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Article

Influence of the Origin of Polyamide 12 Powder on the Laser Sintering Process and Laser Sintered Parts

1
Inspire, Innovation Center for Additive Manufacturing (icams), Lerchenfeldstrasse 3, St. Gallen 9014, Switzerland
2
Department of Mechanical and Process Engineering, Swiss Institute of Technology (ETHZ), Tannenstrasse 3, Zürich 8093, Switzerland
*
Author to whom correspondence should be addressed.
Appl. Sci. 2017, 7(5), 462; https://doi.org/10.3390/app7050462
Submission received: 3 April 2017 / Revised: 24 April 2017 / Accepted: 25 April 2017 / Published: 30 April 2017
(This article belongs to the Special Issue Materials for 3D Printing)

Abstract

:
Different features of polymer powders influence the process of laser sintering (LS) and the properties of LS-parts to a great extent. This study investigates important aspects of the “powder/process/part”-property relationships by comparing two polyamide 12 (PA12) powders commercially available for LS, with pronounced powder characteristic differences (Duraform® PA and Orgasol® Invent Smooth). Due to the fact that the primary influence factor on polymer behaviour, the chemical structure of the polymer chain, is identical in this case, the impacts resulting from powder distribution, particle shape, thermal behaviour, and crystalline and molecular structure, can be studied in detail. It was shown that although both systems are PA12, completely different processing conditions must be applied to accomplish high-resolution parts. The reason for this was discovered by the different thermal behaviour based on the powder production and the resulting crystalline structure. Moreover, the parts built from Orgasol® Invent Smooth unveil mechanical properties with pronounced anisotropy, caused from the high melt viscosity and termination of polymer chains. Further differences are seen in relation to the powder characteristics and other significant correlations could be revealed. For example, the study demonstrated how the particle morphology and shape impact the surface roughness of the parts.

Graphical Abstract

1. Introduction

The laser sintering (LS) of polymer powders is a primary shaping process by definition. A solid body is created out of an unstructured and formless powder bed by the energy input (laser radiation). This means that besides the shape, the properties of the part will also be created during the build process to a great extent. The characteristic of the used powder has an especially large influence on the part properties, as was recently summarized by Sutton et al. [1]. Furthermore, almost all of the material and production parameters influence the final properties of the LS parts. The interference of different build-parameters, but also their difficult and precise control, has far-reaching consequences for the fabricated parts. For LS parts, an exact prediction of the properties is thus difficult [2]. Moreover, the highly complex LS parts are influenced by their three-dimensional orientation in the building chamber of the LS-equipment. In the scientific literature, numerous investigations are described regarding correlations of single build parameters and their combinations on part properties. The following list assembles some important works in this area:
  • Influence of the energy density (Andrew number (An)) [3,4];
  • Influence of molecular properties of the polymer on the micro-structure of the parts [5];
  • Energy density (An) and part orientation in a build envelope [6];
  • Incomplete coalescence of polymer melt and resulting process problems [7];
  • Influence of powder refreshment and build temperature at a constant energy density (An) [8];
  • Influence of Energy density (An) in combination with powder layer thickness [9];
  • Influence of Energy density (An) in combination with powder shape [10];
  • Variations of temperature in a build envelope and part cylinder [11].
It can be recognized from this shortened list with selected non-linear correlations how critical the control of the LS-process can be regarding predictable LS-part properties. In a larger screening work by Wegner et al. [12], the laser power, laser speed, scan spacing, powder bed temperature, layer thickness, and orientation of the parts in the build chamber were investigated, and it could be revealed that scan spacing, in combination with layer thickness, are the most significant in terms of the part density and mechanical properties, if the other parameters are constant.
What is noticeable is that in almost all of the studies mentioned above, the examination is dedicated to only one LS-material. A comparison of the processing behavior and the part properties on at least two materials, as in this study, is rarely done [10,13]. This is surprising, as from a commercial point of view, LS materials have been available for a long time from different sources. Both the company Evonik (Marl, Germany) and the company Arkema (Colombes, France) supply the polyamide 12 (PA12) polymer powders processed in LS. Evonik powders are distributed through the machine suppliers EOS (Krailling, Germany) and 3D-Systems (Rock Hill, SC, USA) under the trade names PA 2200 (EOS) and Duraform® PA (3D-Systems), and are therefore widely dispersed and dominate the LS market. Arkema directly supplies the LS-powder under the trade name Orgasol® Invent Smooth to the market, independently of the major machine manufacturers.
Due to the fact that all three materials are identical regarding their primary chemical structure, as they are all polyamide 12, the comparison of these materials and the resulting parts can be concentrated on secondary factors, like powder shape, particle size distribution, thermal behavior, and microstructural and morphological differences. It is well known in the community of LS-users (service bureaus) that the powders from the different sources behave differently in the LS-process and create different part characteristics. A refined investigation on the influence of powder origin on the laser sintering process and laser-sintered parts is hence obvious.

