Face-centered cubic (cF)#

Atom arrangement#

0

Figure 1: Face-centered cubic lattice structure

Slip systems#

index

slip direction

plane normal

1

[011¯]

(111)

2

[1¯01]

(111)

3

[11¯0]

(111)

4

[01¯1¯]

(1¯1¯1)

5

[101]

(1¯1¯1)

6

[1¯10]

(1¯1¯1)

7

[01¯1]

(11¯1¯)

8

[1¯01¯]

(11¯1¯)

9

[110]

(11¯1¯)

10

[011]

(1¯11¯)

11

[101¯]

(1¯11¯)

12

[1¯1¯0]

(1¯11¯)

{111} fcc slip system

Figure 2: {11¯1} octahedral slip system

index

slip direction

plane normal

13

[110]

(11¯0)

14

[11¯0]

(110)

15

[101]

(101¯)

16

[101¯]

(101)

17

[011]

(011¯)

18

[011¯]

(011)

{110} fcc slip system

Figure 3: {110} non-octahedral slip system

Twin systems#

index

slip direction

plane normal

1

[2¯11]

(111)

2

[12¯1]

(111)

3

[112¯]

(111)

4

[21¯1]

(1¯1¯1)

5

[1¯21]

(1¯1¯1)

6

[1¯1¯2¯]

(1¯1¯1)

7

[2¯1¯1¯]

(11¯1¯)

8

[121¯]

(11¯1¯)

9

[11¯2]

(11¯1¯)

10

[211¯]

(1¯11¯)

11

[1¯2¯1¯]

(1¯11¯)

12

[1¯12]

(1¯11¯)

{111} fcc twin system

Figure 4: {111} twin system

Cleavage systems#

index

slip direction

plane normal

1

[010]

(100)

2

[001]

(010)

3

[100]

(001)

Interaction Matrices#

Slip-Slip#

index

label

description

1

α0

self interaction

2

αcopla

coplanar interaction

3

αcoli

collinear interaction

4

α1

Hirth lock

5

α2

glissile junction

6

α2

glissile junction

7

α3

Lomer lock

8

9

10

11

12

13

  • R. Madec and L.P. Kubin. Dislocation strengthening in FCC metals and in BCC metals at high temperatures Acta Materialia, 126:166-173, 2017. doi:10.1016/j.actamat.2016.12.040.