scholarly journals A Metallurgical Approach to the Cracking Resistance of Hot-Dip Galvanized Zinc Coatings

1996 ◽  
Vol 28 (1-2) ◽  
pp. 35-45 ◽  
Author(s):  
S. Lazik ◽  
C. Esling ◽  
M. J. Phillippe ◽  
J. Wegria ◽  
M. Dubois

The texture of zinc coatings influences to a large extent their formability, due to the anisotropic properties of zinc. The (0002) basal plane is the easiest slip plane in zinc crystal. Its inclination to the deformation axis and direction directly influences the deformation behaviour. This work deals with the effect of the texture and microstructure on the cracking behaviour of zinc coatings. For this purpose, twelve different commercial hot-dip zinc coatings have been studied.

2022 ◽  
Vol 210 ◽  
pp. 114453
Author(s):  
Masoud Ahmadi ◽  
Bekir Salgın ◽  
Bart J. Kooi ◽  
Yutao Pei

2012 ◽  
Vol 717-720 ◽  
pp. 327-330 ◽  
Author(s):  
Huan Huan Wang ◽  
Sha Yan Byrapa ◽  
F. Wu ◽  
Balaji Raghothamachar ◽  
Michael Dudley ◽  
...  

In this paper, we report on the synchrotron white beam topographic (SWBXT) observation of “hopping” Frank-Read sources in 4H-SiC. A detailed mechanism for this process is presented which involves threading edge dislocations experiencing a double deflection process involving overgrowth by a macrostep (MP) followed by impingement of that macrostep against a step moving in the opposite direction. These processes enable the single-ended Frank-Read sources created by the pinning of the deflected basal plane dislocation segments at the less mobile threading edge dislocation segments to “hop” from one slip plane to other parallel slip planes. We also report on the nucleation of 1/3< >{ } prismatic dislocation half-loops at the hollow cores of micropipes and their glide under thermal shear stress.


2018 ◽  
Vol 8 (12) ◽  
pp. 2380 ◽  
Author(s):  
Miaocao Wang ◽  
Fulong Zhu ◽  
Yixin Xu ◽  
Sheng Liu

Silicon carbide (SiC), especially 4H-SiC, is an ideal semiconductor in power electronics due to its outstanding electrical and thermal properties. It has high hardness and brittleness, which makes it difficult to machine. To understand the nanomachining characteristics of off-axis 4H-SiC and provide suggestions on 4H-SiC substrate thinning, the nanocutting process of 4 ∘ off-axis 4H-SiC was simulated by molecular dynamics. The results showed that the stacking fault induced by cutting propagates in the basal plane, and propagates deep into the SiC workpiece when the angle between the cutting direction and the c-axis is smaller than 90 ∘ . Bond reconstruction is found near the slip plane. The cutting depth is also a key parameter in nanocutting. With smaller cutting depth, machining is more like scratching than cutting. With larger cutting depth, more atoms are involved in the cutting, cutting force and workpiece temperature are higher, and more defects exist.


Zinc crystal wires in which the basal plane was nearly parallel to the wire axis were found to twin at abnormally high stresses. No single critical resolved shear stress exists; resolved shear stresses near 3⋅7 Kg/mm 2 were common for short crystals, while longer crystals (which often fractured at the instant of twinning) had an average critical stress of 2⋅9 Kg/mm 2 . All crystals experienced detectable plastic deformation before twinning, by slip on the plane (112¯2) in the direction [1¯1¯23], for which the critical resolved shear stress in tension was 1⋅0 to 1⋅5 Kg/mm 2 . The existence of this slip system was placed beyond doubt by observations on slip lines and lattice rotations. The twinning stress is determined by the work-hardening accompanying the slip on (112¯2), which continues until the lattice has rotated sufficiently for slip to begin on the (0001) planes, originally impeded by the specimen grips. The observations suggest that, quite generally, slip is the necessary prelude to the nucleation of a twin. A model for twin nucleation is developed in detail; it postulates the creation, by homogeneous lattice shear, of a twin nucleus about 250 Å in diameter, at a site where the applied stress is magnified by an array of dislocations. Twins are nucleated at a stress which depends on the slip characteristics of the particular specimen; hence the great spread in published twinning stresses. Crystals which were indented under stress twinned immediately if the resolved stress exceeded about 2 Kg/mm 2 , but indentations made before the test were ineffective, probably because of a strain-ageing effect. Ageing also led to a slow reduction of the high stresses needed to produce basal slip in the twinned crystals. Immediately after the twin had been created, a shear stress, resolved in the basal plane, of 550 g/mm 2 was required; this fell to 200 g/mm 2 two years later, which is still six times the normal basal slip stress. Basal slip in twinned crystals was accompanied by considerable work-softening. Stresses needed to thicken existing twins were very variable but much lower than the stresses for twin creation; thickening of twins always took place smoothly and was never accompanied by stress relaxation.


