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On the S-phase formation and the balanced plasma nitriding of austenitic-ferritic super duplex stainless steel

机译:奥氏体-铁素体超双相不锈钢的S相形成和平衡等离子体渗氮

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Graphical abstractDisplay OmittedHighlightsAt same temperatures, nitrogen PIII energies ruled the structure of α-γ grains.The γN(or S) phase mediated nitriding in both austenite (γ) and ferrite (α) grains.Balanced structure (γN) and mechanical behavior in both α-γ were attained at ∼401 °C.Ion energy per pulse and the γNphase formation correlated in a linear-like fashion.This correlation can be employed as a fine-tune control in the α-γ steel nitriding.AbstractThe different physical responses of austenite (γ) and ferrite (α) iron structures upon nitriding result in technical challenges to the uniform modification of α-γ materials, as the super duplex stainless steel (SDSS). The effects of voltage (7–10 kV), frequency and pulse width on the nitrogen plasma immersion ion implantation of SDSS (α∼56%, γ∼44%) were investigated, correlated with structural, morphological and mechanical analyses. By controlling the treatment power, temperatures ranged from 292 °C to 401 °C. Despite the overall increase in hardness for any of the employed parameters (from ∼6 GPa to ∼15 GPa), the structure of individual grains was strikingly dissimilar at the same temperatures, depending on the energetic conditions of implantation. Modified-α grains containing iron nitrides (ε-Fe2-3N, γ′ -Fe4N) presented intense brittleness, whereas the expanded phase γN(S-phase) laid principally in modified-γ grains, exhibiting ductile-like deformation features and thicker layers. The γNwas the dominant phase in both α-γ grains at ∼401 °C, providing them with balanced structure and mechanical behavior. These phenomena corroborate with γNas mediator of the process, through a mechanism involving the nitrogen-promoted ferrite to austenite conversion and nitrides dissolution at high temperatures. An approximately linear correlation of the γNcontent with respect to the ion energy per pulse was demonstrated, which properly embodies limiting effects to the treatment. This can be a parameter for the α-γ steel surface modification, consisting in a better adjustment to obtain more precise control along with temperature.
机译: 图形摘要 < ce:simple-para>省略显示 突出显示 在相同温度下,氮PIII能量控制着α-γ晶粒的结构。 N (或S)相介导的γ N (或S) 都是奥氏体(γ)和铁素体(α)晶粒。 两个α-γ的平衡结构(γ N )和力学性能均达到401 °C。 每个脉冲的离子能量与γ N 相形成呈线性关系。 此关联可以用作在α-γ钢氮化中进行微调控制。 摘要 氮化后奥氏体(γ)和铁素体(α)铁结构的不同物理响应给均匀改性α-γ带来了技术挑战材料,如超级双相不锈钢(SDSS)。研究了电压(7-10kV),频率和脉冲宽度对SDSS氮等离子体浸没离子注入(α〜56%,γ〜44%)的影响,并与结构,形态和力学分析相关。通过控制处理功率,温度范围为292 C至401C。尽管采用了任何一个参数(从〜6 GPa到〜15 GPa),总的硬度都有所提高,但在相同的温度下,取决于注入的能量条件,单个晶粒的结构明显不同。包含氮化铁的改性α晶粒(ε-Fe 2-3 N,γ'-Fe 4 N)表现出强烈的脆性,而膨胀相γ N (S相)主要位于改性γ晶粒中,并表现出类似延性的变形特征和更厚的层。 γ N 在〜401°C时是两个α-γ晶粒的主要相,为它们提供了平衡的结构和力学性能。这些现象通过涉及氮促进的铁素体到奥氏体转化和氮化物在高温下溶解的机理,与作为该过程介质的γ N 相证实。证明了γ N 含量相对于每个脉冲离子能量的近似线性相关性,恰当地体现了对治疗的限制作用。这可以作为α-γ钢表面改性的参数,包括进行更好的调整以获得与温度一起更精确的控制。

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