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|  Engineering, 2010, 2, 502-506  doi:10.4236/eng.2010.27066 Published Online July 2010 (http://www.SciRP.org/journal/eng)  Copyright © 2010 SciRes.                                                                                 ENG  Effect of Welding on Microstructure and Mechanical  Properties of an Industrial Low Carbon Steel  Zakaria Boumerzoug1, Chemseddine Derfouf1, Thierry Baudin2  1Department of Mechanical Engineering, Biskra University, Biskra, Algeria  2Université Paris-Sud 11, ICMMO, Laboratoire de Physico-Chimie de l’Etat Solide, Orsay, France  E-mail: zboumerzoug@yahoo.fr, derf_dany@yahoo.fr, Thierry.Baudi n@u-psud.fr  Received February 5, 2010; revised April 12, 2010; accepted April 18, 2010  Abstract  In this work, the effect of arc welding on microstructures and mechanical properties of industrial low carbon  steel (0.19 wt. % C) was studied. This steel is used for making gas storage cylinders. In order to realize the  objective, optical microscopy, EBSD, X-ray diffraction, and hardness tests were used. Different zones and  some phases are identified. New microstructural phenomenons are observed by using EBSD technique.  Keywords: Steel, Welding, HAZ, Ferrite  1. Introduction  Welding is a process of joining materials into one piece.  Generally, welding is the preferred joining method and  most common steels are weldable. The phase transfor- mation and mechanical behavior after the welding of  many steels have been investigated. For example, Bay- raktar et al. [1] have studied the grain growth mechanism  during the welding of interstitial free steels. Observations  in the welded joints indicate the presence of very large  grains near the fusion line and these are oriented along  the directions of the heat flow. Concerning the welding  of low carbon steels, it has been shown that the grain-  coarsened zone (GCZ) and heat affected zone (HAZ) are  very critical since embitterment is concentrated in these  areas [2].  It is also known that the final microstructures and me- chanical properties of welded steel depend on some pa- rameters like percentage of carbon and presence of oth- ers elements such as sulfur or phosphorus. Low carbon  steels that have less than 0.25% carbon, display good  welding ability, because they can be generally welded  without special precautions using most of the available  processes. Concerning the previous studies related to the  welding of low carbon steel, there are limited publica- tions [2-8]. For example, Gural et al. [2] have studied the  heat treatment in two phase regions and its effects on  microstructure and mechanical strength after welding of  the low carbon steel. On the other hand, Eroglu and Ak- soy [3] investigated the effect of initial grain size on mi- crostructure and toughness of intercritical heat-affected  zone of low carbon steel.  Concerning the present study, it has been chosen to  investigate the effect of welding on industrial low carbon  steel used for making of gas storage cylinders. Optical  microscopy, EBSD, X-ray diffraction, and hardness tests  have been used as characterization tools.  2. Experimental Procedure  The chemical composition of the base metal is given in  Table 1.  Steel electrodes were used to deposit the welds using  the shielded metal arc welding process. The chemical  composition of the weld metal is presented in Table 2.  Figure 1 illustrates a part of welded sheets of a gas  cylinder and the sample size used in this study. The sur- face studied S is indicated in this figure.  For metallographic observation, the specimens were  etched with 2% nital for 20 s and consequently the mi- crostructures of the base, weld and the heat affected zone  were defined. Specimens were prepared for Electron  Back Scattered Diffraction (EBSD) analysis using stan- dard sample preparation method. A Zeiss 940SEM with a  tungsten filament was used. The SEM device is coupled  with automatic OIMTM (Orientation Imaging Microscopy)  software from the TSL Company. The hardness across  the weld was measured by microhardness tester using a 2  kg load. In addition, X-Ray Diffraction (XRD) was used  to determine the main phases in welded steel by using  Cu α radiation. K  Z. BOUMERZOUG   ET  AL.503 Table 1. Chemical composition of the base metal (0.19 wt. % C).  C% Si% Mn% P% S% Al% Mn% Nb% Ti%  0.19 0.25 0.4 0.025 0.015 0.09 0.009 0.05 0.03  Table 2. Chemical composition of electrode, wt %.  C% Si% Mn% P% S% Al% Nn% Nb% Ti%  0.06-0.12 0.01 0.40-0.6 0.025 0.025 - - - -  Sample  Welded  zone  S  Weld metal  Base metal  Figure 1. Part of welded sheets and sample used in the study. (S: Surface studied).  