1983
DOI: 10.1016/0025-5416(83)90199-4
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Improvement of Creep strength in a nickel-base single-crystal superalloy by heat treatment

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Cited by 365 publications
(104 citation statements)
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“…In an ideal situation, with y'-rafts extending from one side of the crystal to the other in an almost perfectly regular manner, gliding/climbing around it by matrix dislocations is impossible. This conclusion is in accordance with opinions of other authors [ 1,13,21,23,24]. Another example for enhanced creep properties due to tensile pre-rafting can be found in [25].…”
Section: Introductionsupporting
confidence: 91%
“…In an ideal situation, with y'-rafts extending from one side of the crystal to the other in an almost perfectly regular manner, gliding/climbing around it by matrix dislocations is impossible. This conclusion is in accordance with opinions of other authors [ 1,13,21,23,24]. Another example for enhanced creep properties due to tensile pre-rafting can be found in [25].…”
Section: Introductionsupporting
confidence: 91%
“…At intermediate and high temperature the deformation is controlled by dislocation activity and by the rafting phenomenon. At 1223 K (950 ℃) microstructure S is stronger because the longer ageing time gives it a more ordered structure [9]. The F material despite having a smaller precipitate size, which should imply a smaller γ channel width, is much more irregular so that regions of thick γ are more common.…”
Section: Discussionmentioning
confidence: 99%
“…The primary slip plane was identified using Laue X-ray imaging and the test-piece sectioned vertically, parallel to the tensile axis. For high resolution imaging the primary slip plane (-111) was perpendicular to the foil normal [110] and the Burgers vector of the highest Schmid Factor [1][2][3][4][5][6][7][8][9][10][11][12](-111) slip system lies in the plane of the foil. Hence an edge dislocation in this system a/3 [1][2][3][4][5][6][7][8][9][10][11][12] has its line vector parallel to the foil normal and would be in the ideal configuration to image the atom alignment at high resolution.…”
Section: Methodsmentioning
confidence: 99%
“…For high resolution imaging the primary slip plane (-111) was perpendicular to the foil normal [110] and the Burgers vector of the highest Schmid Factor [1][2][3][4][5][6][7][8][9][10][11][12](-111) slip system lies in the plane of the foil. Hence an edge dislocation in this system a/3 [1][2][3][4][5][6][7][8][9][10][11][12] has its line vector parallel to the foil normal and would be in the ideal configuration to image the atom alignment at high resolution. The sample was also cut on the other vertical section normal to [1][2][3][4][5][6][7][8][9][10] and horizontally normal to [001] for imaging the dislocations and stacking faults at lower magnification.…”
Section: Methodsmentioning
confidence: 99%
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