a) Directional solidification simulation as performed in the TS Potts model. IPF coloring of the

a) Directional solidification simulation as performed in the TS Potts model. IPF coloring of the

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Parts produced via laser powder-bed fusion additive manufacturing exhibit complex microstructures that depend on processing variables and often vary widely in crystallographic texture and grain morphology. The need to understand, predict, and control these microstructural variations motivates the development of modeling tools capable of accurately...

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... In recent years, the topic of grain formation and microstructure representation has gained prominence, underscored by the research presented in the study by Pauza et al. [11]. This research highlights the evolving understanding of how grains are formed and organized within materials, especially in the context of AM processes. ...
... This method involves modeling the material subjected to external loads on a mesoscale and subsequently averaging the effects to predict the behavior of the material at the macroscale. Numerical methods [11,15], including the Crystal Elasticity Finite Element (CEFE) method [16,17], and the Crystal Plasticity Finite Element (CPFE) method [18] offer a sophisticated approach for the calculation of the homogenized mechanical properties. These simulations enable direct comparisons with experimental outcomes or can be utilized autonomously to methodically investigate the influence of microstructural features on material behavior. ...
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... Even with intermediate samples, the EBSD measurements alone will provide only a partial picture of the forming process. Incorporating the EBSD measurements into material models is needed to obtain a more detailed understanding of the microstructural evolution at each stage of the additive manufacturing process [26]. ...
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Electron backscatter diffraction (EBSD) is an excellent tool for characterizing the crystallographic orientation aspects of the microstructure of polycrystalline material. In some additively manufactured materials, the material may undergo a phase transformation during the forming process. Although EBSD can only characterize the final microstructure, neighbor information from orientation mapping allows the microstructure before the phase transformation to be reconstructed, provided that the parent–child orientation relationship is known. An investigation of the effectiveness of the reconstruction algorithms for capturing the grain size as well as orientation gradients is undertaken with a focus on additively manufactured Ti-alloy. The EBSD results, coupled with reconstruction algorithms, reveal information on the prior grain size as well as the plastic flow of the material.
... As a result, the melt pool depth is identically equal to half the melt pool width. Following the approach outlined by Pauza et al. [33] to account for different melt pool shapes, the equation for R is modified to where z is a scaling factor. Using z < 1 results in the melt pool depth being greater than half the width, which will occur in the transition and keyhole melt pool regimes of interest in the present study [34]. ...
... This approach mimics texture development in cellular automata models, where the preferred-growth directions correspond to the diagonals of expanding decentered octahedra [36]. A similar concept has also been used to describe texture development in a standard Potts Monte Carlo scheme adapted to simulate LPBF builds [33]. ...
... The time step associated with the Monte Carlo flips is linked to a physical time step following the procedure in [37,41], which is based on grain growth kinetics. As noted in [33], the large thermal gradients in the heat-affected zone surrounding the melt pool in LPBF cause the mobility to rapidly drop off to near-negligible values. As a result, only a limited amount of coarsening occurs in the simulations. ...
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... The stochastic CA approach incorporates nucleation, growth, and diffusion of constituent elements and phases to predict the grain orientations originating in the melt pool. Pauza et al. [152] included the crystallographic orientation information in a Monte-Carlo Potts model for microstructure evolution in a PBF process. Phase field (PF) models, on the other hand, predict the 2D crystal growth dynamics (microstructure evolution) during solidification [62]. ...
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... The Rosenthal solution further assumes a point-like heat source of power [19]. Numerous grain structure simulations models are based on this approximation [22,36,80] as it provides with a simple mathematical expression of the temperature field according to the ( , , ) coordinates attached to the heat source that moves at constant velocity on the material-gas surface, = 0, in the direction along a = 0 line: ...
... The am/ellipsoid app was extended further by Pauza, et. al. in [50,51] to incorporate crystallographic orientation effects. Their work demonstrated that by biasing the spin-flip algorithm to preferentially choose a new spin based on the alignment between fast-solidifying crystal directions and the local temperature gradient, experimentally observed textures could be reproduced for a range of conditions. ...
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... The methodology utilized to simulate the effect of scan rotation on microstructure evolution can be extended to study the effect of scan strategy or any other parameter that one can expect to influence the microstructure evolution. [49]. The methodology used here will be significantly useful for optimizing process parameters to obtain desired microstructure. ...
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Laser powder bed fusion (LPBF) of Haynes 282 is gaining attention recently due to its superior mechanical properties than its conventional counterparts. In spite of the superior mechanical properties, there are significant challenges concerning crystallographic anisotropy. One of the critical but less studied parameters that influences crystallographic anisotropy is the laser scan rotation angle. This study investigates the possibility of controlling the microstructure and crystallographic texture by modifying the laser scan rotation angle. Further, three dimensional Finite difference-Monte Carlo simulations were performed to understand the microstructure evolution with varying process parameters.
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... However, the original Rosenthal equation defines a semi-circular cross section for the melt pool, which is not completely realistic. Therefore, we have used a modified version of this equation introduced by Pauza et al. [37], which determines a wider and deeper melt pool compared to the original equation. The modified Rosenthal equation can be presented as [37]: ...
... Therefore, we have used a modified version of this equation introduced by Pauza et al. [37], which determines a wider and deeper melt pool compared to the original equation. The modified Rosenthal equation can be presented as [37]: ...
... coefficients take values between 0 and 2 [37]. We can obtain the width and depth of the melt pool for different laser powers and scanning speeds using these equations. ...
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Identifying the suitable process parameters is one of the necessities to control the microstructure, and consequently various properties of additively manufactured (AM) parts. To obtain suitable process parameters, it is crucial to understand the effects of each process parameter on various aspects of microstructure of the printed material. In this work, we have conducted a parametric study on the effects of AM process parameters on the grain morphology of the metallic parts, fabricated via directed energy deposition (DED), through the Kinetic Monte Carlo (KMC) simulations. The characteristics of the melt pool and the heat-affected zone (HAZ) were incorporated into the models, and microstructural effects of altering the layer thickness, hatch spacing, scanning speed, and laser power were investigated. We used the Rosenthal equation, to predict the geometry of the melt pool and heat-affected zone formed by certain laser powers. The resulting grain morphology (i.e. the grain size and inclination) was analyzed for a large number of combinations of different process parameters. It was observed that by increasing the laser power, the number of fine and equiaxed grains decreases. On the other hand, increasing the scanning speed had a significant effect on formation of more fine grains in the final model.
... This would effectively interrupt the epitaxial growth of the prior β grains. Along with asymmetric scan rotations, instability of the melt pool and non-uniform thermal gradients [51] could lead to new prior β orientations known as stray grains [52]. Another reason for prior β grain boundary distortion is high laser scan speed which results in high temperature gradients between the edge and inner part of melt pool. ...