2. Materials and Methods

Two polyamide 12 (PA12) powders mainly used in industrial LS-applications were selected for this study (As mentioned, there is a third main LS-powder on the market from the company EOS (Krailling, Germany), named PA 2200. This material is based on Vestosint powder, and behaves in a similar way to Duraform® PA. For this reason, it is not included in the present study):
  • Duraform® PA (abbreviated: DF-PA); Company 3D-Systems, Rock Hill, SC, USA;
    (DF-PA is based on Vestosint® powder from the company Evonik, Marl, Germany)
  • Orgasol® Invent Smooth (abbreviated: Orgasol-IS); Company Arkema, Colombes, France.
It is important to realize that powders from the “Orgasol®-family” [14] and “Vestosint®-family” [15] have been used as PA12 powders in different coating technologies and other applications in huge quantities for decades. Both materials are fine-tuned by the suppliers for their use in LS to a certain extent [16,17]; however, the basic powder production includes the same principle process for the LS-powders:
  • Vestosint® powders are generated by precipitation [18].
  • Orgasol® powders are produced from direct polymerization [19].
The different production techniques have drastic consequences for the morphology of the particles, as can be revealed with microscopy analysis. Figure 1 depicts the differences by means of Scanning Electron Microscopy (SEM) pictures. The differences in the shape and surface structure of single particles can be clearly recognized. Whilst DF-PA exhibits a shape similar to potatoes (Figure 1, left), Orgasol® particles are much more spherical (Figure 1), with a smooth and slightly wavy surface structure (like cauliflower). Comparing both SEM pictures also gives the impression that the particle size distribution is much narrower in the case of Orgasol®-IS, which could be acknowledged during the investigation (see Section 3.1).
For this study, both materials were processed on a commercial laser sintering machine manufactured by DTM (DTM was purchased in 2001 by 3D-Systems and no longer exists). The exact machine type used was a DTM 2500plus HiQ, retro-fitted with a digital scan-head and a six-zone multi- heating system for improved thermal stability. The machine is under active maintenance, used in industrial part production, and the parts present the highest possible quality to date. For the investigation, two processing parameters were set to fixed values:
  • Scan speed: 10 m/s;
  • Layer thickness: 0.1 mm.
Other process settings like the part bed temperature (°C), laser power (W), and scan spacing (mm) were adjusted and optimized so that a (self-designed) process-control-part could be produced with maximum resolution details. This means, for the benchmark part depicted in Figure 2, that all dimensions after build are correct; all slits are open; all walls are built and stand upright without breaking (even the thinnest); the corners are edged and not rounded; the space between the walls is open; and no, or at least as few as possible, undesired (partially) melted powder sticks in-between (for further details, see Figure 2). The evaluation of such a benchmark structure cannot be explained in detail here, but these parts have been successfully used in our production facility to monitor machine and process stability for years as a periodical control instrument. In this way, the experience of the LS-machine operators results in great confidence in the results, even if the qualification is partly based on empirical facts.
A main purpose of this work is to identify the processing parameters for high-resolution parts for each material as a reference, as these targets are the most relevant for industrial applications. During the procedure, test specimens for mechanical examinations were built with the identified machine settings. It is important to recall that the mechanical properties of LS-parts can be influenced by LS-processing parameters to a great extent, as laser sintering is a primary shaping process. Increasing the energy supply supports the fusion of particles and leads to higher mechanical properties, as has often been described in the literature, e. g., Starr et al. worked in this field [9]. So, in principle, one could complete a study on the optimized mechanical properties; however, the best parameters for high mechanical properties would not generate high-resolution parts. Due to an excessive energy input and other processing problems like thermal bleeding, incorrect part dimensions, etc., the parts produced would not be delivered to customers because of their poor resolution.
In order to investigate the mechanical properties and differences according to part build orientation (anisotropy), specimens were placed in the build platform in the XYZ- and ZXY-direction (see ASTM-Standard F2921-11: “Terminology for additive manufacturing-coordinate systems and test methodologies” for nomenclature and Figure 3 for the random distribution of specimens in the building chamber of the LS equipment). The following specimens were built with the previously evaluated processing parameters (high-quality settings):
  • 20 tensile test bars according to ISO 527 (10 each in the XYZ- and ZXY-direction)
  • 20 un-notched impact bars (Charpy-1eU) according to ISO-197 (10 each in the XYZ- and ZXY-direction)
  • 20 notched impact bars (Charpy-1eA) according to ISO-197 (10 each in the XYZ- and ZXY-direction)
The depicted mechanical test specimens in Figure 3 are used to investigate the surface roughness of the parts with a measuring system from the company GelSight Inc. The GelSight-System offers a simple yet powerful way to rapidly, reproducibly, and repeatedly investigate textured surfaces. The setup is composed of a bench top with a movable glass plate, under which a gel pad coated on one side with a reflective material (sensor) is pressed onto the sample (see Figure 4). The gel conforms closely to the surface and lends it its reflective properties, thereby producing a positive imprint of the surface, regardless of its optical properties. The surface is subsequently illumined and photographed from six different directions. A height map is computed from those pictures using a photometric stereo algorithm within minutes (see Figure 4).
Other methods used in this investigation are:
  • Thermal analysis (DSC) was performed on a DSC 25 (TA Instrument, New Castle, DE, USA) with a constant heating and cooling rate of 10 °C/min under a nitrogen atmosphere.
  • The particle size distribution was measured on a LS230 particle analyzer (Beckman Coulter, Brea, CA, USA). The powder particles were dispersed and suspended in ethanol during the measurements.
  • X-ray diffraction patterns were recorded on a Bruker Nanostar U diffractometer (Bruker AXS, Karlsruhe, Germany) with Cu Ka radiation (λ = 1.5419 Å) and a VÅNTEC-2000 MikroGap area detection system. The powder samples were prepared between two Kapton® films. The recorded WAXD patterns were analyzed with the evaluation software BRUKER DIFFRAC.EVA (version 4.1., Bruker AXS, Karlsruhe, Germany).
  • Mechanical Properties were measured with a standard tensile testing machine (Zwick GmbH&Co. KG, Ulm, Germany) regarding ISO 527-1 under controlled environmental conditions (23 °C/50 r.h); samples were used without any special pre-conditioning (dry conditions).
  • Melt Volume Rate (MVR) was determined with a polymer tester Type D 4004 (Dynisco, Franklin, MA, USA) with the following measuring conditions: - temperature 235 °C, - load 5 kg.

