Extended Dislocation Configurations in HCP Silver–Tin Alloys of Low Stacking-Fault Energy

1970 ◽  
Vol 4 (1) ◽  
pp. 201-209 ◽  
Author(s):  
L. K. Ives ◽  
A. W. Ruff
1967 ◽  
Vol 45 (2) ◽  
pp. 787-795 ◽  
Author(s):  
A. W. Ruff Jr. ◽  
L. K. Ives

Direct measurements by transmission electron microscopy on extended dislocation nodes in alloys of tin in silver have led to values for the intrinsic stacking-fault energy. The values decreased smoothly from 23 erg/cm2 for pure silver to 4.2 erg/cm2 for 7.8 at.% tin. The results are compared with previous determinations in other silver-base alloys.


Author(s):  
A. W. Ruff ◽  
L. K. Ives

Recently we have reported the stacking fault energy in a series of hcp silver-tin alloys as a function of composition. The stacking fault energy was found to increase linearly with composition from 5.5 erg/cm2 for an 11.9 at.% tin alloy to 18.9 erg/cm2 for a 17.2 at.% tin alloy. Measurements were made on extended dislocation nodes and double-ribbons observed in thin foils by means of transmission electron microscopy. During the course of this investigation a number of dislocation configurations were observed as the result of interactions between extended dislocations lying on adjacent basal planes. Many of these configurations were identical to those which have been extensively studied by Delavignette and Amelinckx in hexagonal graphite. The same basal plane faulting pattern is found there as in the hcp structure. We have observed other configurations in these alloys that could be associated with cross-slip of basal dislocations or with their interactions with non-basal dislocations. It is the purpose of this paper to discuss faulting in the hcp structure and to describe several of the dislocation configurations observed in these silver-tin alloys.


1969 ◽  
Vol 17 (8) ◽  
pp. 1045-1055 ◽  
Author(s):  
A.W Ruff ◽  
L.K Ives

Author(s):  
L. K. Ives ◽  
A. W. Ruff

A determination of the intrinsic stacking fault energy as a function of composition has been previously reported for the face-centered-cubic phase in the silver-tin alloy system. The method involved direct measurements on extended dislocation nodes observed by transmission electron microscopy in alloys containing from 0 to 7.8 at.% tin. The stacking fault energy γ was found to decrease from a value of 22.8 erg/cm3 for silver to 4.2 erg/cm2 for the 7.8 at.%. alloy. Figure 1 shows the phase diagram for this system. At room temperature, the α-phase limit occurs at about 8.5 to 9 at.%. tin. A two-phase region extends to approximately 11.5 at.% followed by the ζ- Ag Sn phase region which exists to about 17 at.% tin. A series of hexagonal ζ alloys of various compositions are presently under study to determine the variation of the stacking fault energy with composition. Preliminary results indicate that the stacking fault energy increases with increasing solute concentration in the ζ-phase region. Extended dislocation nodes have been observed in all the ζ alloys, together with extended ribbons in the dilute alloys. This paper will consider only the results obtained on the most dilute alloy (12 at.% tin) and compare them with the a-phase results.


Author(s):  
K. Z. Botros ◽  
S. S. Sheinin

The main features of weak beam images of dislocations were first described by Cockayne et al. using calculations of intensity profiles based on the kinematical and two beam dynamical theories. The feature of weak beam images which is of particular interest in this investigation is that intensity profiles exhibit a sharp peak located at a position very close to the position of the dislocation in the crystal. This property of weak beam images of dislocations has an important application in the determination of stacking fault energy of crystals. This can easily be done since the separation of the partial dislocations bounding a stacking fault ribbon can be measured with high precision, assuming of course that the weak beam relationship between the positions of the image and the dislocation is valid. In order to carry out measurements such as these in practice the specimen must be tilted to "good" weak beam diffraction conditions, which implies utilizing high values of the deviation parameter Sg.


2020 ◽  
pp. 5-18
Author(s):  
D. V. Prosvirnin ◽  
◽  
M. S. Larionov ◽  
S. V. Pivovarchik ◽  
A. G. Kolmakov ◽  
...  

A review of the literature data on the structural features of TRIP / TWIP steels, their relationship with mechanical properties and the relationship of strength parameters under static and cyclic loading was carried out. It is shown that the level of mechanical properties of such steels is determined by the chemical composition and processing technology (thermal and thermomechanical processing, hot and cold pressure treatment), aimed at achieving a favorable phase composition. At the atomic level, the most important factor is stacking fault energy, the level of which will be decisive in the formation of austenite twins and / or the formation of strain martensite. By selecting the chemical composition, it is possible to set the stacking fault energy corresponding to the necessary mechanical characteristics. In the case of cyclic loads, an important role is played by the strain rate and the maximum load during testing. So at high loading rates and a load approaching the yield strength under tension, the intensity of the twinning processes and the formation of martensite increases. It is shown that one of the relevant ways to further increase of the structural and functional properties of TRIP and TWIP steels is the creation of composite materials on their basis. At present, surface modification and coating, especially by ion-vacuum methods, can be considered the most promising direction for the creation of such composites.


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