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Microstructure and laser irradiation characteristics of TiC-free and TiC-doped tungsten-based coatings prepared by supersonic atmospheric plasma spraying

机译:超声波大气等离子喷涂制备的无掺杂钨基涂层的微观结构和激光辐照特性

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摘要

Tungsten-based coatings without TiC addition (TIC-free) and with 1.5 wt% TiC addition (TiC-doped) were fabricated by supersonic atmospheric plasma spraying (SAPS) technique, respectively. The as-sprayed coatings were then irradiated by laser. The results showed that the as-sprayed coatings were mainly composed of lamellar structure. TiC phase located mainly at lamellar gaps of the as-sprayed TiC-doped coating with a morphology of strip filled the gaps. The as-sprayed TiC-doped coating exhibited dense structure, lower porosity, reduced oxygen content and higher thermal conductivity as compared with the as-sprayed TiC-free coating. The as-Irradiated coatings could be divided into remelted zone, un-remelted zone and/or mixing zone. Cracks were more easily formed in the as-irradiated TiC-free coating than in the as-irradiated TiC-doped coating. The stripped TiC phase in the as-sprayed TiC-doped coating changed into quasi-spherical/spherical ones in the remelted zone of the irradiated coating and distributed along the tungsten grain boundaries. The averaged tungsten grain size in the remelted zone of the as-irradiated TiC-doped coating was about 5.4 mu m and that of the as-irradiated TiC-free coating was about 14.8 mu m. There were about 96 wt% alpha(W) and about 4 wt% gamma(W) existed in the remelted zone near the surface of the as-irradiated TiC-free coating. Only alpha(W) could be received in the remelted zone far from the surface of the as-irradiated TiC-free coating and the remelted zone of the as-irradiated TiC-doped coating. There were no obvious diffraction peaks for gamma(W) could be indexed from the XRD patterns for the as-irradiated TiC-doped coating. The ability of the as-sprayed TiC-doped coating to resist laser irradiation was greater than the as-sprayed TiC-free coating, mainly attributing to the higher thermal conductivity of the as-sprayed TiC-doped coating and the refinement effect of TiC particles in the as-irradiated TiC-doped coating.
机译:通过超声常压等离子体喷涂(SAPS)技术,制造了无TiC添加(无TiC的TiC)和1.5wt%TiC添加(TiC掺杂)的基于钨的涂层。然后通过激光照射喷涂的涂层。结果表明,喷涂涂层主要由层状结构组成。 TiC相位主要位于喷涂的TiC掺杂涂层的层间隙,具有填充间隙的形态。与喷涂的无涂层相比,喷雾的掺杂涂层具有致密的结构,较低的孔隙率,降低的氧含量和较高的导热性。作为辐照涂层可分为雷熔断区,未经熔融区和/或混合区。在作为照射的TiC掺杂的涂层中,在无辐射的TIC涂层中更容易形成裂缝。喷涂的TIC掺杂涂层中的剥离的TIC相变为辐射涂层的重熔区域中的准球形/球形,并沿钨晶界分布。作为照射的TiC掺杂涂层的重熔区中的平均钨晶粒尺寸约为5.4μm,并且如辐照的无涂层的涂层约为14.8μm。在AS照射的TIC涂层表面附近,在雷熔断区中存在约96wt%α(w)和约4wt%γ(w)。只有α(W)可以在远离AS照射的TIC-涂层的表面的表面的重熔区域中接收,并且可以在辐照的TIC掺杂涂层的雷熔断区中得到。对于γ(W)没有明显的衍射峰可以从XRD图案中指向AS照射的TiC掺杂涂层。喷涂的TiC掺杂涂层抵抗激光照射的能力大于喷涂的无线涂层,主要归因于喷涂的TIC掺杂涂层的较高导热率和TIC颗粒的细化效果在作为照射的TIC掺杂涂层中。

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