Effects of laser processing parameters on the mechanical properties, topology, and microstructure of additively manufactured porous metallic biomaterials: A vector-based approach
Graphical abstract
Introduction
Additively manufactured (AM) porous structures are a new class of biomaterials, which have shown many advantages [1], [2], [3], [4] over conventional biomaterials. Moreover, it is possible to use AM techniques to fabricate patient-specific implants based on the computed tomography (CT) images of each patient. Titanium and its alloys exhibit properties that make them suitable for biomedical applications including a high degree of biocompatibility, corrosion resistance, and durability [5], [6], [7]. Using AM techniques, it is also possible to manufacture interconnected open-cell porous biomaterials with controlled unit cell shape and size. Porous biomaterials have shown several advantages over traditional solid implants. For example, the high degree of porosity in the volume of such structures drastically decreases the stiffness of the metallic implant to the values close to the stiffness of natural bone. The low stiffness of the implant helps in better distributing the mechanical load between implant and natural bone and, thus, assists in avoiding future bone resorption. The hollow space inside porous structures also allows for easy body fluid transport inside the implant [8], [9] and consequently stimulates bone ingrowth, thereby improving implant fixation and longevity.
The most well-known AM techniques for making metallic porous biomaterials are selective laser melting (SLM) [10] and selective electron beam melting (SEBM) [11]. In both techniques, the usual workflow starts off with constructing a surface tessellation language (STL) file describing the geometry of the to-be-manufactured part. The CAD file is then virtually cut into several slices with predefined thicknesses (usually in the range of 30–100 μm [12]). The laser or electron beam then follows the contours found in every slice and melts the specified areas within the powder bed, thereby fusing the powder together and creating a solid part in a layer-by-layer fashion. After the laser/electron beam has scanned the contours found in each layer, the powder bed moves down by the slice thickness and a fresh layer of powder is deposited on the build plate. As a rapid melting-solidification process, the microstructure, topology, and mechanical properties of the resulting part are strongly dependent on the laser/electron beam processing parameters [13], [14], [15], [16], [17].
In the past, a few groups [12], [18], [19], [20], [21], [22], [23] have studied the effects of laser beam parameters on the microstructure and the mechanical properties of porous biomaterials. In the previous studies, the 3D constructed CAD files of the porous structure have been used to determine the scanning line of the laser beam. In such techniques (as demonstrated in Fig. 3 of [24]), the 3D model of the structure is constructed in CAD programs. The resulted model is converted into STL file and then sliced by the 3D printer preparation software. Each strut in each layer can consist of several melting paths. In the current study, we use a different, i.e. vector-based, approach to manufacture porous biomaterials. In this approach, the lattice structure is designed by defining the struts as vectors describing its start and end coordinates without any strut diameter data, and thus no STL files are needed to describe the surface of the structure. Slicing to the desired height creates a cloud of intersection points between the vectors and the slice planes. During manufacturing, each intersection point is molten by a single strike of the laser (Fig. 1). In the jumps between the points, the laser is deactivated. The selected power and the exposure time of the laser on each point determines the energy input and, thus, the size of the melt pool and the diameter of the struts constituting the porous structure. This approach has two major advantages over the STL-based technique. First, it removes the intermediates steps required for creating the STL file and slicing the resulting geometry. Those intermediate steps could be computationally expensive and reduce the accuracy of the contours. Second, there is a direct relationship between the processing parameters and the microstructure, topology, and mechanical properties of the resulting porous structure. We studied how the laser processing parameters including laser power and exposure time affect the microstructure, topology, and mechanical properties of the resulting AM porous biomaterials. Porous structures were therefore additively manufactured with a wide range of exposure times and laser powers. The effect of those parameters on the surface roughness, strut diameter, hardness, relative density, elastic modulus, yield stress, first maximum stress, and plateau stress of the porous structures was studied.
Section snippets
Materials and manufacturing
In conventional Powder Bed Fusion processes, the product is built based on a STL-file with all dimensions defined before printing. For lattice structures, the scanning strategy is based on the area of the object on a specific slice plane. Large areas will have a combination of a hatch and a contour while small areas, like struts of several 100 μm will have contours only. In the vector-driven approach, the strut thickness of the lattice structure that is built, is not pre-defined. The
Results
By changing the laser power and exposure time parameters, porous structures with a wide range of strut diameter (155 < d < 276) and relative density (0.06 < μ < 0.46) were manufactured (Fig. 4b–c). The porous structures made by the lowest laser machine parameters (i.e. exposure time of 150 μs and laser powers of 80 W and 96 W) were not completely manufactured and therefore were not suitable for mechanical testing. Therefore, the corresponding strut diameter, relative density, and mechanical property
Discussions
The results of this study demonstrated that the vector-based approach is a viable alternative for STL-based design of AM porous biomaterials. The microstructure and mechanical properties of the matrix material, as indicated by the hardness values within the struts, were similar as long as the laser energy input was high enough. It was therefore possible to achieve porous biomaterials with different porosities, strut diameters, and relative densities simply by modifying the laser processing
Conclusions
In this study, the effects of variation in two main laser processing parameters, namely laser power P and exposure time ts, on the topological parameters and mechanical properties (relative density, surface hardness, elastic modulus, yield stress, plateau stress, and first maximum stress) were investigated. It was found that all the noted mechanical properties increase with increasing either laser power or exposure time. Therefore, among the 36 types of porous structure manufactured in this
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