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International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645
www.ijmer.com 1253 | Page
Aezeden Mohamed
Faculty of Engineering and Applied Science, Memorial University, St. John's, NL, Canada
Abstract: Hastelloy C22 and Inconel 600 and 601 alloys specimens were cyclically deformed. Specimens were sectioned
and investigated. Results indicated that the grain structure of Hastelloy C22 revealed planar slip bands, whereas Inconel
600 and 601 showed slip bands having triangular ribbon morphology. The triangular ribbon bands were more distinct in
Inconel 601 than in Inconel 600.
Keywords: Hastelloy, Inconel, planar bands, triangular ribbon bands, cyclic deformation.
I. INTRODUCTION
Slip bands are very common features in fatigued alloys such as aluminum alloy and nickel alloys [1,2], the
formation of which has been attributed to their low stacking-fault energy (SFE). Low SFE leads to the formation of wide and
extended dislocations, with reduced ability of screw dislocations to cross-slip onto other slip planes.
The occurrence of slip bands in materials depends on their stacking-fault energy. However, several authors [3–5]
have demonstrated that reduced stacking-fault energy may not be the reason for the manifestation of deformation as slip
banding in some solid solutions. They suggested that carbon content plays a great role in determining the nature of bands in
nickel alloys [3-5] and other precipitation hardened alloys. The precipitates within the matrix sheared due to dislocations
movement [5-8]. Normally, precipitation-hardened alloys show wavy bands in a way similar to that exhibited by single-
phase alloys with high stacking-fault energy. Clavel and Pineau suggested that that the formation of slip bands was the prime
factor for initiating nucleation which leads to fracture in nickel-based alloys. They also studied cyclic deformation of supper
alloy IN718 concluded that the precipitates were slipped during cyclic deformation. Worthem [9] also observed a set of
groups of deformation slip bands during cyclic deformation of IN718. Therefore, although slip bands have been observed
due to SFE by several investigators [6–8], there seems to be no study on the investigated the effect of carbon content on slip
bands of Hastelloy C22, Inconel 600, and Inconel 601. In the present study, scanning electron microscope (SEM) was
employed to investigate the morphology of slip bands formed in these alloys during cyclic deformation.
II. MATERIALS AND EXPERIMENTAL PROCEDURES
To investigate the morphology of slip bands in Ni-based alloys, round bars of Hastelloy C22, Inconel 600 and
Inconel 601 were machined into standard fatigue specimens. Their chemical compositions are given in Table 1. Prior to
tension-tension fatigue testing, the machined samples were subjected to heat treatment at 1000ºC for 1 hour followed by air
cooling to ensure an equiaxed microstructure and therefore reproducible mechanical properties. Fatigue testing was
conducted at room temperature under the same test parameter using INSTRON1332 testing machine which was connected to
INSTRON8500 programmable control unit with a frequency of 10 Hz. All tests were conducted at room temperature. After
fatigue failure, discs were cut from regions immediately adjacent to the fracture surface and perpendicular to the loading axis
using an electrical discharge machine (EDM). They were subsequently polished to high smoothness and etched using
modified Kalling’s II reagent.
Table 1: Chemical compositions of three Ni-based alloys (wt.%).
Alloy Ni Cr Fe Mo C
Hastelloy C22 Bal. 21.42 2.95 13.67 0.003
Inconel 600 Bal. 15.77 8.58 - 0.05
Imconel 601 Bal. 22.14 16.09 - 0.3
III. RESULTS
The morphologies of the slip bands formed in the cyclically deformed specimens of the Hastelloy C22, Inconel 600
and Inconel 601 alloys are shown in "Fig. 1", "Fig. 2", and "Fig. 3", respectively. Slip bands was observed on the surfaces of
all specimens tested, but the appearance of slip bands in the specimens of the three alloy specimens was different with
respect to slip band density. The activation of multiple planar bands in Hastelloy C22 is shown in "Fig.1", where the slip
bands formed in two directions within the grain. This suggests that cyclical deformation of Hastelloy C22 with straight grain
boundary structure exhibited slip bands similar to those found in materials with low stacking fault energy. Two groups of
parallel slip bands, with one group inclined at approximately 70◦
to the other, were found is the deformed alloy. This
suggests that Hastelloy C22 experienced higher plastic deformation and longer fatigue life as compared to Inconel 600 and
Inconel 601.
