To Study the Effect of Stress Concentration Factor on Mild Steel Due to Heat Treatment

5
@ IJTSRD | Available Online @ www ISSN No: 245 Inte R To Study the Effe Mild St Aman Roy Department of Mechanical Engin NetajiSubhash Engineering College, K Pratick Chand Samanta Department of Mechanical Engin NetajiSubhash Engineering College, K ABSTRACT The present work is to study the effe types of heat treatment processe concentration factor (Kt) of a plate w hole subjected to a uniform loading. F Analysis using ABAQUS 6.13-1 has order to calculate, Ktfor rectangular pla of different diameters. Stress-Strain generated from standard tensile speci E8) with Universal Testing machine (H and after various types of heat treat Young’s Modulus, Poisson’s Ratio an strain verses Stress are calculated fro strain diagram and feed as an Input par FEA analysis. The results shows that th for quenching has a higher value in c room temperature mild steel specimen of Kt for normalizing and annealing value in comparison to room temperat specimen. Keywords: Stress Concentration facto treatment, Tensile Test, Finite Element A w.ijtsrd.com | Volume – 1 | Issue – 6 | Sep-Oct 56 - 6470 | www.ijtsrd.com | Volum ernational Journal of Trend in Sc Research and Development (IJT International Open Access Journ ect of Stress Concentration Fa teel due to Heat Treatment neering, Kolkata, India a neering, Kolkata, India Ranik D Department of Mechan NetajiSubhash Engineering C K. Bhattach Department of Mechan NetajiSubhash Engineering C ect of various es on stress with a circular Finite Element been done in ates with holes diagrams are imens (ASTM HEICO), before tment process. nd the Plastic om the Stress- rameter for the he value of Kt comparison to and the value show a lower ture mild steel or (Kt), Heat Analysis NOMENCLATURE 1. INTRODUCTION The application of mathema methods of stress analysis information on values of stre for widely different designs. then obtained by multiplying stress. This knowledge of m related to the mechanical pro and so an estimate of stren general, this estimate is not a r ideal homogeneous and elast arriving at the theoretical stre does not accurately represent D Width of spe d F T t Diameter of c Force (N) Thickness of Theoretical Greek Symbols σ Stress (N m -1 ) Subscripts max Maximum nom Nominal 2017 Page: 257 me - 1 | Issue 6 cientific TSRD) nal actor on Das nical Engineering, College, Kolkata, India haryya nical Engineering, College, Kolkata, India atical and experimental has produced reliable ess concentration factors The maximum stress is a factor by the nominal maximum stress can be operties of the material, ngth can be made. In reliable one, because the tic material assumed i n ess concentration factor t the structural material ecimen (m) circular hole (m) specimen (m) )

description

The present work is to study the effect of various types of heat treatment processes on stress concentration factor Kt of a plate with a circular hole subjected to a uniform loading. Finite Element Analysis using ABAQUS 6.13 1 has been done in order to calculate, Kt for rectangular plates with holes of different diameters. Stress Strain diagrams are generated from standard tensile specimens ASTM E8 with Universal Testing machine HEICO , before and after various types of heat treatment process. Youngs Modulus, Poissons Ratio and the Plastic strain verses Stress are calculated from the Stress strain diagram and feed as an Input parameter for the FEA analysis. The results shows that the value of Kt for quenching has a higher value in comparison to room temperature mild steel specimen and the value of Kt for normalizing and annealing show a lower value in comparison to room temperature mild steel specimen. Aman Roy | Ranik Das | Pratick Chand Samanta | K. Bhattacharyya "To Study the Effect of Stress Concentration Factor on Mild Steel Due to Heat Treatment" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456-6470, Volume-1 | Issue-6 , October 2017, URL: https://www.ijtsrd.com/papers/ijtsrd2506.pdf Paper URL: http://www.ijtsrd.com/engineering/mechanical-engineering/2506/to-study-the-effect-of-stress-concentration-factor-on-mild-steel-due-to-heat-treatment/aman-roy

Transcript of To Study the Effect of Stress Concentration Factor on Mild Steel Due to Heat Treatment

Page 1: To Study the Effect of Stress Concentration Factor on Mild Steel Due to Heat Treatment

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ISSN No: 2456

InternationalResearch

To Study the Effect of Stress Concentration Factor on Mild Steel due t

Aman Roy Department of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

Pratick Chand SamantaDepartment of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

ABSTRACT The present work is to study the effect of various types of heat treatment processes on stress concentration factor (Kt) of a plate with a circular hole subjected to a uniform loading. Finite Element Analysis using ABAQUS 6.13-1 has been done in order to calculate, Ktfor rectangular plates with holes of different diameters. Stress-Strain diagrams are generated from standard tensile specimens (ASTM E8) with Universal Testing machine (HEICO), before and after various types of heat treatment process. Young’s Modulus, Poisson’s Ratio and the Plastic strain verses Stress are calculated from the Stressstrain diagram and feed as an Input parameter for the FEA analysis. The results shows that the value of Kt for quenching has a higher value in comparison to room temperature mild steel specimen and the value of Kt for normalizing and annealing show a lower value in comparison to room temperature mild steel specimen.

