晶粒长大对高纯<strong>Al {111}/{111}</strong>近奇异晶界的影响

晶粒长大对高纯Al {111}/{111}近奇异晶界的影响

冯小铮, 王卫国, Gregory S. Rohrer, 陈松, 洪丽华, 林燕, 王宗谱, 周邦新

Effects of Grain Growth on the {111}/{111} Near Singular Boundaries in High Purity Aluminum

FENG Xiaozheng, WANG Weiguo, Gregory S. Rohrer, CHEN Song, HONG Lihua, LIN Yan, WANG Zongpu, ZHOU Bangxin

表3 再结晶高纯Al在500℃保温期间具有<111>/θ取向差关系不相邻晶粒及其邻近各晶粒取向统计(对应图7)

Table 3 Orientation statistics of the grains around the nonadjacent growing grains having <111>/θ misorientation in the high purity aluminum heated at 500^oC (See in Fig.7)

Grain No.	Euler angle of growing grain	Euler angle of the grain adjacent to growing grain	Misorientation between growing grain and the adjacent grain
1	(289.1° 20.1° 49°)	-	-
2		(0.8° 36.4° 84.6°)	[ $\bar{1} \bar{2} 2$ ]/36.6°
3		(170.8° 42.3° 10.5°)	[ $1 \bar{4} \bar{4}$ ]/47.5°
4		(257.9° 43.3° 16°)	[123]/40.5°
5		(79.1° 33° 64.7°)	[ $1 \bar{7} 5$ ]/52.5°
6		(343.6° 39.8° 7.1°)	[ $24 \bar{1}$ ]/32.6°
7		(358.2° 43.7° 60.3°)	[432]/43.5°
8	(145.8° 38.1° 48.8°)	-	-
1		(289.1° 20.1° 49°)	[ $11 \bar{1}$ ]/52.3°
2		(0.8° 36.4° 84.6°)	[ $\bar{2} 21$ ]/35.3°
7		(358.2° 43.7° 60.3°)	[ $6 \bar{2} \bar{3}$ ]/31.6°
10		(153.5° 47.8° 30.7°)	[ $\bar{6} \bar{5} 1$ ]/16.6°
11		(32° 47.2° 64.6°)	[ $\bar{2} 01$ ]/23.6°
12		(300.7° 26.6° 54.2°)	[ $\bar{2} \bar{1} 3$ ]/58.1°
9		(139.4° 53° 47.2°)	[ $21 \bar{1}$ ]/16.7°
13		(286.4° 25.9° 4.7°)	[ $2 \bar{1} \bar{1}$ ]/40.1°
14		(342° 32.3° 71.3°)	[ $3 \bar{1} \bar{1}$ ]/46.4°
15	(149.1° 33.3° 38.8°)	-	-
16		(334.8° 19.4° 26.3°)	[ $\bar{8} 5 \bar{1}$ ]/53.0°
17		(286.4° 32.6° 16.5°)	[ $02 \bar{3}$ ]/38.6°
18		(36.3° 32° 31.9°)	[ $\bar{3} 51$ ]/41.3°
19		(77.3° 32.1° 64.3°)	[ $3 \bar{3} \bar{2}$ ]/52.0°
20		(89.2° 30.2° 64.3°)	[ $3 \bar{3} \bar{2}$ ]/40.4°
21		(262° 44.9° 50.6°)	[ $\bar{1} \bar{3} 2$ ]/31.7°
22	(281.3° 29.4° 49.1°)	-	-
15		(149.1° 33.3° 38.8°)	[ $\bar{1} \bar{1} 1$ ]/49.1°
21		(262° 44.9° 50.6°)	[ $\bar{2} \bar{3} 0$ ]/23.8°
23		(20.2° 18.4° 57.4°)	[ $0 \bar{3} 1$ ]/38.6°
24		(92.7° 41.7° 67.3°)	[233]/44.3°
25		(236° 39.7° 25.4°)	[ $\bar{2} 1 \bar{2}$ ]/38.9°
26	(256.8° 26.1° 29.7°)	-	-
27		(268.1° 32.1° 31.3°)	[ $\bar{5} \bar{1} 7$ ]/14.1°
28		(247.6° 31.6° 37.2°)	[310]/7.1°
29		(117.8° 35.8° 22.2°)	[ $\bar{1} \bar{3} 4$ ]/52.1°
30		(203.9° 3° 82.7°)	[ $02 \bar{1}$ ]/24.4°
31		(248.3° 10.3° 57.6°)	[ $\bar{2} \bar{3} 4$ ]/25.4°
32		(207.7° 36.6° 58.9°)	[ $53 \bar{2}$ ]/30.0°
33		(168.2° 38.5° 4.5°)	[ $1 \bar{2} \bar{3}$ ]/47.0°
34		(66.4° 10.3° 65.7°)	[111]/43.9°
35		(322.3° 36.4° 41.9°)	[ $\bar{2} 0 \bar{1}$ ]/39.1°
36		(271.3° 29.1° 34.3°)	[ $8 \bar{3} \bar{2}$ ]/18.9°
37	(81.1° 30° 65.4°)	-	-
26		(256.8° 26.1° 29.7°)	[ $\bar{1} 11$ ]/52.0°
32		(207.7° 36.6° 58.9°)	[ $0 \bar{1} \bar{1}$ ]/42.8°
38		(19.1° 11.3° 65.1°)	[ $\bar{2} \bar{3} \bar{4}$ ]/40.1°
39		(29.5° 18.9° 25.5°)	[149]/23.2°
40		(38.1° 24.4° 15.7°)	[ $01 \bar{5}$ ]/20.1°
33		(168.2° 38.5° 4.5°)	[ $\bar{2} 21$ ]/48.5°