Cyclic Deformation of Hastelloy and Inconel Alloys and Slip
Bands Formation
International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645
www.ijmer.com 1254 | Page
The morphology of slip bands formed in Inconel 600 and Inconel 601, as shown in "Fig. 2" and "Fig.3", is different
from that of C22. The bands formed in these materials are in the form of triangular ribbons within the grain. The bands
morphology may therefore be dependent on their carbon contents is responsible for the type of carbides morphology as
shown on Table 1.
Although slip bands are generally straight and continuous, some interruptions, kinks and divergences in slip bands
may be readily visible at high magnifications as shown in "Fig.1".
Figure 1: Scanning electron micrograps of Hastelloy C22 specimens showing planar bands fatigued at (a) 500
MPa and 7x106
cycles, (b) 550MPa and 3x106
cycles.
Figure 2: Scanning electron micrographs of Inconel 600 specimens showing short triangular ribbon-type slip
bands fatigued at (a) 500MPa and 7x105
cycles, (b) 550MPa and 3x105
cycles.
Figure 3: Scanning electron micrographs of Inconel 601 specimens showing long triangular ribbon bands
fatigued at (a) 500MPa, and 430x103
cycles, (b) 550MPa and 3x105
cycles.
International Journal of Modern Engineering Research (IJMER)
www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645
www.ijmer.com 1255 | Page
IV. DISCUSSION
It is well accepted that slip bands produced by cyclic deformation can manifest as orientated distribution of defects
such as dislocations. These defects would affect the deformation behavior of the grain structure greatly, causing deformation
to take place readily along the slip planes. A strong evidence for the occurrence of slip nucleated in grain boundaries was
shown in copper by Vinogradov [10]. Therefore, it is reasonable to suggest that the formation of slip bands in the three Ni-
based alloys tested in the present study resulted from the grain boundary as shown in "Fig. 1", "Fig. 2", and "Fig. 3".
In the case of a complete stress-strain cycle slip bands may disappear totally leaving few slip bands in the specimen surface.
However, some micro structural changes do take place internally owing to plastic incompatibility, especially at triple
junctions and grain boundaries, resulting in the formation of void-type defects along the slip plane and grain boundary. With
further cycling, the concentration of this type of defects would increase gradually. It is also likely that coalescence of defects
and formation of voids would occur due to further plastic deformation. At the same time micro cracks would appear at the
surface because fatigue damage usually occurs more easily on surfaces. Further cycling would not only promote void
formation, but it will increase the level of plastic deformation; when the plastic deformation reaches a threshold value, the
material cracks and eventually fractures. This would result in the formation of deformation steps during cyclic deformation
resulting in a net displacement in the surface after cyclic deformation this was more pronounced in alloy C22 as shown in
"Fig.1".
Accumulation of cyclic plastic deformation would eventually bring about the formation of slip bands as shown in
"Fig.1", "Fig. 2" and "Fig. 3". It is shown clearly in the present paper that there is a direct connection between morphology
of slip bands and morphology of grain boundary, which, dependent on the amount of carbides formed on grain boundary. It
can be seen that the higher the carbon content of the alloy, the greater is the chance to nucleate triangular ribbon-type slip
bands at the grain boundary. However, the slip bands morphology factors responsible for cyclic deformation are still open
questions and need further investigations.
V. CONCLUSION
The current study briefly investigated the morphologies of slip bands in Hastelloy, and in Inconel alloys cyclically
deformed. Results, revealed that planar type slip bands in Hastelloy C22, whereas triangular ribbon type slip bands in
Inconel 600 and Inconel 601 alloys. The triangular ribbon bands were more distinct in Inconel 601 than in Inconel 600. The
formation and morphology of the two types of slip bands may be attributed to the carbon content of the alloys.
