<th id="5nh9l"></th><strike id="5nh9l"></strike><th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th><strike id="5nh9l"></strike>
<progress id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"><noframes id="5nh9l">
<th id="5nh9l"></th> <strike id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span>
<progress id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span><strike id="5nh9l"><noframes id="5nh9l"><strike id="5nh9l"></strike>
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"></span><span id="5nh9l"><video id="5nh9l"></video></span>
<th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th>
<progress id="5nh9l"><noframes id="5nh9l">

激光增材鎳基合金內部疲勞失效行為研究

Investigation of the internal failure mechanism of laser-additively manufactured nickel-based superalloy

  • 摘要: 內部失效是激光增材制造鎳基高溫合金在高溫下的典型疲勞失效模式,目前對這種失效模式的認知尚不充分. 在650 ℃下進行了不同應力比的軸向疲勞試驗,隨后采用掃描電鏡、電子背散射衍射、聚焦離子束和透射電子顯微鏡等測試技術,研究了增材制造鎳基高溫合金的多尺度內部失效行為. 結果表明,不論是否受缺陷影響,微裂紋主要從晶粒取向較軟的大晶粒處萌生,然后沿最大剪切應力方向滑移和擴展,形成晶體學小平面,因此與晶粒特征相關的小平面開裂是一種典型的內部失效模式. 對小平面裂紋附近的位錯結構進行分析,在650 ℃時,局部塑性變形是由反相邊界剪切、沉淀物旁通以及堆積層錯剪切機制的共同作用所引起的. 結合裂紋尖端應力強度因子的定義,提出了與小平面裂紋特征相關的裂紋成核壽命預測方法,預測結果與實驗結果具有較好的一致性.

     

    Abstract: Nickel-based superalloys exhibit excellent high strength and thermal fatigue resistance at 650 ℃, making them widely used for manufacturing elevated-temperature components such as turbine blades for aero-engines. Laser-powder bed fusion (L-PBF) is a rapidly developing metal additive manufacturing technology that is increasingly important for producing nickel-based superalloy products. The design and service life of aero-engine turbine blades typically require more than 107 load cycles. Therefore, it is crucial to investigate the very-high-cycle fatigue characteristics of L-PBF nickel-based superalloys at increased temperatures. Internal failure is a common elevated-temperature fatigue mode of L-PBF nickel-based superalloys that is currently not well understood. To address this issue, first, axial fatigue tests with stress ratios of ?1 and 0.1 are conducted at 650 ℃. Specifically, partial typical internal failure fractures at a stress ratio of 0.1 are selected as the focus of this study. Second, scanning electron microscopy and ultra-depth field microscopy are employed to observe the 2D and 3D morphology of the fatigue fracture surfaces and analyze the crack nucleation areas and growth paths. The results show that irrespective of the presence of defects, the emergence and aggregation of numerous facets occur in the “facetted cracking area (FCA),” a typical internal failure characteristic of L-PBF nickel-based superalloys. Measurements indicate that the size of these facets leading to cracking is comparable to that of large grains and correlates with variations in grain orientation. Therefore, internal failures are categorized into two modes of cracking: “defect-assisted faceted cracking” and “non-defect-assisted faceted cracking.” Third, the FCA exhibiting typical internal failure fractures is sectioned and subjected to electron backscatter diffraction analysis to observe surface and subsurface crystallographic features related to crack nucleation and growth behavior. The analysis reveals that microcracks mainly originate from large grains with softer orientations, propagate through slips, expand along the direction of maximum shear stress, and ultimately form a perforated fracture pattern. Fourth, subsurface microcrack features beneath the FCA are examined via focused ion beam milling and imaging. Transmission electron microscopy is then employed to observe slip bands and dislocation structures near the microcracks. The results confirm that the fatigue deformation mechanism of facets at 650 ℃ is mainly controlled by a combination of anti-phase boundary shearing, precipitate bypassing, and stacking fault shearing. This mechanism is especially evident under stress concentration effects induced by cracks or defects. Finally, according to the definition of the crack tip stress intensity factor, a crack nucleation life prediction method that accounts for the characteristics of faceted cracks is proposed. The predicted results align well with the experimental findings.

     

/

返回文章
返回
<th id="5nh9l"></th><strike id="5nh9l"></strike><th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th><strike id="5nh9l"></strike>
<progress id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"><noframes id="5nh9l">
<th id="5nh9l"></th> <strike id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span>
<progress id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span><strike id="5nh9l"><noframes id="5nh9l"><strike id="5nh9l"></strike>
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"></span><span id="5nh9l"><video id="5nh9l"></video></span>
<th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th>
<progress id="5nh9l"><noframes id="5nh9l">
259luxu-164