材料研究学报, 2026, 40(3): 161-168 DOI: 10.11901/1005.3093.2025.237

研究论文

Sn含量对DD26单晶高温合金组织与性能的影响

金师行1,2, 梅松3, 卢玉章2, 黄亚奇2, 郑伟2, 申健,2, 张健,2

1.中国科学技术大学材料科学与工程学院 合肥 230026

2.中国科学院金属研究所 沈阳 110016

3.上海科技大学 智造系统工程中心 上海 201210

Effect of Sn on Microstructure and Properties of DD26 Nickel-based Single Crystal Superalloy

JIN Shihang1,2, MEI Song3, LU Yuzhang2, HUANG Yaqi2, ZHENG Wei2, SHEN Jian,2, ZHANG Jian,2

1.School of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China

2.Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China

3.Center for Adaptive System Engineering, ShanghaiTech University, Shanghai 201210, China

通讯作者: 申健,研究员,shenjian@imr.ac.cn,研究方向为单晶高温合金先进定向凝固技术;张健,研究员,jianzhang@imr.ac.cn,研究方向为单晶叶片材料及先进制备技术

收稿日期: 2025-07-23   修回日期: 2025-10-22  

基金资助: 国家重点研发计划(2021YFB3702900)
中国科学院金属研究所创新基金(2024-PY04)
辽宁省科学技术计划(2022JH2/101300226)

Corresponding authors: SHEN Jian, Tel: 13804984964, E-mail:shenjain@imr.ac.cn;ZHANG Jian, Tel: 13840053283, E-mail:jianzhang@imr.ac.cn

Received: 2025-07-23   Revised: 2025-10-22  

Fund supported: National Key Research and Development Program of China(2021YFB3702900)
IMR Innovation Fund(2024-PY04)
Science and Technology Program of Liaoning Province(2022JH2/101300226)

作者简介 About authors

金师行,男,2002年生,硕士生

摘要

用液态金属冷却(LMC)定向凝固工艺制备4种不同Sn含量(质量分数分别为0%、0.01%、0.05%、0.10%)的DD26镍基单晶高温合金,研究了Sn含量对其铸态和完全热处理态的显微组织、室温拉伸性能和975 ℃/255 MPa持久性能的影响。结果表明:随着Sn含量的提高DD26单晶合金的一次枝晶间距、γ/γ′共晶组织的含量、γ′相的平均尺寸和体积分数都没有显著的变化。铸态合金中的Sn元素与Ni基体元素未形成化合物,Sn以固溶态在枝晶间的γ/γ′共晶组织周围偏析,热处理使Sn元素的偏析消失而均匀地分布在合金中。Sn的添加对DD26单晶合金的室温拉伸性能和975 ℃/255 MPa持久性能的影响较小。

关键词: 金属材料; 镍基单晶高温合金; 液态金属冷却工艺; Sn元素; 组织; 力学性能

Abstract

Four DD26 nickel-based single-crystal superalloys with varying Sn contents (mass fractions of 0%, 0.01%, 0.05%, and 0.10%) were prepared using liquid metal cooling (LMC) directional solidification process. The influence of Sn-amount on the microstructures, as well as the room-temperature tensile properties and stress rupture properties tested under 975 oC/255 MPa was investigated for the as-cast and heat-treated alloys. It was found that there was no significant change in primary dendrite arm spacing, γ/γ′ eutectic content, or the average size and volume fraction of the γ′ phase in DD26 single crystal superalloys with the increase of Sn content. No compounds involving Sn and Ni formed in as-cast alloy, and the Sn segregated around the γ/γ′ eutectic structures in the interdendritic regions. After heat treatment, the segregation of Sn disappeared and Sn distributed uniformly throughout the alloy. No measurable effect on either the tensile properties or the stress rupture performance of DD26 single crystal superalloys was observed with the addition of Sn.