REFERENCES
[1] P. Lukas, L. Kunz, and J. Krejci, Fatigue behaviour of single crystals of a Cu22%Zn alloy, Material Science Engineering A., A 158
(2), 1992, 177–183.
[2] Y. F,Li, and C. Laird, Cyclic response and dislocation structures of AISI 316L stainless steel, Materials Science and Engineering A,
186 (1-2), 1994, 87-103.
[3] L. Xiao, and Y. Umakoshi, Cyclic deformation behaviour and dislocation structure of Ti5 at. % Al single crystals oriented for
double prism slip, Philosophical Magazine A,, 82, (12), 2002, 2379-2396.
[4] V. Gerold, H.P. Karnthaler, On the Origin of Planar Slip in FCC Alloys, Acta Metallurgica, 37 (8), 1989, 2177-2183.
[5] S. Heino, B. Karlsson, Cyclic deformation and fatigue behaviour of 7Mo–0.5N super austenitic stainless steel slip characteristics and
development of dislocation structures, Acta Materialia, 49, (2), 2001, 353-363.
[6] H. F. Merrick, Effect of heat treatment on the structure and properties of extruded P/M alloy 718, Metallurgical and Materials
Transactions A, 7, (4), 1976, 505-514.
[7] H. F. Merrick, The low cycle fatigue of three wrought nickel-base alloys, Metallurgical Transactions A, 5, (4), 1974, 891-897.
[8] M. Clavel, and A. Pineau, Frequency and wave-form effects on the fatigue crack growth behavior of alloy 718 at 298K and 823K,
Metallurgical Transactions A, 9A, (4), 1978, 471-480.
[9] D. W. Worthem, and I. M. Robertson, I.M., F. A. Leckie, D. F. Socie, and C. J. Altstetter, Inhomogeneous deformation in
INCONEL 718 during monotonic and cyclic loadings, Metallurgical transactions. A, 21 A, (12), 1990, 3215-3220.
[10] A. Vinogradov, S. Hashimoto, V. Patlan, and K. Kitagawa, Atomic force microscopic study on surface morphology of ultra-fine
grained materials after tensile testing, 12
th International Conference on the Strength of Materials ICSMA-12, Materials Science and
Engineering A, 319-321, 2001, 862-866.

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  • 1. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645 www.ijmer.com 1253 | Page Aezeden Mohamed Faculty of Engineering and Applied Science, Memorial University, St. John's, NL, Canada Abstract: Hastelloy C22 and Inconel 600 and 601 alloys specimens were cyclically deformed. Specimens were sectioned and investigated. Results indicated that the grain structure of Hastelloy C22 revealed planar slip bands, whereas Inconel 600 and 601 showed slip bands having triangular ribbon morphology. The triangular ribbon bands were more distinct in Inconel 601 than in Inconel 600. Keywords: Hastelloy, Inconel, planar bands, triangular ribbon bands, cyclic deformation. I. INTRODUCTION Slip bands are very common features in fatigued alloys such as aluminum alloy and nickel alloys [1,2], the formation of which has been attributed to their low stacking-fault energy (SFE). Low SFE leads to the formation of wide and extended dislocations, with reduced ability of screw dislocations to cross-slip onto other slip planes. The occurrence of slip bands in materials depends on their stacking-fault energy. However, several authors [3–5] have demonstrated that reduced stacking-fault energy may not be the reason for the manifestation of deformation as slip banding in some solid solutions. They suggested that carbon content plays a great role in determining the nature of bands in nickel alloys [3-5] and other precipitation hardened alloys. The precipitates within the matrix sheared due to dislocations movement [5-8]. Normally, precipitation-hardened alloys show wavy bands in a way similar to that exhibited by single- phase alloys with high stacking-fault energy. Clavel and Pineau suggested that that the formation of slip bands was the prime factor for initiating nucleation which leads to fracture in nickel-based alloys. They also studied cyclic deformation of supper alloy IN718 concluded that the precipitates were slipped during cyclic deformation. Worthem [9] also