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In Part I of this article, the role of the Zn content in the development of solidification microstructures in Al-Zn alloys was investigated experimentally using X-ray tomographic microscopy. The transition region between h100i dendrites found at low Zn content and h110i dendrites found at high Zn content was characterized by textured seaweed-type structures. This Dendrite Orientation Transition (DOT) was explained by the effect of the Zn content on the weak anisotropy of the solid-liquid interfacial energy of Al. In order to further support this interpretation and to elucidate the growth mechanisms of the complex structures that form in the DOT region, a detailed phase-field study exploring anisotropy parameters' space is presented in this paper. For equiaxed growth, our results essentially recapitulate those of Haxhimali et al. [1] in simulations for pure materials. We find distinct regions of the parameter space associated with h100i and h110i dendrites, separated by a region where hyperbranched dendrites are observed. In simulations of directional solidification, we find similar behavior at the extrema, but in this case, the anisotropy parameters corresponding to the hyperbranched region produce textured seaweeds. As noted in the experimental work reported in Part I, these structures are actually dendrites that prefer to grow misaligned with respect to the thermal gradient direction. We also show that in this region, the dendrites grow with a blunted tip that oscillates and splits, resulting in an oriented trunk that continuously emits side branches in other directions. We conclude by making a correlation between the alloy composition and surface energy anisotropy parameters.
In Part I of this article, the role of the Zn content in the development of solidification microstructures in Al-Zn alloys was investigated experimentally using X-ray tomographic microscopy. The transition region between h100i dendrites found at low Zn content and h110i dendrites found at high Zn content was characterized by textured seaweed-type structures. This Dendrite Orientation Transition (DOT) was explained by the effect of the Zn content on the weak anisotropy of the solid-liquid interfacial energy of Al. In order to further support this interpretation and to elucidate the growth mechanisms of the complex structures that form in the DOT region, a detailed phase-field study exploring anisotropy parameters' space is presented in this paper. For equiaxed growth, our results essentially recapitulate those of Haxhimali et al. [1] in simulations for pure materials. We find distinct regions of the parameter space associated with h100i and h110i dendrites, separated by a region where hyperbranched dendrites are observed. In simulations of directional solidification, we find similar behavior at the extrema, but in this case, the anisotropy parameters corresponding to the hyperbranched region produce textured seaweeds. As noted in the experimental work reported in Part I, these structures are actually dendrites that prefer to grow misaligned with respect to the thermal gradient direction. We also show that in this region, the dendrites grow with a blunted tip that oscillates and splits, resulting in an oriented trunk that continuously emits side branches in other directions. We conclude by making a correlation between the alloy composition and surface energy anisotropy parameters.
The transition rate (mass change) in a free quasi-two-dimensional growth of individual NH 4 Cl dendrites from a supersaturated aqueous solution is investigated. It is found that the integral experimental kinetic curves can be fitted by an exponential function corresponding to a Weibull model. It is shown that the Kolmogorov-Avrami theory can be applied to the description of growth kinetics of the individual dendrite. In addition we find small amplitude relaxation oscillations of the dendrite mass with base frequency of about 0.1 Hz. The origin of these oscillations is connected with the interaction of the diffusion fields of an existing and arising secondary branches. This conclusion agrees qualitatively with our computer simulation results.
Figure 1 a depicts the dip coating process for the production of certain classes of TMD structures. First, a piece of SiO 2 / Si or quartz wafer is immersed into an aqueous (NH 4 ) 2 MoS 4 (or (NH 4 ) 2 WS 4 ) solution (0.23% w/v (g mL −1 ) in DI water) and removed at different speeds to control the drying velocity. As the water evaporates, small nuclei are formed at the solution-substrate interface, and these nuclei initiate the growth of various solid (NH 4 ) 2 MoS 4 , or (NH 4 ) 2 WS 4 morphologies as intermediate states of MoS 2 and WS 2 . The self-assembled TMD morphologies are strongly dependent on the evaporation rate of the solvent and the diffusion rate of the TMD-precursors in solution. Figure 1 b,c presents optical images of the selfassembled (NH 4 ) 2 MoS 4 structures formed at different evaporation speeds and pH conditions. At very fast evaporation speeds (approximately 320 nl s −1 ) induced by high temperature (80 °C), a uniform thin fi lm of (NH 4 ) 2 MoS 4 was formed after the complete removal of the solvent (condition A, Figure 1 b) because there was insuffi cient time to induce the formation of nucleation seeds. In contrast, at evaporation speeds that were two orders of magnitude slower (0.67-1.72 nl s −1 ), dendritic structures were formed (condition B, Figure 1 c). The dendrite structures have many worm-like stems with a large number small side branches; self-assemblies of these seeds randomly formed on the substrate.In addition to these two nonoriented phases, the spontaneous formation of well-oriented wire patterns was observed when the acidity of solution increased from pH 6.41 to pH 5.02 at the same evaporation speed as condition B (condition C, Figure 1 d). Interestingly, these long wires, which grew from seeds formed in parallel arrays at the initial solution/substrate/air contact line, displayed uniform spacing between the wires without serious distortion of the arrays. The formation of aligned wires can be explained by the "fi ngering instability" phenomenon. [ 18,19 ] When the solvent begins evaporating at the solution/substrate contact line, fi ngering instability induced by the regulation of the evaporation speed, which affects the internal fl ow of the solution, leads to the periodic formation of nucleation-seed arrays. In turn, this results in the spontaneous growth of regular, unidirectional wire arrays from the seeds during the drying process (Figure 1 d). The critical dependence of the directional growth mechanism on the pH variation is not yet clear. However, we believe that the acidity of the reaction media can effectively suppress the gradation of the precursor diffusion, which is the driving force in the generation of the dendrite side-arms and the lateral expansion of the selfassembly, thereby preserving the main stream and, as a result, enhancing the formation of aligned wire arrays. [ 20 ] Thus, the evaporation speed, solution concentration and pH are the key factors that control the nucleation and growth processes, which lead to different self-assembled structures.A sub...
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