Keywords: metallic materials; nickel-based single crystal superalloy; liquid metal cooling processing; Sn; microstructure; mechanical property

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本文引用格式

金师行, 梅松, 卢玉章, 黄亚奇, 郑伟, 申健, 张健. Sn含量对DD26单晶高温合金组织与性能的影响[J]. 材料研究学报, 2026, 40(3): 161-168 DOI:10.11901/1005.3093.2025.237

JIN Shihang, MEI Song, LU Yuzhang, HUANG Yaqi, ZHENG Wei, SHEN Jian, ZHANG Jian. Effect of Sn on Microstructure and Properties of DD26 Nickel-based Single Crystal Superalloy[J]. Chinese Journal of Materials Research, 2026, 40(3): 161-168 DOI:10.11901/1005.3093.2025.237

镍基单晶高温合金的高温抗氧化性优异和综合力学性能良好,是制造先进航空发动机和燃气轮机涡轮叶片的首选材料[1~7]。制备单晶叶片的定向凝固,是关键工序之一[8~11]。温度梯度是定向凝固的重要参数。在传统的定向凝固工艺(High rate solidification,HRS)中热量发生热辐射散失,凝固后期的温度梯度和冷却速率不断降低,产生严重的组织粗化和凝固偏析。液态金属冷却工艺(Liquid metal cooling,LMC)的主要传热方式是热传导,可显著提高固液界面前沿的温度梯度和细化单晶叶片的组织[12~17]、降低偏析、减小缩孔的尺寸和数量以及减少冶金缺陷,从而提高其力学性能[18~21]。

目前国内外工程化应用的LMC工艺中,冷却介质有Al和Sn。Sn的熔点(232 ℃)比Al的熔点(660 ℃)低,因此使用Sn作为冷却介质的LMC工艺其温度梯度更高。与传统HRS定向凝固工艺比较,LMC-Al的温度梯度提高了约30% (即60 ℃/cm),而LMC-Sn的温度梯度则大幅度提高到80~120 ℃/cm[12~14]。

虽然LMC-Sn工艺的温度梯度比传统的HRS和LMC-Al工艺的温度梯度高,但是LMC-Sn工艺中微量的冷却介质Sn可能进入铸件而将其污染[22]。随着LMC-Sn工艺应用的推广,Sn污染越来越受到关注。但是研究表明,在Sn含量为0.104% (质量分数,下同) 和不含Sn的SC16单晶合金中γ′析出相的形状、尺寸和体积分数没有显著的差异[23]。研究发现,即使SC16和PWA 1483两种单晶合金中Sn的含量高达0.415%,其蠕变强度和低周疲劳强度也没有受到显著的影响[23]。Dreshfield等[24]研究掺杂Sn的Inconel 718合金时也发现,在含Sn合金中并未产生新的析出相或不良显微组织。合金中Sn的含量为0.08%或更低,对合金的室温、425 ℃和650 ℃的拉伸性能几乎没有影响;在650 ℃施加469 MPa、579 MPa、793 MPa的应力条件下,含量低于0.08%的Sn对合金的持久寿命几乎没有影响;但是Sn质量分数高到1%时,793 MPa下的寿命大幅降低。在早期的研究中也有类似的结果[25]。因此,对高温合金中微量Sn的影响仍然存在争议,相关机理并不清楚。同时,高温合金的性能取决于组织,而目前国内外对Sn元素在高温合金中的存在形式和演化缺少系统的研究。鉴于此,本文以Sn为LMC定向凝固工艺的冷却介质制备不同Sn含量的DD26单晶高温合金试棒,系统研究其对DD26镍基单晶高温合金的组织和性能的影响。

1 实验方法

采用LMC-Sn定向凝固工艺制备DD26单晶试棒,熔炼母合金时分别不加或加入质量分数为0.01%、0.05%、0.10%的Sn (下文简称0%Sn合金、0.01%Sn合金、0.05%Sn合金、0.10%Sn合金。四种合金中Sn含量的实测结果分别为< 0.0001%、0.013%、0.052%、0.11%)。

选取DD26单晶晶体取向偏离[001]方向15°以内的单晶试棒,用真空热处理炉对其进行标准热处理,热处理制度为1260 ℃ ± 10 ℃/2 h,空冷+ 1080 ℃ ± 10 ℃/2 h,空冷+ 870 ℃/24 h,空冷[26]。使用差示扫描量热仪(DSC)对不同Sn含量的单晶合金进行差热分析,结合金相法测定合金的相变点和固、液相线温度。测试DSC时从室温升温到1000 ℃,升温速率为40 ℃/min,再从1000 ℃升温到1450 ℃,升温速率为10 ℃/min,降温时从1450 ℃降到1000 ℃,降温速率为10 ℃/min,再从1000 ℃降到室温,降温速率为40 ℃/min。