observed a set of groups of deformation slip bands during cyclic deformation of IN718. Therefore, although slip bands have been observed due to SFE by several investigators [6–8], there seems to be no study on the investigated the effect of carbon content on slip bands of Hastelloy C22, Inconel 600, and Inconel 601. In the present study, scanning electron microscope (SEM) was employed to investigate the morphology of slip bands formed in these alloys during cyclic deformation. II. MATERIALS AND EXPERIMENTAL PROCEDURES To investigate the morphology of slip bands in Ni-based alloys, round bars of Hastelloy C22, Inconel 600 and Inconel 601 were machined into standard fatigue specimens. Their chemical compositions are given in Table 1. Prior to tension-tension fatigue testing, the machined samples were subjected to heat treatment at 1000ºC for 1 hour followed by air cooling to ensure an equiaxed microstructure and therefore reproducible mechanical properties. Fatigue testing was conducted at room temperature under the same test parameter using INSTRON1332 testing machine which was connected to INSTRON8500 programmable control unit with a frequency of 10 Hz. All tests were conducted at room temperature. After fatigue failure, discs were cut from regions immediately adjacent to the fracture surface and perpendicular to the loading axis using an electrical discharge machine (EDM). They were subsequently polished to high smoothness and etched using modified Kalling’s II reagent. Table 1: Chemical compositions of three Ni-based alloys (wt.%). Alloy Ni Cr Fe Mo C Hastelloy C22 Bal. 21.42 2.95 13.67 0.003 Inconel 600 Bal. 15.77 8.58 - 0.05 Imconel 601 Bal. 22.14 16.09 - 0.3 III. RESULTS The morphologies of the slip bands formed in the cyclically deformed specimens of the Hastelloy C22, Inconel 600 and Inconel 601 alloys are shown in "Fig. 1", "Fig. 2", and "Fig. 3", respectively. Slip bands was observed on the surfaces of all specimens tested, but the appearance of slip bands in the specimens of the three alloy specimens was different with respect to slip band density. The activation of multiple planar bands in Hastelloy C22 is shown in "Fig.1", where the slip bands formed in two directions within the grain. This suggests that cyclical deformation of Hastelloy C22 with straight grain boundary structure exhibited slip bands similar to those found in materials with low stacking fault energy. Two groups of parallel slip bands, with one group inclined at approximately 70◦ to the other, were found is the deformed alloy. This suggests that Hastelloy C22 experienced higher plastic deformation and longer fatigue life as compared to Inconel 600 and Inconel 601. Cyclic Deformation of Hastelloy and Inconel Alloys and Slip Bands Formation
  • 2. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645 www.ijmer.com 1254 | Page The morphology of slip bands formed in Inconel 600 and Inconel 601, as shown in "Fig. 2" and "Fig.3", is different from that of C22. The bands formed in these materials are in the form of triangular ribbons within the grain. The bands morphology may therefore be dependent on their carbon contents is responsible for the type of carbides morphology as shown on Table 1. Although slip bands are generally straight and continuous, some interruptions, kinks and divergences in slip bands may be readily visible at high magnifications as shown in "Fig.1". Figure 1: Scanning electron micrograps of Hastelloy C22 specimens showing planar bands fatigued at (a) 500 MPa and 7x106 cycles, (b) 550MPa and 3x106 cycles. Figure 2: Scanning electron micrographs of Inconel 600 specimens showing short triangular ribbon-type slip bands fatigued at (a) 500MPa and 7x105 cycles, (b) 550MPa and 3x105 cycles. Figure 3: Scanning electron micrographs of Inconel 601 specimens showing long triangular ribbon bands fatigued at (a) 500MPa, and 430x103 cycles, (b) 550MPa and 3x105 cycles.
