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Infl uence of resin fl ow on shrinkage of additive manufacturing coated sand molds

机译:树脂流动对增材制造覆膜砂型收缩率的影响

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Coated sands are used extensively for additive manufacturing sand molds in the metal casting process, and the packing structure changes caused by the resin fl ow promote the shrinkage and deformation of the part. During the coated sand heating, the resin on the surface fl owing to the contact points of the particles forms the resin neck and causes particles to pack close to each other. In this work, the diameters of the coated ceramsite sand before and after heating were measured based on in-situ experimental observations with image measuring apparatus and blue laser, to obtain the relationship between resin coating thickness and the particle diameter. The particle packing model was established to describe the particles’ achievement of a stable state one by one. A re-packing simulation was then performed after reducing the particle diameter according to the resin coating thickness, to obtain the shrinkage ratios at different particle size distributions. It was found that the resin coating thickness increased from 0.8 to 2.3 μm as the particle diameter increased from 107 to 500 μm, for the coated ceramsite sand with the resin content of 2wt.%; the shrinkage ratio decreased fi rst and then increased as the particle diameter increased. The experimental minimum shrinkage ratio was 3.28%, and the corresponding particle diameter was 300-375 μm, while the minimum shrinkage ratio obtained by simulation was 3.43%, and the corresponding particle diameter was 214-300 μm. After mixing the fi ve groups proportionally, the shrinkage ratios of the simulation and experiment dropped to 2.81% and 3.04%, respectively, indicating the best results.
机译:覆膜砂被广泛用于金属铸造过程中的增材制造砂模中,由树脂流引起的堆积结构变化会促进零件的收缩和变形。在覆膜砂加热期间,由于颗粒的接触点而在表面上的树脂形成树脂颈并导致颗粒彼此靠近堆积。在这项工作中,基于图像测量装置和蓝色激光的原位实验观察,测量了加热前后的陶瓷陶粒直径,从而获得树脂涂层厚度与粒径之间的关系。建立了粒子堆积模型,以逐一描述粒子达到稳定状态的过程。然后,根据树脂涂层厚度减小粒径后,进行重新装填模拟,以获得不同粒径分布下的收缩率。发现对于树脂含量为2wt。%的陶瓷陶粒砂,随着粒径从107增加到500μm,树脂涂层厚度从0.8μm增加到2.3μm;收缩率首先下降,然后随着粒径的增加而增加。实验的最小收缩率为3.28%,对应的粒径为300〜375μm,通过模拟求出的最小收缩率为3.43%,对应的粒径为214〜300μm。在按比例混合五个组之后,模拟和实验的收缩率分别降至2.81%和3.04%,表明效果最佳。

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