Keywords: Stress Concentration factor (Kt), Heat treatment, Tensile Test, Finite Element Analysis

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 1 | Issue – 6 | Sep-Oct 2017

ISSN No: 2456 - 6470 | www.ijtsrd.com | Volume

International Journal of Trend in Scientific Research and Development (IJTSRD)

International Open Access Journal

To Study the Effect of Stress Concentration Factor on Mild Steel due to Heat Treatment

Department of Mechanical Engineering, College, Kolkata, India

Pratick Chand Samanta Department of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

Ranik DasDepartment of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

K. BhattacharyyaDepartment of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

The present work is to study the effect of various treatment processes on stress

concentration factor (Kt) of a plate with a circular hole subjected to a uniform loading. Finite Element

1 has been done in order to calculate, Ktfor rectangular plates with holes

Strain diagrams are generated from standard tensile specimens (ASTM E8) with Universal Testing machine (HEICO), before and after various types of heat treatment process. Young’s Modulus, Poisson’s Ratio and the Plastic

calculated from the Stress- strain diagram and feed as an Input parameter for the FEA analysis. The results shows that the value of Kt for quenching has a higher value in comparison to room temperature mild steel specimen and the value

ng and annealing show a lower value in comparison to room temperature mild steel

: Stress Concentration factor (Kt), Heat treatment, Tensile Test, Finite Element Analysis

NOMENCLATURE

1. INTRODUCTION The application of mathematical and experimental methods of stress analysis has produced reliable information on values of stress concentration factors for widely different designs. The maximum stress is then obtained by multiplying a factor by the nominalstress. This knowledge of maximum stress can be related to the mechanical properties of the material, and so an estimate of strength can be made. In general, this estimate is not a reliable one, because the ideal homogeneous and elastic material assumed iarriving at the theoretical stress concentration factor does not accurately represent the structural material

D Width of specimen (m)d F T t

Diameter of circular Force (N) Thickness of specimen (m)Theoretical

Greek Symbols σ Stress (N m-1)Subscripts max Maximum nom Nominal

Oct 2017 Page: 257

6470 | www.ijtsrd.com | Volume - 1 | Issue – 6

Scientific (IJTSRD)

International Open Access Journal

To Study the Effect of Stress Concentration Factor on

Das Department of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

K. Bhattacharyya Department of Mechanical Engineering,

NetajiSubhash Engineering College, Kolkata, India

The application of mathematical and experimental methods of stress analysis has produced reliable information on values of stress concentration factors for widely different designs. The maximum stress is then obtained by multiplying a factor by the nominal stress. This knowledge of maximum stress can be related to the mechanical properties of the material, and so an estimate of strength can be made. In general, this estimate is not a reliable one, because the ideal homogeneous and elastic material assumed in arriving at the theoretical stress concentration factor does not accurately represent the structural material

Width of specimen (m) Diameter of circular hole (m)

Thickness of specimen (m)

)

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actually used in practice. This causes observed strength values of notched parts to be equal to or greater than, that which is indicated by the application of theoretical stress concentration factors. Stress concentration is defined as the localization of high stresses due to the irregularities present in the component and abrupt changes of the cross section.To determine the stress concentration the specimen is subjected to a uniform load for different diameters of hole present in it. Since the area around the hole is less there is a sudden rise in the magnitude of stresses in the vicinity of the hole.

The localized stresses in the neighbourhood of the hole are far greater than the stresses obtained by elementary equations as mentioned in Mechanical Engineering Design [1]. But due to heat treatment the mechanical properties get altered thus the stresses get changed.

Localised stress is being calculated as

𝜎 =F

(D d)T

In order to consider the effect of stress concentration and find out localised stresses, a factor called stress concentration factor is used

The stress concentration factor (Kt) is calculated from the nominal stress 𝜎nomobtained from Eq. (1) and maximum stress 𝜎max from FEA. The stress concentration factor is calculated as

K = max

nom

As, Kt is a very important factor in machine design various works have been done on stress concentration by various researchers like Shaik and Mirzana [2] with composite material; sun et al. [3] on upper yield point of mild steel but this work is mainly focused the change in the nature of Kt on mild steel before and after heat treatment.