3. Results

3.1. Processing Parameters

The elaborated processing parameters for the production of quality-optimized parts from DF-PA and Orgasol-IS are summarized in Figure 5. The processing parameters were assessed by an inspection of the benchmark parts (see Figure 2) produced and optimized over different iterations. Figure 5 also depicts the benchmark parts produced from both polymers with the given settings, to demonstrate their high resolution regarding the adequate details (explanation see Figure 2, too).
In the LS-process, the energy input regarding the area is defined with the so-called Andrew number (An) given in Formula (1) [20].
Andrew number (An) (J/mm2) = laser power (W)/(hatch distance (mm) × scan speed (mm/s))
It can be clearly recognized from the numbers in Figure 5 that the total energy input for both materials is distinctly different. An for Orgasol-IS is two times higher than for DF-PA. This is achieved by the lower hatch distance and higher laser power of Orgasol-IS. The energy input difference can be explained by the drastically lower part bed temperature for Orgasol-IS during sintering, which was 164 °C compared to 175 °C for DF-PA. The lower the surface temperature of the powder in the part bed, the more energy must by supplied by the laser to melt the polymer. However, the question of where the differences in the part bed temperature arise remains. This is quite unanticipated, as both materials are PA12 and the equilibrium melting point (Tm) for PA12 is 178°C [21]. So, for DF-PA and Orgasol-IS, an almost similar processing temperature during LS-processing should be expected.

