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Acta Metall Sin  2018, Vol. 54 Issue (11): 1503-1524    DOI: 10.11900/0412.1961.2018.00342
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High-Resolution Transmission Electron Microscopic Study of Various Borides Precipitated in Superalloys
Xiuliang MA(), Xiaobing HU
Institute of Metal Research, Chinese Academy of Sciences, Shenyang 110016, China
Cite this article: 

Xiuliang MA, Xiaobing HU. High-Resolution Transmission Electron Microscopic Study of Various Borides Precipitated in Superalloys. Acta Metall Sin, 2018, 54(11): 1503-1524.

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Abstract  

Microelement B is widely added into almost all commercial superalloys because B contributes to strengthening grain boundaries at high temperature during service. Generally, B is present in two different forms. Besides the solute state in matrix, B tends to react with transition elements at high temperatures, giving rise to various borides including M2B, M3B2 and M5B3 phases. An accurate knowledge of the microstructural characterizations of these borides is of great importance for a better understanding of the structure-property relationship and designing materials with improved properties. By means of various advanced techniques based on the aberration-corrected transmission electron microscopy (TEM), microstructural features of above borides have been systematically investigated. Various defect features which were controversial in the past have been clarified. In this paper, after a brief review on the studies of borides, the atomic-scale information on the microstructural features has been presented. Finally, some prospects for future studies have been proposed.

Key words:  superalloy      boride      crystallographic feature      polyhedral stacking      transmission electron microscopy     
Received:  23 July 2018     
ZTFLH:  TG146.1  
Fund: Supported by National Basic Research Program of China (Nos.2009CB623705 and 2010CB631206) and National Natural Science Foundation of China (No.11327901)

URL: 

https://www.ams.org.cn/EN/10.11900/0412.1961.2018.00342     OR     https://www.ams.org.cn/EN/Y2018/V54/I11/1503

