Additive manufacturing attracts much interest for manufacturing and repair of structural parts for the aerospace industry. This paper presents comparative characterization of aircraft items made of Al 4047 alloy, Ti-6Al-4V alloy, and 17-4 precipitation hardened (PH) (AISI 630) stainless steel, either manufactured or repaired by laser engineered net shaping (LENS). Chemical analysis, density, and surface roughness measurements, X-ray micro-computed tomography (μ-CT) analysis, metallography, and micro-hardness testing were conducted. In all three materials, microstructures typical of rapid solidification were observed, along with high density, chemical composition, and hardness comparable to those of the counterpart wrought alloys (even in hard condition). High standard deviation in hardness values, anisotropic geometrical distortion, and overbuild at top edges were observed. The detected defects included partially melted and unmelted powder particles, porosity, and interlayer lack of fusion, in particular at the interface between the substrate plate and the build. There was a fairly good match between the density values measured by μ-CT and those measured by the Archimedes method; there was also good correlation between the type of defects detected by both techniques. Surface roughness, density of partially melted powder particles, and the content of bulk defects were significantly higher in Al 4047 than in 17-4 PH stainless steel and Ti-6Al-4V alloy. Optical gaging can be used reliably for surface roughness measurements. The implications of these findings are discussed.
Thin film-capped metallic nanoparticles (TFCMNPs) hold big promise for rapid, low-cost, and portable tracing of gas analytes. We show that sensing properties can be controlled by the configuration of the TFCMNPs. To this end, two methods were developed: layer by layer (LbL) and drop-by-drop, i.e., drop casting (DC). The TFCMNP prepared via LbL method was homogeneous and gradually increased in thickness, absorbance, and conductivity relative to TFCMNP prepared via DC method. However, our results indicate that the sensing of TFCMNP devices prepared via DC is significantly higher than that of equivalent LbL devices. These discrepancies can be explained as follows: LbL forms a high dense layer of TFCMNPs without vacancies, and a well-controlled deposition of NPs. The distance between the adjacent NPs is controlled by the capped ligands and the linker molecules making a rigid TFCMNP. Thus, exposing LbL devices to analyte induces a marginal change in the NP-NP distance. However, in DC devices, the analyte induces major change in the NP distances and permittivity due to their lack of connection, making the sensing much more pronounced. The DC and LbL methods used thiol and amine ligands-capped metallic nanoparticles to demonstrate the applicability of the methods to all types of ligands. Our results are of practical importance for integrating TFCMNPs in chemiresistive sensing platforms and for (bio) and chemical sensing applications
Additively manufactured (AM) materials and hot rolled materials are typically orthotropic, and exhibit anisotropic elastic properties. This paper elucidates the anisotropic elastic properties (Young’s modulus, shear modulus, and Poisson’s ratio) of Ti6Al4V alloy in four different conditions: three AM (by selective laser melting, SLM, electron beam melting, EBM, and directed energy deposition, DED, processes) and one wrought alloy (for comparison). A specially designed polygon sample allowed measurement of 12 sound wave velocities (SWVs), employing the dynamic pulse-echo ultrasonic technique. In conjunction with the measured density values, these SWVs enabled deriving of the tensor of elastic constants (Cij) and the three-dimensional (3D) Young’s moduli maps. Electron backscatter diffraction (EBSD) and micro-computed tomography (μCT) were employed to characterize the grain size and orientation as well as porosity and other defects which could explain the difference in the measured elastic constants of the four materials. All three types of AM materials showed only minor anisotropy. The wrought (hot rolled) alloy exhibited the highest density, virtually pore-free μCT images, and the highest ultrasonic anisotropy and polarity behavior. EBSD analysis revealed that a thin β-phase layer that formed along the elongated grain boundaries caused the ultrasonic polarity behavior. The finding that the elastic properties depend on the manufacturing process and on the angle relative to either the rolling direction or the AM build direction should be taken into account in the design of products. The data reported herein is valuable for materials selection and finite element analyses in mechanical design. The pulse-echo measurement procedure employed in this study may be further adapted and used for quality control of AM materials and parts.
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