3.2. Thermal Analysis (DSC)

Differential Scanning Calorimetry (DSC) uncovers the reason for the previously described differences by an examination of their thermal properties. Figure 6 compares the DSC-runs of both polymers. Although both systems are PA12, it can be undeniably recognized from Figure 6 that they present substantially different melting and crystallization performances. The thermal transition signals show no congruence in either 1st heating or in cooling, but only during the 2nd heating.
The exact thermal transition values (Tm, Tmonset, Tc, Tconset) achieved from the DSC-runs depicted in Figure 6 and their respective enthalpies (ΔHm, ΔHc), are summarized in Table 1.
The DSC-runs in Figure 6 and the respective thermal values in Table 1 show some distinct thermal differences between DF-PA and Orgasol-IS. The following features and findings of the thermal properties can be derived:
  • The melting point (Tm) and melting-onset (Tmonset) of DF-PA is 5.0 °C, which is 7.2 °C higher than for Orgasol-IS. This is a clear sign of why the part bed temperature for Orgasol-IS must be drastically lowered, as the build temperature in LS-processing is typically set close to the melting onset.
  • The melting enthalpy (ΔHm) for both materials is over 100 J/g, and therefore, is two times higher than would be expected for standard PA12 [20] as it was found in the respective 2nd heating runs (approx. 50 J/g–60 J/g).
  • The crystallization point (Tm) and crystallization onset (Tmonset) for DF-PA is 7.9 °C, which is 5.7 °C lower than for Orgasol-IS.
  • In the 2nd heating run, all values are significantly different from their individual first heating run and show lower values, with a tendency for the lowest values for DF-PA.
These findings give a clear indication that the polymer manufacturers adjust both materials for optimized LS-processing. A high melting enthalpy is induced and is beneficial for a high contour resolution of parts, as it raises the threshold for the thermal bleeding of neighboring particles. The shift in Tm and Tc, and their respective onsets, is an adjustment to create more stable processing through the widening of the sintering window. The sintering window is calculated using Formula 2 [22].
Sintering window (°C) = Melting onset (°C)-Crystallization onset (°C)
The sintering window is particularly pronounced for DF-PA with a value of 32.5 °C, compared to 19.6 °C for Orgasol-IS. A lower onset of crystallization is a key element for the desired suppression of crystallization during the slow cooling rates of the LS-process. DF-PA explicitly outperforms Orgasol-IS in this context. This big difference in the sintering window is the reason for the well-known difficulties frequently encountered in the industrial production using Orgasol-IS. If the thermal adjustment of the laser sintering equipment is not precise, or if the temperature on the building platform is inhomogeneous, as is regularly observed for older LS-machines, premature crystallization may occur for Orgasol-IS during the LS-process and cause the curling or warpage of parts, leading to a build termination. The distinct difference between both LS-powders with respect to their thermal behavior is obvious from a DSC investigation and explains their well-known disparate behavior in industrial LS-processing. However, the question regarding the origin of these differences still remains. Is plain tempering of the polymers after production used to increase the degree of crystallinity in the semi-crystalline status? In that case, the effect should be equivalent for both polymers. However, this is not the case and the differences are hidden in a more refined adjustment of the crystalline structure.

3.3. X-ray Analysis

The adjustment of melting with respect to enthalpy and the transition point is achieved with the different production processes of the powder materials (see Figure 1). In the case of pressure-supported precipitation from organic solvents (DF-PA), this leads to the expected “γ-crystal-structure”, along with a “α-crystal-structure” [23]. This is unusual for thermally treated PA12; however, this combination of crystalline structures has a great influence on the thermal behavior of the powder.
Figure 7 depicts the Wide-Angle X-Ray Scattering-analysis (WAXD) of both powders in a virgin state. The differences are obvious at a distribution angle (2Θ) between 20° and 25°, as seen in Figure 7. The signal for DF-PA is much broader and pronounced compared to Orgasol–IS. Due to the formation of the α-crystalline-structure during the precipitation of DF-PA, the area for the XRD-signal is much wider and indicates a higher crystallinity [24].
The distinct melting behaviors can be related to different crystalline structures, since an additional tempering step is carried out to obtain higher values for crystallization enthalpy (ΔHm) compared to “Standard-PA12” (see Table 1). Furthermore, the melting point of a polymer depends on the thickness of the crystalline lamellae (lc), as described by the Gibbs-Thomson-Equation [25]. The more monomeric units that are present between the lamellae of a single crystal, the higher the lateral spread and the intrinsic energy become, resulting in a higher melting point. The precipitation process of DF-PA may also induce larger lamella structures with higher melting points. In general, the different production processes for both PA12 LS-polymers largely influence their thermal behaviors. The precipitation process for DF-PA obviously offers more possibilities to influence its crystalline structure, in a positive sense regarding LS-processing, by the formation of an additional α-phase and the increase of the lamellae dimensions.

