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Near-substrate plasma characteristics and relationships between heat fluxes into substrates and them of a supersonic ammonia and nitrogen-hydrogen-mixture DC plasma jet for nitriding under a low pressure environment

机译:用于低压环境下氮化的超音速氨和氮氢混合直流等离子体射流的近基板等离子体特性及其与基板的热通量之间的关系

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Spectroscopic and electrostatic probe measurements were made to examine plasma characteristics near a titanium plate under nitriding for a supersonic direct-current arc plasma jet generator under a low pressure environment. Heat fluxes into the plate from plasma were also evaluated with a Nickel slug and thermocouple arrangement. Ammonia and mixtures of nitrogen and hydrogen were used as the working gas. In the mixture of N_2+nH_2, the H_2 mole fraction n was varied from 0 to 3, in which mole fractions of 0 and 3 corresponded to pure nitrogen and simulated ammonia, respectively. The thermodynamical nonequilibrium plasma came to be a temperature-equilibrium one as approaching the plate because the plasma flow tended to stagnate just in front of the plate. The electron temperature had a small radial variation. Both the electron number density and the heat flux decreased radially outward except for the electron density for N_2, and an increase in H_2 mole fraction raised them at a constant radial position because of increasing tank pressure. Although the electron number density for N_2 was the much highest at a constant radial position, the heat flux was the lowest. This is expected because the enthalpy for N_2 is the lowest owing to no H-atoms and the lowest tank pressure. Although the electron number density for NH_3 was relatively low, the electron temperature was the highest. Therefore, the heat flux for NH_3 is expected to be the highest because of the high enthalpy by a large amount of high temperature H-atoms and the highest tank pressure. In nitriding experiments, in cases with NH_3 and a mixture of N_2+3H_2, hard TiN-rich surfaces were made even at a large radial position of 50 mm. A neutral radical of NH with a radially wide distribution is expected to contribute to the better nitriding as a chemically active and no heating process.
机译:进行了光谱和静电探针测量,以检查低压环境下超音速直流电弧等离子体射流发生器氮化后钛板附近的等离子体特性。还用镍塞和热电偶布置评估了从等离子体进入板的热通量。使用氨以及氮和氢的混合物作为工作气体。在N_2 + nH_2的混合物中,H_2的摩尔分数n从0变为3,其中0和3的摩尔分数分别对应于纯氮和模拟氨。热力学非平衡等离子体在接近板时成为温度平衡的,因为等离子流趋于停滞在板的前面。电子温度具有小的径向变化。除N_2的电子密度外,电子数密度和热通量都沿径向向外减小,并且由于罐压力的增加,H_2摩尔分数的增加使它们在恒定的径向位置处升高。尽管在恒定的径向位置上N_2的电子数密度最高,但热通量最低。这是可以预期的,因为由于没有H原子和最低的储罐压力,N_2的焓是最低的。尽管NH_3的电子数密度相对较低,但电子温度最高。因此,由于大量的高温H原子产生的高焓和最高的罐压力,预计NH_3的热通量最高。在氮化实验中,在使用NH_3和N_2 + 3H_2的混合物的情况下,即使在50mm的较大径向位置上,也可以制成富含TiN的硬表面。 NH呈放射状分布的中性自由基有望作为化学活性且无需加热的过程有助于更好的氮化。

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