用Zeiss Axiovert 200MAT型光学显微镜、TESCANCLARA 2023扫描电子显微镜和电子探针观察合金铸态和完全热处理态的显微组织;使用Image-J和Image-Pro Plus软件计算γ′强化相的平均尺寸和体积分数、一次枝晶间距和γ/γ′共晶组织的含量。对铸态和热处理态样品,至少统计3个视场的数据取其结果的平均值。

分别测量合金的室温拉伸性能和975 ℃/255 MPa高温持久性能,测量室温拉伸性能的样品尺寸为M10 mm× Φ5 mm,每种Sn含量的样品2根;测量975 ℃/255 MPa高温持久性能的样品尺寸为M14 mm × Φ5 mm,每种Sn含量的样品3根。用差热分析法表征不同Sn含量铸态合金的相变温度。

2 结果和讨论

2.1 Sn含量对合金相变温度的影响

图1给出了4种不同Sn含量DD26合金的DSC降温曲线。可以看出,不同Sn含量的DD26合金在降温中发生的相变过程相似,表1列出了单晶合金的开始熔化、碳化物析出峰值温度和γ/γ′共晶析出的峰值温度(数据来源于图1)。0%Sn合金、0.01%Sn合金、0.05%Sn合金和0.10%Sn合金中γ/γ′共晶析出的开始温度、峰值和结束温度较为接近,添加0.10%的Sn对合金的相变温度没有显著的影响。

图1

图1   不同Sn含量合金的差热分析曲线

Fig.1   DTA curves of Sn-containing alloys during cooling process


表1   在降温过程中Sn含量对合金相变温度的影响

Table 1  Effect of Sn content on phase transformation temperatures during cooling

Alloyγ/γ′ precipitation/ oCCarbides / oCLiquidus / oC
0%Sn alloy121913341393
0.01%Sn alloy122113331391
0.05%Sn alloy122513351385
0.10%Sn alloy122413341390

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2.2 Sn对DD26合金铸态组织的影响

2.2.1 DD26合金的显微组织

图2给出了不同Sn含量铸态DD26合金的枝晶组织。可以看出,4种合金的铸态组织均呈现典型的十字形枝晶形貌,枝晶间分布有白色γ/γ′共晶组织。不同Sn含量合金的一次枝晶间距和γ/γ′共晶组织的体积分数如图3所示。可以看出,不同Sn含量的铸态合金中一次枝晶间距和γ/γ′共晶组织的体积分数相近。这表明,即使合金的Sn含量高达0.10%,对铸态合金的枝晶参数也没有显著的影响。

图2

图2   不同Sn含量铸态合金的枝晶组织

Fig.2   Dendritic microstructures of as-cast alloys with different Sn contents (a) 0%Sn alloy, (b) 0.01%Sn alloy, (c) 0.05%Sn alloy, (d) 0.10%Sn alloy


图3

图3   不同Sn含量铸态合金中的一次枝晶间距和共晶的体积分数

Fig.3   Primary dendrite arm spacing and eutectic volume fraction in as-cast alloys with varying Sn contents


图4给出了不同Sn含量(0.01%Sn合金、0.05%Sn合金、0.10%Sn合金)铸态DD26合金的枝晶干和枝晶间γ′相的形貌。可以看出,铸态组织中的枝晶干、枝晶间的γ′相呈细小、规则的立方体形状。与枝晶干相比,枝晶间的γ′相更为粗大。不同Sn含量铸态合金中枝晶干和枝晶间区域的γ′相体积分数和平均尺寸的统计结果,在图5中给出。可以看出,合金中Sn的含量高达0.10%,对铸态合金的显微组织也没有太大的影响。

图4

图4   不同Sn含量铸态合金中的枝晶干、枝晶间γ′相的形貌

Fig.4   Morphology of γ′ phase in dendrite core and interdendritic regions of as-cast alloys with different Sn contents (a) 0.01%Sn dendrite core, (b) 0.05%Sn dendrite core, (c) 0.10%Sn dendrite core, (d) 0.01%Sn interdendritic region, (e) 0.05%Sn interdendritic region, (f) 0.10%Sn interdendritic region