3.4. Powder Size Distribution

Besides the thermal and crystalline differences described so far, both materials also present a different powder size distribution. This can be observed in Figure 1. A refined analysis of these differences can be found in Figure 8. A comparison of the scattering for both powders is presented regarding their respective volume distributions, achieved with laser diffraction measurements. The visual impression of Figure 1 is confirmed. Orgasol-IS has smaller particles and a narrower distribution than DF-PA, as confirmed by the numbers issued from the laser diffraction test presented in Figure 8.
The smaller particle size distribution of Orgasol-IS, in combination with the visually identified higher sphericity of the particles (Figure 1), should lead to a higher packing density of the powder (the investigations on the exact sphericity are to be published elsewhere soon). This is the case and can be found in the material specification data sheets of the powder producers. For Orgasol-IS, a bulk packed density of 0.55 g/cm3 regarding ISO 1068-1975 is given, while DF-PA shows a bulk packed density of 0.53 g/cm3 (own measurement). This is an additional effect, explaining a higher An in the processing of Orgasol-IS (see Figure 5). A higher powder packing density should lead, as a first consequence, to LS-parts with a higher part density, and this, in turn, would lead to improved mechanical properties.

3.5. Mechanical Properties and Anisotropy

The mechanical properties summarized in Table 2 were achieved by the investigation of parts described in Section 2. All parts were produced and randomly distributed in the LS build chamber of the said DTM machine per Figure 3, with the build parameters given in Figure 5. In order to have a better overview of the data for the present study (the data rows are named “present work” in Table 2), the results are compared with data from the powder producers presented in their respective “Material Data Sheet (MDS)”.
The following comments and conclusions can be derived from Table 2:
  • The XYZ-orientation of the values of this work match relatively well with the MDS values for Young’s modulus and tensile strength. This can be expected, as these values are material inherent to a great extent.
  • For Elongation at the break in the XYZ-direction, only about half of the published value was achieved. This could be due to applying high-resolution build parameters for this study. Published mechanical data will be achieved most likely with property optimized build settings.
  • For the Charpy measurements, there is only one MDS value published: 34 kJ/m2 for un-notched Orgasol-IS. As this value is consistent with this study’s measured value, it is assumed that all Charpy data for the XYZ-direction also lie in the expected range.
So, for the XYZ-direction, all measured values are truthful compared to MDS-data. In order to reveal the anisotropy of the parts, an analysis for the XYZ- and ZXY-direction data leads to the following statements:
  • For tensile strength, DF-PA remains at nearly the same level, while Orgasol-IS drops to almost half the value.
  • For Elongation at the break, the drop for DF-PA is about 50%, whilst Orgasol-IS loses 85% of the initial magnitude.
  • Finally, in the case of the Charpy tests (un-notched and notched) for Orgasol-IS, the loss of stability in the ZXY-direction is drastic in comparison to DF-PA.
In summary, this means that Orgasol–IS is much more affected by anisotropic mechanical properties than DF-PA.
As LS is a layer-by-layer technology, the weak point in the microstructure of the parts is the boundary between the layers. Based on the mechanical test results, this means that layer adhesion for Orgasol-IS is largely reduced. A sufficient isotropy during the sintering process can be achieved by a good interconnection of the polymer melt at the layer interface, through sufficient polymer chain entanglement. These diffusion-driven effects are correlated with the polymer melt viscosity.