  • 3. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.3, Issue.2, March-April. 2013 pp-1253-1255 ISSN: 2249-6645 www.ijmer.com 1255 | Page IV. DISCUSSION It is well accepted that slip bands produced by cyclic deformation can manifest as orientated distribution of defects such as dislocations. These defects would affect the deformation behavior of the grain structure greatly, causing deformation to take place readily along the slip planes. A strong evidence for the occurrence of slip nucleated in grain boundaries was shown in copper by Vinogradov [10]. Therefore, it is reasonable to suggest that the formation of slip bands in the three Ni- based alloys tested in the present study resulted from the grain boundary as shown in "Fig. 1", "Fig. 2", and "Fig. 3". In the case of a complete stress-strain cycle slip bands may disappear totally leaving few slip bands in the specimen surface. However, some micro structural changes do take place internally owing to plastic incompatibility, especially at triple junctions and grain boundaries, resulting in the formation of void-type defects along the slip plane and grain boundary. With further cycling, the concentration of this type of defects would increase gradually. It is also likely that coalescence of defects and formation of voids would occur due to further plastic deformation. At the same time micro cracks would appear at the surface because fatigue damage usually occurs more easily on surfaces. Further cycling would not only promote void formation, but it will increase the level of plastic deformation; when the plastic deformation reaches a threshold value, the material cracks and eventually fractures. This would result in the formation of deformation steps during cyclic deformation resulting in a net displacement in the surface after cyclic deformation this was more pronounced in alloy C22 as shown in "Fig.1". Accumulation of cyclic plastic deformation would eventually bring about the formation of slip bands as shown in "Fig.1", "Fig. 2" and "Fig. 3". It is shown clearly in the present paper that there is a direct connection between morphology of slip bands and morphology of grain boundary, which, dependent on the amount of carbides formed on grain boundary. It can be seen that the higher the carbon content of the alloy, the greater is the chance to nucleate triangular ribbon-type slip bands at the grain boundary. However, the slip bands morphology factors responsible for cyclic deformation are still open questions and need further investigations. V. CONCLUSION The current study briefly investigated the morphologies of slip bands in Hastelloy, and in Inconel alloys cyclically deformed. Results, revealed that planar type slip bands in Hastelloy C22, whereas triangular ribbon type slip bands in Inconel 600 and Inconel 601 alloys. The triangular ribbon bands were more distinct in Inconel 601 than in Inconel 600. The formation and morphology of the two types of slip bands may be attributed to the carbon content of the alloys. REFERENCES [1] P. Lukas, L. Kunz, and J. Krejci, Fatigue behaviour of single crystals of a Cu22%Zn alloy, Material Science Engineering A., A 158 (2), 1992, 177–183. [2] Y. F,Li, and C. Laird, Cyclic response and dislocation structures of AISI 316L stainless steel, Materials Science and Engineering A, 186 (1-2), 1994, 87-103. [3] L. Xiao, and Y. Umakoshi, Cyclic deformation behaviour and dislocation structure of Ti5 at. % Al single crystals oriented for double prism slip, Philosophical Magazine A,, 82, (12), 2002, 2379-2396. [4] V. Gerold, H.P. Karnthaler, On the Origin of Planar Slip in FCC Alloys, Acta Metallurgica, 37 (8), 1989, 2177-2183. [5] S. Heino, B. Karlsson, Cyclic deformation and fatigue behaviour of 7Mo–0.5N super austenitic stainless steel slip characteristics and development of dislocation structures, Acta Materialia, 49, (2), 2001, 353-363. [6] H. F. Merrick, Effect of heat treatment on the structure and properties of extruded P/M alloy 718, Metallurgical and Materials Transactions A, 7, (4), 1976, 505-514. [7] H. F. Merrick, The low cycle fatigue of three wrought nickel-base alloys, Metallurgical Transactions A, 5, (4), 1974, 891-897. [8] M. Clavel, and A. Pineau, Frequency and wave-form effects on the fatigue crack growth behavior of alloy 718 at 298K and 823K, Metallurgical Transactions A, 9A, (4), 1978, 471-480. [9] D. W. Worthem, and I. M. Robertson, I.M., F. A. Leckie, D. F. Socie, and C. J. Altstetter, Inhomogeneous deformation in INCONEL 718 during monotonic and cyclic loadings, Metallurgical transactions. A, 21 A, (12), 1990, 3215-3220. [10] A. Vinogradov, S. Hashimoto, V. Patlan, and K. Kitagawa, Atomic force microscopic study on surface morphology of ultra-fine grained materials after tensile testing, 12 th International Conference on the Strength of Materials ICSMA-12, Materials Science and Engineering A, 319-321, 2001, 862-866.