Structure Space group Lattice parameter Atom (Wyckoff Fractional coordinate
nm position) x y z
W2B I4/mcm a=0.56 W (8h) 0.169 0.669 0.000
C16 (No.140) c=0.47 B (4a) 0.000 0.000 0.250
V3B2 P4/mbm a=0.57 V (4h) 0.173 0.673 0.500
D5a (No.127) c=0.30 V (2a) 0.000 0.000 0.000
B (4g) 0.388 0.888 0.000
Cr5B3 I4/mcm a=0.55 Cr (16l) 0.166 0.666 0.150
D81 (No.140) c=1.06 Cr (4c) 0.000 0.000 0.000
B (8h) 0.625 0.125 0.000
B (4a) 0.000 0.000 0.250
Table 1  Crystallographic data of W2B, V3B2 and Cr5B3 phase[32]
Fig.1  Structural configurations of M3B2 (a), M5B3 (b) and M2B (c) (The basic polyhedral unit of trigonal prisms and anti-square prisms for each structure are shadowed)[32]
Structure Space group Lattice parameter Atom (Wyckoff Fractional coordinate
nm position) x y z
Cr2B I4/mcm a=0.52 Cr (8h) 0.167 0.667 0.000
C16 (No.140) c=0.43 B (4a) 0.000 0.000 0.250
Cr2B Fddd a=1.47 Cr (16e) 0.917 0.000 0.000
Cb (No.70) b=0.74 Cr (16f) 0.000 0.333 0.000
c=0.43 B (16e) 0.373 0.000 0.000
Cr2B P6222 a=0.43 Cr (6f) 0.500 0.000 0.390
Ca (No.180) c=1.09 Cr (6j) 0.166 0.332 0.500
β=120° B (3a) 0.000 0.000 0.333
B (3c) 0.500 0.500 0.333
Table 2  Crystallographic data of C16-, Cb- and Ca-Cr2B phases[33]
Fig.2  Pictorial diagram of square anti-prism (a), structural projection along fourfold axis (b) and twofold axis (c)
Fig.3  Schematic diagram showing the directional equivalence among C16-, Cb-, and Ca-Cr2B in the conjunct plane of (110)C16, (100)Cb and (001)Ca (a), the structural projection of orthorhombic Cb-M2B along [011]Cb (b) and [011?]Cb (c), tetragonal C16-Cr2B along [001]C16 (d), and hexagonal Ca-Cr2B along [110]Ca (e), [100]Ca (f) and [010]Ca (g) directions showing the polyhedral configuration in each structure[33]
Fig.4  Structural projection along [100]Ca for Ca-Cr2B (a) and the corresponding simplified description (b), structural simplification of [001]C16 (c), [11?1]C16 (d), [001]Cb (e), [011]Cb (f) and [001]N2 (g) (The atomic fractional coordinates along the projected direction, and characteristic projected lengths for the basic structure units of A, A, B and B are indicated. The indicated ao and bo direction in Fig.4c is based on the basic unified orthorhombic lattice. The denoted 2d, 3d, 4d, 6d represent the periods along the stacking direction of ao for C16-, Cb-, Ca- and N2-Cr2B structure respectively, in which d is the lattice length of ao. The denoted layer α1, α2, β1, β2 in Fig.4g represents four different stacking layers)[33]
Fig.5  Structural derivation for the polytypic Cr2B (N represents the number of stacking layers)[33]
Fig.6  Dark (a) and bright (b) field TEM images showing the M2B precipitates within the matrix (γ /γ’)
Fig.7  A series of electron diffraction patterns (EDPs) of a M2B-type boride obtained by large-angle tilting with [001] (a), [102] (b), [101] (c), [100] (d), [113] (e), [111] (f), [110] (g) and [210] (h) zone axis (A C16-type M2B with the space group of I4/mcm is determined according to the EDPs. The square-framed diffraction spots are proposed to result from double-diffraction)[31]
Fig.8  A series of EDPs of a M2B-type boride obtained by large-angle tilting with [100] (a), [101] (b), [103] (c), [001] (d), [310] (e), [110] (f), [010] (g), [011] (h) and [013] (i) zone axis (A Cb-type M2B with the space group of Fddd is determined according to the EDPs. The square-framed diffraction spots are proposed to result from double-diffraction)[31]
Fig.9  EDPs (a~c) obtained from highly defected regions within M2B, schematics of the EDPs for C16 along [001]C16 (d) and [11?1]C16 (e), and Cb along [001]Cb (f) and [011]Cb (g)
Fig.10  HAADF image (a), STEM-EDX spectrum (b) and TEM-EELS (c) showing the grain interior precipitation and chemical features of the lath-like M2B-type boride
Fig.11  Schematic showing the crystallographic relationship of various orientations within (110)C16 and (100)Cb (a), and schematics showing the distribution of reflections along [010]Cb (b) and [11?3]C16 (c), respectively
Fig.12  Dark field TEM image showing the 60° rotation twin within a M2B grain (a), EDPs corresponding to area I can be indexed as [001]C16 (b), [11?3]C16 (c) and [11?1]C16 (d) zone-axis, respectively. EDPs obtained from area II with the same tilt angles as Figs.12b~d corresponding to [11?1]C16 (e), [11?0]C16 (f) and [11?1?]C16 (g) zone-axis, respectively[31]
Fig.13  HRTEM image of a C16 structure including stacking fault along [001]C16 direction (a) and magnified image of rectangle in Fig.13a (b)[31]
Fig.14  HRTEM image of a C16 structure including stacking fault along [11?0]C16 direction (a) and magnified image of rectangle in Fig.14a (b)[31]
Fig.15  HRTEM image taken along [013]Cb direction showing details of a 60° rotation twin in Cb structure (a), <011>Cb lattice image taken from the same area as in Fig.15a but with a 30° tilting angle along [001]Cb direction (b), [001]Cb HRTEM image of Cb structure with stacking fault indicated by the arrow (c) (The oblique lines in Figs.15a and c correspond to (101)Cb and (110)Cb, respectively)[31]
Fig.16  Atomic resolution HAADF images (a~d) showing various kinds of structural intergrowth in M2B-type boride[33]
Fig.17  Atomic resolution HAADF image showing the long period stacking order (LPSO) structure with the uncertain period number of 6 or 12 or 18 or even bigger[33]
Fig.18  A series of EDPs of a M3B2-type boride obtained by large-angle tilting with [001] (a), [101] (b), [201] (c), [100] (d), [112] (e), [111] (f), [110] (g) and [210] (h) zone axes
Fig.19  TEM bright filed image showing the M3B2 precipitates in grain interior (a) and EDX spectrum corresponding to M3B2 (b)
Fig.20  Atomic resolution HAADF images along [001] (a), [100] (b) and [110] (c) showing the ordered occupation of metal atoms M in M3B2 phase. Atomic configuration in the unit cell of the ordered M3B2 phase (d) and the corresponding projection along [001] (e), [100] (f), and [110] (g) showing the structural features of the ordered structure (The blue balls designated by L represent large metal atoms such as W and Mo. The green balls designated by S represent small metal atoms such as Cr, Co. The B atoms are indicates by red balls)[32]
Fig.21  Direct determination of the chemical ordering within M3B2-type borides using element maps of Cr-K (a), Co-K (b), Ni-K (c), W-M (d), Mo-L (e), and composite map using Cr-K and W-M (f) edges[35]
Fig.22  HRTEM image along [110] direction showing the planar defect in M3B2
Fig.23  Local intergrowth of polyhedral layer within M3B2 boride[32]
Fig.24  A series of EDPs of a M5B3-type boride obtained by large-angle tilting with [001] (a), [101] (b), [301] (c), [100] (d), [111] (e), [221] (f), [110] (g), and [210] (h) zone axes (The square-framed reflections are resulted from double-diffraction)
Fig.25  BF-STEM image (a) and EDX spectrum (b) showing the grain interior precipitation and chemical composition of M5B3-type boride
Fig.26  Atomic resolution HAADF images taken along [001] (a), [100] (b) and [110] (c) direction showing the ordered occupation of metal atoms M in M5B3 phase. Atomic configuration in the unit cell of the ordered M5B3 phase (d) and the corresponding projection along [001] (e), [100] (f) and [110] (g) showing the structural features of the ordered structure (The blue balls designated by L represent large metal atoms such as W and Mo. The green balls designated by S represent small metal atoms such as Cr, Co. The B atoms are indicates by red balls)[32]
Fig.27  Element maps using Cr-K (a), Co-K (b), Ni-K (c), W-M (d), Mo-L (e), and composite map using Cr-K and W-M (f) showing the chemical ordering within M5B3-type boride[35]
Fig.28  HRTEM image along [110] direction showing the planar defect within M5B3 phase (The top right inset is a FFT image)
Fig.29  Atomic resolution HAADF images along [110] (a), and [100] (b) zone axes showing the local intergrowth of polyhedral layer within M5B3 boride[32]
Fig.30  Low magnification HAADF image (a), the corresponding composite EDPs (b) and atomic resolution HAADF image (c) showing the large scale intergrowth between M3B2 and M5B3 boride
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