3.6. Melt Viscosity and Chain Termination

In a first and very simple approach, the melt viscosity of polymers can be determined by MVR (Melt-Volume-Rate) measurements. If Orgasol-IS and DF-PA are measured in a virgin state, the following values are obtained: MVR (DF-PA): approx. 60 g/cm3 and MVR (Orgasol-IS): approx. 15 g/cm3 (measurements are performed with: 235 °C/5 kg). This large difference in viscosity is a clear indication that polymer interdiffusion for Orgasol-IS is reduced, as a lower MVR-value means a higher viscosity. A restrained mixing of molten polymer, and consequently, limited chain entanglement at the layer boundaries of the LS-parts, would be the likely consequence.
However, there exists a second effect on a molecular level influencing the inter-layer bonding for these polymers. The synthesis of PA12 is technically accomplished by the ring opening polyaddition of lauryl lactam. The principle of the sequence of the reaction is presented in Figure 9 (deprived of stoichiometric correctness). This figure schematically depicts what can be controlled regarding the end-groups during the course of polyaddition.
If the end-groups are chemically terminated, a polymer with a defined chain length is achieved, resulting in a fixed melt viscosity. On the contrary, if the end-groups are unregulated, it results in a still reactive polymer with chains that can be extended under suitable conditions like those encountered in LS, by the reaction of remaining end groups (post-condensation). For LS-polymers, this means that if end-groups are still active, they can strongly support the process of layer adhesion by post-condensation in the interdiffusion zone of evolving LS-parts. A better layer-adhesion and reduced anisotropy of LS-parts is the result.
A melt viscosity check (MVR) helps to verify the presence of an active chain end polymer. If DF-PA powder is extracted from the LS-process and subjected to MVR-measurement after a few process loops, the MVR of DF-PA is drastically reduced to values lower than 20 g/cm3. At the same time, MVR-values of Orgasol-IS remain almost unchanged after several loops. In conclusion, the enhanced isotropy of the DF-PA parts can be explained by two effects:
  • DF-PA starts in a low viscous status, with a high flowability of melt that leads to a good interdiffusion in the boundary-zone of progressing LS-parts.
  • In the zone of interdiffusion, post-condensation takes place and gives the parts additional stability in the overlapping zone by covalent bonding.

3.7. Surface Roughness

Considering the pronounced difference in the particle shape in Figure 1, it can be expected that the more homogeneous morphology of Orgasol-IS particles and their narrower size distribution (Figure 8) result in a much smoother surface of LS-parts. This corresponds to the long-lasting rumor in the LS-community that Orgasol-IS parts exhibit better, more precise, and smoother surfaces.
To confirm or disprove this idea, the surface roughness of respective parts (tensile bars) was investigated with GelSight. The orientation of the surface in the LS-process is taken into account: “up-face”, “down-face”, or the vertical walls due to the layer-wise building process and their orientation in the building envelope. Figure 10 depicts the received height maps of the different samples and the respective values for the area roughness parameter Sq (root mean square height roughness) and Sa (average height roughness) evaluated over the complete 3D surface, respectively. The field of view of the area measured is 5 mm × 7.5 mm.
With the presented surface measurements, it can be shown that for the two surface roughness parameters, Sa and Sq, and for all investigated part directions, the values are better, i.e. lower for Orgasol-IS compared to DF-PA. Especially the bottom surface (corresponding to the first sintered layer of a part) seems to be significantly improved for Orgasol-IS. The surfaces are typically investigated through hand rubbing to get an impression of the part’s haptic. So, the analytical investigations with GelSight confirm the subjective rating that Orgasol-IS-parts exhibit smoother surfaces and connect it, for the first time, with the reproducible analytical data and measurements required to further optimize surface analyses for LS-parts.

4. Discussion

Table 3 summarizes the considered features for both investigated polymers DF-PA and Orgasol-IS in some key words and depicts several prominent findings in this connection. In general, the manufacturers of PA12 improve their polymers for their use in LS regarding several properties. However, the companies Evonik and Arkema have different strategies to adjust their materials marketed as Duraform® PA and Orgasol® Invent Smooth for the laser sintering process. Principally due to the different production technologies, they supply materials with different particle size distributions and particle shapes, which have severe influences on the processing, packing density, and surface roughness of the parts. The thermal situation is controlled through the different production processes. The melting and crystallization of both materials is adjusted for a good and stable behavior during LS-processing. However, the precipitation process offers better possibilities to fine-tune the crystalline structure of the polymer and DF-PA presents a much larger sintering window, resulting in a better and more forgiving processing behavior.
The biggest advantage of DF-PA can be identified in the improved homogenous mechanical properties of the LS-parts in all directions. The anisotropy for Orgasol-IS is pronounced and LS-part producers (service bureaus) must be aware of this fact. However, the regulated viscosity of Orgasol-IS leads to reduced powder “aging” (post-condensation), which is beneficial from an economical point of view because the refresh rate is about 10% (statement of producer), and is thus much lower than for DF-PA (refresh rate from 30% to 50%). Moreover, Orgasol-IS typically supplies parts with smoother surfaces, with a higher detailing grade due to the more homogenous particles.