2. SPECIMEN The specimen is made up of mild steel

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actually used in practice. This causes observed strength values of notched parts to be equal to or greater than, that which is indicated by the direct application of theoretical stress concentration factors.

Stress concentration is defined as the localization of high stresses due to the irregularities present in the component and abrupt changes of the cross section.

tration the specimen is subjected to a uniform load for different diameters of hole present in it. Since the area around the hole is less there is a sudden rise in the magnitude of stresses

neighbourhood of the hole are far greater than the stresses obtained by elementary equations as mentioned in Mechanical Engineering Design [1]. But due to heat treatment the mechanical properties get altered thus the stresses get

(1)

In order to consider the effect of stress concentration and find out localised stresses, a factor called stress

) is calculated from obtained from Eq. (1) and

from FEA. The stress

(2)

is a very important factor in machine design various works have been done on stress concentration by various researchers like Shaik and Mirzana [2] with composite material; sun et al. [3] on upper yield point of mild steel but this work is mainly focused on

on mild steel before and

Fig. 1: Tensile test specimen. The percentage of carbon in mild steel is less which makes it strong and tough but not When the mild steel is heated above its recrystallization temperature, where deformed grains are replaced by a new set of defectsnucleate and grow until the original grains are entirely consumed due to which the mechanichanged. 3. EXPERIMENTAL PROCEDURE 3.1 Heat treatments The heat treatments that have been performed in this study are Annealing, Normalising and Quenching[4].

Fig. 2: Heating the tensile test specimens above its transformation temperature.

The tensile test specimens were kept in the furnace 30 degrees above the recrystallization temperature of mild steel which was found to be 880 degree Celsius for 20 minutes shown in fig. 2. For Annealing the tensile test specimen was cooleby keeping it for 24 hours, for Quenching the specimen was bathed in water pool and for Normalizing it was kept in steady air at room temperature for 4-5 hours.

3.2 Tensile test

The tensile test is performed on the specimen before and after heat treatment in Universal Testing Machine (HEICO) shown in Fig 3.

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Fig. 1: Tensile test specimen.

The percentage of carbon in mild steel is less which makes it strong and tough but not radially tempered. When the mild steel is heated above its recrystallization temperature, where deformed grains are replaced by a new set of defects-free grains that nucleate and grow until the original grains are entirely consumed due to which the mechanical properties get

EXPERIMENTAL PROCEDURE

The heat treatments that have been performed in this study are Annealing, Normalising and Quenching[4].

Fig. 2: Heating the tensile test specimens above its mperature.

The tensile test specimens were kept in the furnace 30 degrees above the recrystallization temperature of mild steel which was found to be 880 degree Celsius for 20 minutes shown in fig. 2. For Annealing the tensile test specimen was cooled in the furnace itself by keeping it for 24 hours, for Quenching the specimen was bathed in water pool and for Normalizing it was kept in steady air at room

The tensile test is performed on the specimen before nd after heat treatment in Universal Testing Machine

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Fig. 3: Universal Testing Machine (HEICO)

Due to the dual phase strengthening mechanics; the mild steel has a good balance of strength and ductility.The yield stress value for the quenched specimen was observed to be greater than that of normalized and annealed specimens, while the normalized specimen also has a greater value than that of annealed specimen, which has the least value.

Engineering stress/strain was obtained from ttensile test. These values were converted to true stress/strain values by the following Eq. (3) and Eq. (4) [5, 6]

𝜀 = ln(1 + 𝜀 )

𝜎 = 𝜎 (1 + 𝜀 )

The value of ultimate tensile stress were observed to be in the order Quenched> before heat treated>Annealed>Normalized, possibly due to the refinement of the grains at primary phase after the subsequent cooling processes. The ultimate stress and the yield stressof the material after and before heat treatments are enlisted in the Table 1.

Table 1: Yield stress and ultimate stress for different tensile test specimen.

Tensile test specimen

Yield stress (MPa)

Ultimate stress (MPa)

Without heat treatment

307.701 615.403

Quenching 733.805 1386.742

Normalizing 250.457 406.992

Annealing 198.858 423.495

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Fig. 3: Universal Testing Machine (HEICO)

Due to the dual phase strengthening mechanics; the mild steel has a good balance of strength and ductility.

the quenched specimen was observed to be greater than that of normalized and annealed specimens, while the normalized specimen also has a greater value than that of annealed

Engineering stress/strain was obtained from the tensile test. These values were converted to true stress/strain values by the following Eq. (3) and Eq.