图5

图5   不同Sn含量铸态合金中的枝晶干和枝晶间γ′相的体积分数和平均尺寸

Fig.5   Volume fraction and average size of γ′ phase in dendrite core (a) and interdendritic regions (b) of as-cast alloys with varying Sn contents


2.2.2 Sn元素在DD26合金中的分布

图6给出了0.10%Sn铸态DD26合金中各个元素的分布。可以看出,Sn元素在γ/γ′共晶组织周围偏析,图6中(a)区域的局部放大在图7中给出。可以看出,Sn元素主要偏析在γ/γ′共晶外围,Sn没有在碳化物和硼化物中偏聚。在Sn含量较高的区域,没有发现含Sn的析出相。

图6

图6   0.10%Sn铸态合金中元素的分布

Fig.6   Element distribution mapping of 0.10%Sn as-cast alloy


图7

图7   图6中(a)区域放大后的元素分布

Fig.7   Element distribution mapping of the magnified region (a) in Fig.6


进一步定量分析了图7中所示区域的元素分布。图8给出的放大图表明,1区域为γ/γ′共晶,2区域为碳化物,3区域为硼化物,4区域为Sn元素富集区,各区域的元素占比列于表2。在Sn富集区,Sn元素的原子分数为3.68%,Ni元素的原子分数为64.06%。如果只考虑Ni和Sn两种元素,在0.1%Sn合金的Sn富集区中Ni-Sn成分约为Ni94.6Sn5.4 (原子分数,%)。根据图9中的Ni-Sn二元相图[27],Ni元素的原子分数为94.57%时,在从液相降温到约600 ℃的凝固过程中并不会与Ni元素生成化合物,继续降温时进入了相图中的两相区,但是因为凝固速率较高难以生成析出相。这表明,铸态合金中Sn元素与Ni基体元素没有生成化合物,只是偏析在枝晶间的γ/γ′共晶组织周围。

图8

图8   Sn元素的聚集区域

Fig.8   Segregation region of Sn element


表2   各区域中元素的占比

Table 2  Elemental composition analysis of different regions (atomic fraction, %)

RegionNiSnTiAlCBCrCoNbWMoHf
161.240.342.4614.258.90-3.577.010.841.40--
252.29-1.978.8216.88-6.118.141.823.060.680.24
310.060.400.550.937.9345.1815.352.861.066.619.07-
464.063.681.686.827.37-5.127.90-1.30-2.06

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图9

图9   Ni-Sn二元相图[27]

Fig.9   Ni-Sn binary phase diagram[27]


2.3 固溶态DD26合金中Sn元素的分布

图10给出了0.10%Sn合金固溶热处理后的电子探针结果。可以看出,固溶热处理后,原来铸态合金Sn元素在共晶周围的偏析消失,Sn元素在合金中的分布较为均匀。

图10

图10   0.10%Sn合金固溶热处理后元素的分布

Fig.10   Element distribution mapping of 0.10%Sn alloy after solution heat treatment


计算了0.10%Sn合金在固溶热处理(1260 ℃)过程中Sn元素的扩散行为。采用一维扩散模型,基于Fick第二定律的高斯解定性计算了合金元素扩散距离的均方根(Root mean square displacement,xrms)。一维扩散模型适用于描述固溶热处理过程中合金元素(本文中主要计算Sn元素)从枝晶间局部偏聚转变为均匀分布的扩散过程。

根据Fick第二定律,扩散过程可用

∂C∂t=D∂2C∂x2

描述。其中C为Sn元素的浓度(mol/m³);t为时间(s);D为扩散系数(m2/s);x为扩散距离(m)。

对于初始时刻t = 0时的浓度分布C(x,0),假设Sn元素在枝晶间局部区域的初始浓度较高,而在其他区域的浓度较低。经过时间t后,浓度分布趋于均匀。

用高斯法求解Fick第二定律,即 式(1),得到的解为

Cx, t=C04πDtexp-x24Dt

式中的浓度分布与标准高斯概率密度函数

fx=1σ2πexp -x22σ2

的数学形式相同。比较指数项系数可得

x24Dt=x22σ2

解得扩散过程的方差表达式为

σ2=2Dt

均方根位移(Root mean square displacement,xrms)定义为标准差σ,则

xrms=σ=2Dt

其中xrms为Sn原子扩散的平均距离,是统计学意义上的特征长度。

扩散系数遵循Arrhenius定律[28]