5. Conclusions

Regarding the production of LS-parts, adopters of this technology can work with two principal solutions for PA 12 standard material. The first is the precipitated “Vestosint”, and the second is the directly polymerized “Orgasol” powder. The choice will generate differences and has consequences for the LS-process and LS-parts. Users with a higher demand for better surfaces gain benefits from using Orgasol-IS; however, this concurrently means that they must have a more precise control of the thermal situation in their machine because of the reduced sintering window. Due to the controlled viscosity of Orgasol-IS, a further advantage of this material can be realized from a commercial point of view, as the production powder can be set to a much lower refreshing rate.
If the enhanced mechanical properties in all spatial directions are the prominent issue for the desired LS-parts, the producer should use DF-PA. The easier processing of this powder is due to the significantly larger sintering window, forgiving more mistakes during processing, and accepts higher thermal instabilities in (older) LS-equipment.

Acknowledgments

The authors are grateful to Michael Schneider from irpd AG for producing the parts in an industrial environment and supplying all his technical know-how in producing high-quality LS-parts. Other thanks go to Leonardo Scardigno who performed some of the presented measurements. Finally, a big thanks goes to Felix Reifler from Empa for performing the X-ray analysis.

Author Contributions

Manfred Schmid initiated the investigation, planned and conducted the trials, and wrote the paper. Rob Kleijnen measured and deduced the thermal investigations and the particle size distribution, and performed the mechanical measurements. Marc Vetterli performed the surface roughness measurements of LS-parts and interpreted the respective results. Konrad Wegener is supervisor of the group, initiated the idea of material comparison in this way, and gave valuable input on all steps of the study progress.

Conflicts of Interest

The authors declare no conflict of interest. Inspire icams is an independent research institute in Switzerland with no subjection to any of the mentioned commercial products or companies.