(3)

(4)

The value of ultimate tensile stress were observed to be in the order Quenched> before heat treated>Annealed>Normalized, possibly due to the refinement of the grains at primary phase after the subsequent cooling processes. The ultimate stress and he yield stressof the material after and before heat

able 1: Yield stress and ultimate stress for different tensile test specimen.

Ultimate stress (MPa) 615.403

1386.742

406.992

423.495

4. FINITE ELEMENT ANALYSIS

Elasto-plastic analysis for different diameter of hole in the specimen is performed using ABAQUS 6.13The material consecutive properties are defined by the Young’s modulus and Poisson’s ratio, and yield stress verses plastic strain obtained from tensile test data performed at room temperature before and after heat treatment in Universal Testing Machine (HEICO) in Fig. 3. The data obtained from the tensile test are being plotted in the fig. 8, after subtracting the elastic strain from the total strain we get the plastic strain and corresponding plastic stress are obtained.

Three dimensional final modelling of the mild splate has been done for a constant thickness of 5mm. The FE model was meshed with 8 node isoperimetric hexahedral elements with 8 Gauss points taken for all calculations. Reduced integration with full Newtonian non-linear analysis computation is carrithe specimens. The mesh size is kept 0.9mm throughout the specimen. Since large strain is expected near the circumference of hole, perpendicular to the direction of applied load. Material non linearity is being introduced in the specimen; large strain analysis in the FE model is incorporated. The stress distribution pattern on the plate without heat treatment, Annealing, Normalizing, and Quenching is shown in Fig.4, Fig.5, Fig.6 and Fig.7 respectively.

Fig. 4: FEA of the plate with a cirdia.0.015mm without heat treatment.

Fig. 5: FEA of the plate with a circular hole of dia.0.015mmafter annealing.

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FINITE ELEMENT ANALYSIS

plastic analysis for different diameter of hole in the specimen is performed using ABAQUS 6.13-1.

consecutive properties are defined by the Young’s modulus and Poisson’s ratio, and yield stress verses plastic strain obtained from tensile test data performed at room temperature before and after heat treatment in Universal Testing Machine (HEICO) in

3. The data obtained from the tensile test are being plotted in the fig. 8, after subtracting the elastic strain from the total strain we get the plastic strain and corresponding plastic stress are obtained.

Three dimensional final modelling of the mild steel plate has been done for a constant thickness of 5mm. The FE model was meshed with 8 node isoperimetric hexahedral elements with 8 Gauss points taken for all calculations. Reduced integration with full Newtonian

linear analysis computation is carried out for all the specimens. The mesh size is kept 0.9mm throughout the specimen. Since large strain is expected near the circumference of hole, perpendicular to the direction of applied load. Material non linearity is being introduced in the

rge strain analysis in the FE model is incorporated. The stress distribution pattern on the plate without heat treatment, Annealing, Normalizing, and Quenching is shown in Fig.4, Fig.5, Fig.6 and

Fig. 4: FEA of the plate with a circular hole of dia.0.015mm without heat treatment.

Fig. 5: FEA of the plate with a circular hole of dia.0.015mmafter annealing.

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Fig. 6: FEA of the plate with a circular hole of dia.0.015mmafter normalizing.

Fig. 7: FEA of the plate with a circular dia.0.015mmafter quenching

Since, after heat treatment the steel changes its properties

5. RESULTS & DISCUSSIONS 5.1 Stress Strain nature of Mild steel Stress strain curve is the behaviour of material when it is subjected to uniform load. Annealing refined microstructure and normalizing provide uniformity in grain size, for which the specimen’s hardness gets decreased. Quenching reduce grain size of the specimen, hence making the specimen harder. As stress is a factor of hardness, the stress changed.

The input parameters, Young’s modulus are calculated from the slope of the stress strain graph before yield stress and Poisson’s ratio is calculated by dividing transverse strain by lateral strain.

This change of stress due to different heat treatments is shown in the fig.8.

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Fig. 6: FEA of the plate with a circular hole of

Fig. 7: FEA of the plate with a circular hole of

Since, after heat treatment the steel changes its

Stress strain curve is the behaviour of material when it is subjected to uniform load. Annealing produce refined microstructure and normalizing provide uniformity in grain size, for which the specimen’s hardness gets decreased. Quenching reduce grain size

the specimen harder. As stress is a factor of hardness, the stress also gets

The input parameters, Young’s modulus are calculated from the slope of the stress strain graph before yield stress and Poisson’s ratio is calculated by

strain by lateral strain.

heat treatments

Fig. 8: Stress strain curve before and after different heat treatments.