2018 ◽  
Vol 941 ◽  
pp. 1242-1247
Author(s):  
Shinji Ando ◽  
Hiroaki Rikihisa ◽  
Masayuki Tsushida ◽  
Hiromoto Kitahara

In this study, to investigate effects of yttrium and other elements for non-basal slips, magnesium alloy single crystals were stretched parallel to basal plane in various temperatures, and polycrystalline magnesium alloys were also tested to estimate contribution of non-basal slips to their tensile deformation behaviour. In pure magnesium single crystals, second order pyramidal (c+a) slip (SPCS) was observed at 298K. Above room temperature, first order pyramidal (c+a) slip (FPCS) was active. In the Mg - (0.6-0.9) Y alloy single crystals, FPCS was observed at 77K to 298K, while yield stress of the Mg-Y alloy single crystals was higher than that of pure magnesium. In tensile test of polycrystalline specimen, slips lines of non-basal slip systems such as SPCS, FPCS and prismatic slip were observed even at yielding in addition to basal slip lines. Among the non-basal slips, activities of FPCS and prismatic slips were increased with increasing strain in Mg - Y alloy polycrystals. Our study suggested that active non-basal slip system in tension parallel to basal plane is (c+a) pyramidal slip and enhanced ductility of magnesium - yttrium alloy would be caused from increased activity of FPCS by yttrium addition.


Author(s):  
M.K. Hibbs ◽  
R. Sinclair

In an effort to optimize both the hardness and toughness of carbides used in cemented cutting tools, a project has been undertaken to relate variations in these mechanical properties to the defect structure of deformed WC and (W,Ti)C. This paper describes the defects in stoichiometric WC as revealed by TEM studies. Possible relationships between them and the atomic configuration and bonding in the material will be discussed. WC has a hexagonal unit cell with W atoms at the 0,0,0 position and C atoms at the 1/3,2/3,1/2 position. The c/a ratio is approximately unity with a=2. 91Å and c=2.84Å. Although the basal plane is the close-packed plane, the slip plane has been determined by other workers and confirmed by this study to be {1010}.


Author(s):  
H. Hashimoto ◽  
Y. Sugimoto ◽  
Y. Takai ◽  
H. Endoh

As was demonstrated by the present authors that atomic structure of simple crystal can be photographed by the conventional 100 kV electron microscope adjusted at “aberration free focus (AFF)” condition. In order to operate the microscope at AFF condition effectively, highly stabilized electron beams with small energy spread and small beam divergence are necessary. In the present observation, a 120 kV electron microscope with LaB6 electron gun was used. The most of the images were taken with the direct electron optical magnification of 1.3 million times and then magnified photographically.1. Twist boundary of ZnSFig. 1 is the image of wurtzite single crystal with twist boundary grown on the surface of zinc crystal by the reaction of sulphur vapour of 1540 Torr at 500°C. Crystal surface is parallel to (00.1) plane and electron beam is incident along the axis normal to the crystal surface. In the twist boundary there is a dislocation net work between two perfect crystals with a certain rotation angle.


Author(s):  
P. L. Burnett ◽  
W. R. Mitchell ◽  
C. L. Houck

Natural Brucite (Mg(OH)2) decomposes on heating to form magnesium oxide (MgO) having its cubic ﹛110﹜ and ﹛111﹜ planes respectively parallel to the prism and basal planes of the hexagonal brucite lattice. Although the crystal-lographic relation between the parent brucite crystal and the resulting mag-nesium oxide crystallites is well known, the exact mechanism by which the reaction proceeds is still a matter of controversy. Goodman described the decomposition as an initial shrinkage in the brucite basal plane allowing magnesium ions to shift their original sites to the required magnesium oxide positions followed by a collapse of the planes along the original <0001> direction of the brucite crystal. He noted that the (110) diffraction spots of brucite immediately shifted to the positions required for the (220) reflections of magnesium oxide. Gordon observed separate diffraction spots for the (110) brucite and (220) magnesium oxide planes. The positions of the (110) and (100) brucite never changed but only diminished in intensity while the (220) planes of magnesium shifted from a value larger than the listed ASTM d spacing to the predicted value as the decomposition progressed.


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