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By The Institution of Civil Engineers The Institution of Structural Engineers

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In addition to vacancy dislocation loops, SFT can also be formed (either directly by nucleation or through dissociation b e in intersecting slip planes with the formation of stair-rod dislocations and Shockley partials [30]). [111] [001 ν/[11Π121 r(11D-P'anes b) Fig. 20. c. metals: a) - atomic arrangement of a faulted loop in a (110) plane, b) - perfect loop where stacking fault has been removed by shearing of the atomic arrangement by a/6 [112]. From [13]. c. lattices. The stacking fault of imperfect loops with Burgers vector of 1/2 (110) can be unfaulted in two ways, through shear in the (100) or in the (110) direction: 1/2 [110] + 1/2 [00T] -> 1/2 [llT], 1/2 [110] + 1/2 [T10] -+ [010].

WOOD, M. : Rep. AERE-R. 10251, AERE Harwell, 1981. [55] SIMONEN, E. : J. Nucl. Mater. 133/134, 1985, 640. Suggested Further Reading Physics of Irradiation Effects in Metals, ed. , Siofok, Hungary 1991. Materials Science Forum 97-99, 1992. 3. 1 Types of Steels, their Chemical Compositions and Microstructures A steel's type is one of the most important factors affecting its radiation damage. Large differences exist in the sensitivity to radiation damage among the various types of steels and finished products (plate, worked pieces, welds, heated zones).

From [13]. 52 Radiation Damage can occur through slip, climb or self-climb by pipe diffusion mechanisms and the loop shape can change. c. lattice, b e = 1/3 ( H I ) , b s = 1/6 <112> and b p = = 1/2 (110); the stacking fault is intrinsic for vacancy loops, Fig. 19, and extrinsic for interstitial loops, Fig. 20. In addition to vacancy dislocation loops, SFT can also be formed (either directly by nucleation or through dissociation b e in intersecting slip planes with the formation of stair-rod dislocations and Shockley partials [30]).

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