deterioration of the powder particles. Because of the strength of the materials, the metallographical preparation of the experimental samples needs a great experience and a new method procedure. The sample were cut with a Secotom 15/50 cutting machine from the company Struers. Secotom machine performs precise and deformation-free cutting of section metals. The cooling with a special aqueous liquid permits to avoid a heating of the sample and consequently a modification of the structure. The cut piece was hot mounted (180 °C at 250 bar) under an automatic process.
The next step is ground with several successively finer abrasive grits, polished until all the scratches from the last grind are removed with an automatic process for a maximum preparation quality and bests results and etched with an aqueous acid solution (3% Nital) and then  ding.
The magnetic properties in AC and DC field were measured using a Brockhaus Hysteresis graph 200 MPD.

Macrocospical examination
In comparison to the reference toroid without the laser treatment, the macro graphical examination of the toroids at the outer diameter (Figure 6) shows a surface that is smooth and bright. The presence of opened pores cannot be seen.

Metallurgical examination
The laser thickness has been measured at five different position as it indicates in the graphic of Figure 7 by metallurgical examination.
The thickness of the layer varied between 150 and 360 µm (Figure 8). Microcracks in the layer and at the interface between the layer and the matrix cannot be detected. The porosity in the layer is reduced and free of pores > 5 µm. A densification in the area has taken place without to modify the core of the matrix with the presence of opened pores. The examination shows clearly that the laser treatment lead to good results. SEM micrograph (Figure 9) shows the surface morphology between the laser treated surface without the presence of opened pores (right side) and the surface with the matrix with the presence of opened pores, that is not modified by the laser power. The transition line is free of microcracks which can appear during the cooling drogen) at temperature between 900 and 1100 °C. Scan rate, scan line speed, laser power and frequency are the variables operating parameters to obtain a densified layer of about 100-300 µm on the surface.
Three toroids have been treated by laser treatment. The goal was in the experimental procedure to realize the densification by laser process the outer diameter.
For the evaluation of the magnetic properties, the compacted and curing toroid samples have 50 drive primary and 50 sense secondary turn of win-  can be seen in the Figure 10. The structure is ductile with the formation of particles boundary without the presence of pores. It signifies that the tem-of the ring due to a stress situation.
The fracture surface of the laser treated area  The Vickers hardness of the reference ring and of the laser treated ring was measured. The re-sults of the micro hardness is summarized in the Table 1. The effect of densified surface after the laser treatment on the micro hardness is absoperature in this area permits to obtain a local liquid phase « sintering ».

Hardness
Hardness is a characteristic of a material, not a fundamental physical property. It is defined as the resistance to indentation, and it is determined by measuring the permanent depth of the indentation.
The Vickers hardness test method, also referred to as a microhardness test method, is mostly used    may be used to quantify the core losses when a magnetic material is exposed to alternating magnetic fields. One approach consists of determining the behavior of the material as a function of excitation parameters and material constants. The first component is related to the hysteresis portion of the core losses, which depends on the structure and composition of the material, the second component is related to the eddy-current losses while the last component refers to the excess losses or anomalous losses.
The core loss of the reference toroid and the laser treated toroids are represented in the Figure 11 for two different polarisation.
For these toroids at > 300 Hz the behavior by 0.5 and 1.0 Tesla is similar. The highest core losses are measured in laser treated rings and the lowest in reference material without laser treatment. At frequency < 200 HZ the iron losses are under 50 W/kg. However at high frequency the core loss increases considerably.

Conclusions
The following conclusions have been drawn from this study: lutely clear. The micro hardness of the surface is about 50% higher than the micro hardness of the reference ring.

Determination of the magnetic properties
The determination of the magnetic properties have been measured on three toroids in each state.

Direct Magnet Field (DC) results
The results of the magnetic properties in direct magnet field (DC) for the laser treated toroid are summarized in the Table 2 and for the reference toroid in the Table 3. The comparison of the values from the two tables for the iron loss shows clearly that the iron loss for the laser traded toroid is higher than the iron loss of the reference toroid. An increase of the applied lead to an augmentation of the iron loss and this from 13% at 500 A/m to 38% at 1000 A/m. The permeability is higher for the laser traded toroid.

Alternative Magnet Field (AC) results
Core losses are defined as the power absorbed by a core under stated conditions of applied time varying magnetic field. Different approaches  Figure 11: Core loss versus frequency at two different polarisation.