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Figure 1. Different morphology of the particles caused by the production process.
Figure 1. Different morphology of the particles caused by the production process.
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Figure 2. “Benchmark-Part” to optimize the processing parameter towards high-quality parts.
Figure 2. “Benchmark-Part” to optimize the processing parameter towards high-quality parts.
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Figure 3. Randomly distributed specimens as built for both investigated powders.
Figure 3. Randomly distributed specimens as built for both investigated powders.
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Figure 4. GelSight measurements with greyscale pictures and a calculated surface height map.
Figure 4. GelSight measurements with greyscale pictures and a calculated surface height map.
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Figure 5. Comparison of processing parameters for the production of parts.
Figure 5. Comparison of processing parameters for the production of parts.
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Figure 6. Comparison of the thermal behavior of Duraform® PA (DF-PA) (blue) and Orgasol® Invent Smooth (Orgasol-IS) (red) by thermal analysis (DSC).
Figure 6. Comparison of the thermal behavior of Duraform® PA (DF-PA) (blue) and Orgasol® Invent Smooth (Orgasol-IS) (red) by thermal analysis (DSC).
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Figure 7. X-ray diffraction (XRD) patterns of Orgasol-IS and DF-PA.
Figure 7. X-ray diffraction (XRD) patterns of Orgasol-IS and DF-PA.
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Figure 8. Comparison of volume distribution of DF-PA and Orgasol-IS by laser diffraction.
Figure 8. Comparison of volume distribution of DF-PA and Orgasol-IS by laser diffraction.
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Figure 9. Polyaddition of lauryl lactam with or without end-group regulation.
Figure 9. Polyaddition of lauryl lactam with or without end-group regulation.
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Figure 10. Comparison of surfaces from different part orientations of DF-PA and Orgasol-IS.
Figure 10. Comparison of surfaces from different part orientations of DF-PA and Orgasol-IS.
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Table 1. Thermal transition points (Tm, Tmonset, Tc, Tconset) and corresponding enthalpies (ΔHm, ΔHc).
Table 1. Thermal transition points (Tm, Tmonset, Tc, Tconset) and corresponding enthalpies (ΔHm, ΔHc).
PA12 TypeDF-PAOrgasol-ISDiff. Absolute
First heating run
 Melting point Tm (°C)187.0182.0Δ = 5.0 °C
 Melting onset Tmonset (°C)180.8173.6Δ = 7.2 °C
 Melting enthalpy ΔHm (J/g)110.7102.3
Cooling run
 Crystallization point Tc (°C)143.2151.1Δ = 7.9 °C
 Crystallization onset Tconset (°C)148.3154.0Δ = 5.7 °C
 Crystallisation enthalpy ΔHc (J/g)48.056.1
Second heating run
 Melting point Tm (°C)175.8177.4Δ = 1.6 °C
 Melting onset Tmonset (°C)167.5171.3Δ = 3.8 °C
 Melting enthalpy ΔHm (J/g)51.362.3
Table 2. Results of the tensile and impact tests for Duraform® PA (DF-PA) and Orgasol® Invent Smooth (Orgasol-IS) in different orientations and compared with data from the Material Data Sheet (MDS) * of powder suppliers.
Table 2. Results of the tensile and impact tests for Duraform® PA (DF-PA) and Orgasol® Invent Smooth (Orgasol-IS) in different orientations and compared with data from the Material Data Sheet (MDS) * of powder suppliers.
ValueUnitDuraform® PAOrgasol® Invent Smooth
MDS *Present WorkMDS *Present Work
build directionXYZXYZZXYXYZXYZZXY
Young’s modulusMPa15861675 ± 411610 ± 6118001700 ± 251580 ± 21
ISO-527-1
Tensile strengthMPa4347.6 ± 1.540.6 ± 3.44551.7 ± 0.729.3 ± 3.6
ISO-527-1
Elongation at break%146.6 ± 0.73.7 ± 0.62012.0 ± 0.41.9 ± 0.3
ISO-527-1
Charpy un-notchedkJ/m2-32.3 ± 2.610.2 ± 2.03434.6 ± 2.02.8 ± 0.7
ISO 197 1eU
Charpy notchedkJ/m2-2.0 ± 0.52.1 ± 0.1-2.6 ± 0.51.3 ± 0.2
ISO 197 1eA
* MDS = material data sheets of powder producers.
Table 3. Summary of the main features of laser sintering (LS)-powders and characteristic influences on parts and processing.
Table 3. Summary of the main features of laser sintering (LS)-powders and characteristic influences on parts and processing.
FeatureDuraform® PAOrgasol® Invent Smooth
productionprecipitationdirect polymerisation
particle shape“potato”
→ compromise regarding flowability
Spherical
→ more detailed parts
→ better part surfaces
thermal situationlarge sintering window
→ easier processing
Crystal-size and structure!
needs homogeneous and stable thermal conditions during processing
powder distributionBroad
→ medium powder flowability
Narrow
→ high powder flowability
→ better powder packing density
chain terminationopen chains
→ easy flowing melt
→ enhanced properties due to “post-condensation”
Blocked
→ less powder “ageing”
(economic)
mechanical propertiesincreased homogeneity in all directionspronounced drop in z-direction (anisotropy)

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MDPI and ACS Style

Schmid, M.; Kleijnen, R.; Vetterli, M.; Wegener, K. Influence of the Origin of Polyamide 12 Powder on the Laser Sintering Process and Laser Sintered Parts. Appl. Sci. 2017, 7, 462. https://doi.org/10.3390/app7050462

AMA Style

Schmid M, Kleijnen R, Vetterli M, Wegener K. Influence of the Origin of Polyamide 12 Powder on the Laser Sintering Process and Laser Sintered Parts. Applied Sciences. 2017; 7(5):462. https://doi.org/10.3390/app7050462

Chicago/Turabian Style

Schmid, Manfred, Rob Kleijnen, Marc Vetterli, and Konrad Wegener. 2017. "Influence of the Origin of Polyamide 12 Powder on the Laser Sintering Process and Laser Sintered Parts" Applied Sciences 7, no. 5: 462. https://doi.org/10.3390/app7050462

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