5.2 Effect of heat treatment on stress concentration factor

The Stress Concentration factor (Kthe experiment for different d/D after heat treatment are enlisted in Table 2.After heat treatment due to the transformation of crystals the hardness of mild steel gets changed as stated earlier. Stress concentration factor being a factor of stress, also gets changed.

Table 2: Stress concentration factor for different values of d/D

d/D Kt Without heat treatment

Annealing

5/30 1.82 1.659 10/30 1.96 1.331

15/30 1.554 1.046

20/30 1.096 1.112

25/30 1.026 0.676

Due to heat treatment there is a change in stress of the material as observed in fig.8, thus the stress concentration factor also gets altered. For annealing and normalizing due to uniformity of crystal structure stress generated in the specimen is less thgenerated in normal specimen. In quenching due to the formation of finer grains, stress generated in the specimen is comparatively less than normal specimen.

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Fig. 8: Stress strain curve before and after different heat treatments.

Effect of heat treatment on stress concentration

The Stress Concentration factor (Kt) obtained from the experiment for different d/D values before and

enlisted in Table 2.After heat treatment due to the transformation of crystals the hardness of mild steel gets changed as stated earlier. Stress concentration factor being a factor of stress,

ble 2: Stress concentration factor for different values of d/D

Normalizing

Quenching

1.79 1.79 1.67 1.96

1.26 1.931

0.96 1.817

0.677 1.238

Due to heat treatment there is a change in stress of the material as observed in fig.8, thus the stress concentration factor also gets altered. For annealing and normalizing due to uniformity of crystal structure stress generated in the specimen is less than stress generated in normal specimen. In quenching due to the formation of finer grains, stress generated in the specimen is comparatively less than normal specimen.

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Hence, stress concentration factor varies. This change of the nature of Kt with d/D are being plotted in the Fig. 9 before and the heat treatment processes.

Fig. 9: Stress concentration factor of mild steel

before and after heat treatment.

CONCLUSION

From the results obtained from the experiment, it can be concluded that mechanical properties depends mainly on the various heat treatment and cooling rate. Thus, depending upon the application proper heat treatment should be adopted. Since, for annealed metal Kt is low hence it should be used for high ductility and minimum toughness. maximum hardness normalizing the carbon steel will give the satisfactory result, as Kt is maximum.

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Hence, stress concentration factor varies. This change being plotted in the

Fig. 9 before and the heat treatment processes.

Fig. 9: Stress concentration factor of mild steel before and after heat treatment.

From the results obtained from the experiment, it can properties depends

mainly on the various heat treatment and cooling rate. Thus, depending upon the application proper heat treatment should be adopted. Since, for annealed

is low hence it should be used for high uctility and minimum toughness. Whereas for

maximum hardness normalizing the carbon steel will is maximum.

REFERENCES

1) Budynas, R.G. and Nisbett, J.K, 2011, Shigley’s Mechanical Engineering Design. Ninth Edition, McGraw-Hill Education.

2) Shaik, A.S. and Mirzana, I.M., 2016, IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-ISSN: 2278334X, Volume 13, Issue 4 Ver. VII (Jul. 2016), PP 01-05.

3) Sun, H-B., Kaneda, Y., Ohmori, M. and Yoshida, F, 2006, Materials Transactions,(2006) pp. 96 to 100 #2006 The Japan Society for Technology of Plasticity

4) Totten (ed). Steel Heat Treatment Handbook. vol.1. Metallurgy and Technologies, vol. 2, Equipment and Process Design, 2nd edition. CRC Press, Boca Raton, 2007.

5) Daris and Oelmann, The structures, propertiesheat treatment of metals. The Pitman Press Great Britain, 1983.

6) Vijaty Sharan Sony Ericsson, StressModification-An Experimental and Analytical Investigation of the Large Strain Tensile Response of Glassy Polymers, Polymer Eng. And Science, vol. 30(20),pp. 1288

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Oct 2017 Page: 261

Budynas, R.G. and Nisbett, J.K, 2011, Shigley’s Mechanical Engineering Design. Ninth Edition,

Mirzana, I.M., 2016, IOSR Journal of Mechanical and Civil Engineering

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#2006 The Japan Society for

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and Oelmann, The structures, properties and

heat treatment of metals. The Pitman Press

Vijaty Sharan Sony Ericsson, Stress-strain An Experimental and Analytical

Investigation of the Large Strain Compressive and Response of Glassy Polymers, Polymer

Eng. And Science, vol. 30(20),pp. 1288-98,1990.