DT=D0exp-QRT

其中D0为前置因子(m2/s),Q为扩散活化能(J/mol),R为气体常数(8.314 J/(mol·K)),T为绝对温度(K)。

固溶热处理温度为1260 ℃,即TSolid = 1533 K,扩散相关参数基于Neumann等关于镍合金中杂质元素扩散的研究[29],其中Sn元素在镍合金中的扩散参数为D0 = 4.56 × 10-4 m2/s,Q = 2.673 × 105 J/mol。

在1260 ℃阶段(TSolid = 1533 K,t = 7200 s),将TSolid = 1533 K代入Arrhenius方程

DTSolid=D0exp-QRTSolid

可计算固溶温度下的扩散系数3.555 × 10-13 m2/s。计算结果表明,扩散距离为

xrms=2DTSolidt

可定性计算出Sn元素在热处理过程中的扩散距离约为71.55 μm。结合图6和图7所示的Sn元素富集区空间分布,此扩散距离横跨枝晶间区域,显著超越初始偏聚区尺度,从而合理地解释了Sn元素从枝晶间偏聚区域向均匀分布的扩散过程。结果表明,固溶热处理后,在铸态条件下Sn元素在共晶周围的偏析消失,在合金中的分布较为均匀(图10)。

2.4 Sn对DD26合金性能的影响

图11给出了不同Sn含量DD26合金的室温拉伸性能。可以看出,不同Sn含量DD26单晶合金的抗拉强度分别为(1050.0 ± 70.0) MPa,(959.0 ± 27.0) MPa,(1114.5 ± 19.5) MPa,(1013.5 ± 96.5) MPa,延伸率分别为(13.0 ± 2.0)%,(12.0 ± 1.0)%,(11.25 ± 0.3)%,(11.5 ± 3.5)%。这表明,即使合金的Sn含量高达0.10%,对其室温拉伸性能也没有显著的影响。不同Sn含量合金的975 ℃/255 MPa高温持久性能,如图12所示。可以看出,不同Sn含量合金的高温持久寿命分别为(53.1 ± 0.3) h,(58.7 ± 3.0) h,(56.7 ± 4.3) h,(53.0 ± 2.0) h。这表明,合金的持久寿命相差不大,即高达0.10%的Sn含量对合金的高温持久性能也没有显著的影响。其原因是,拉伸和持久性能主要取决于析出相,而添加Sn对铸态单晶合金的一次枝晶间距、γ/γ′共晶含量、γ′相的平均尺寸和体积分数都没有显著的影响。虽然0.10%Sn铸态合金中Sn偏析在枝晶间共晶组织周围,但是热处理已经将其消除。这表明,即使合金中Sn元素的含量高达0.10%,对服役前合金的组织几乎没有影响。这表明,在合金中添加Sn对其室温拉伸性能、975 ℃/255 MPa高温持久性能的影响不大。

图11

图11   不同Sn含量合金的室温拉伸性能

Fig.11   Room temperature tensile properties of alloys with different Sn contents


图12

图12   不同Sn含量合金的975 ℃/255 MPa持久性能

Fig.12   Creep properties of alloys with different Sn contents at 975 oC/255 MPa


3 结论

(1) 含量为0.01%、0.05%、0.10%的Sn元素对铸态DD26单晶高温合金的熔化温度、碳化物析出峰值温度和γ/γ′共晶析出峰值温度的影响不大。Sn含量对铸态单晶合金中的一次枝晶间距、γ/γ′共晶含量、γ′相的平均尺寸和体积分数没有显著的影响。

(2) 在铸态0.10%Sn合金中Sn元素在共晶外围富集,没有生成含Sn化合物。热处理后合金中Sn元素的富集消失,Sn元素均匀地分布在合金中。

(3) 含量高达0.10%的Sn元素,对DD26单晶合金的室温拉伸性能和975 ℃/255 MPa高温持久性能没有影响。

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