3. Results and Discussion  In the first part of this paper, the microstructure of base  metal of industrial low carbon steel (0.19 wt. % C) is  presented. In the second part, the effect of welding on the  microstructure evolution is illustrated.  3.1. Base Metal  Typical microstructure of sheet (base metal) is composed  of ferrite and small regions of pearlite (α-Fe + Fe3C) at  grain boundaries edges and corners (Figure 2(a)). Fig- ure 2(b) shows an EBSD image of the base metal, which  is largely composed of equiaxed ferrite grains.    Figure 2(c) illustrates a histogram of grain size which  indicates that average grain size is 10 µm. On the other  hand, Figure 2(d) shows curve of misorientation distri- bution (blue) which is near the istropic materials (red).  For low magnification (Figure 3), the bands of per- lite-rich area (banding) were observed. This macroseg- regation phenomenon, which is called banding, is due to  the presence of high percentage of Mn (0.4-0.5%) in  these zones. In more alloyed weld metals, elements such  as chromuim and molybdenum can be found to be seg- regated in these areas [9].  3.2. After Welding  In order to clarify the effect of welding on sheets, the  microstructures of welded joints were analyzed using  optical microscopy and EBSD. The EBSD map of near- est region to HAZ (Figure 4) shows the effect of direc- tion heat flow on elongation of ferrite grains. Bayraktar  et al. [1], have observed in interstitial free steels that the  welded joints are characterized by the presence of very  large grains near the fusion line and these grains are ori- ented along the directions of the large heat flow.  This strongly “oriented” structure is in some aspects  very similar to certain solidification microstructure, whose  morphology depends also on heat flow. On the other  hand, it has been found that solidification theory can be  applied to welding [10,11].  Concerning the heat-affected zone (HAZ), Figure 5 ill-  ustrates clearly the microstructures of this zone. It contains    Copyright © 2010 SciRes.                                                                                 ENG   Z. BOUMERZOUG   ET  AL.  504  50 μm  111  001 101  70 μm  {hkl}  (a)                                               (b)  (c)                                                          (d)  Figure 2. Microstructures of industrial low carbon steel (0.19 wt. % C) in base metal by (a) optical and (b) EBSD  map–distribution of directions <hkl>//z superimposed to the Kikuchi pattern quality factor (c) Histogram of grain size and (d)    curves of misorientation distribution (blue: experimental results and red: isotropic distribution).  Widmanstatten ferrite, and some colonies of pearlite. It is  known that solid-state phase transformations, such as  grain growth, recrystallization, phase transitions, anneal- ing, and tempering, all occur in the HAZ of steel welds.  The coarse grained region of the HAZ is adjacent to the  weld fusion zone and contains grains larger than those in  the base metal. It has been found that there are two phase  transformations that occur in the HAZ during cooling.  The first is the high temperature transformation of δ-Fe  to γ-Fe. The second transformation is the γ-Fe to α-Fe  transformation [12].  However, Figure 6 shows that the center of weld metal  is totally different from the other zones, because it is  characterized by pseudo-grains and a microstructural in-  homogenity which is a result of the fastest cooling rates.  It appears that this zone contains mainly ferrite and some  colonies of pearlite. The microstructure that evolved in  the weld is heterogeneous due to the temperature gradi- ents and the chemical gradients that evolve during the  process [11].  In order to know the main phases in the welded joints  (Weld metal + HAZ), XRD diffraction was particularly  applied in this region (Figure 7). From three ferrite  peaks observed in this spectrum: the bcc (110), bcc (200)   Bands of  pearlite Figure 3. Microstructure of industrial low carbon steel  (0.19 wt. % C) in base metal.  Copyright © 2010 SciRes.                                                                                 ENG   Z. BOUMERZOUG   ET  AL.505 70 μm  {hkl}  (<hkl>//DN) 001 101  111  Figure 4. EBSD map (distribution of directions <hkl>//z  superimposed to the Kikuchi pattern quality factor) in  nearest region to HAZ after arc welding of an industrial  low carbon steel (0.19 wt. % C) (map taken in the base  metal but just near the welded metal “near the weld fusion  zone”).  Coarse grained α ferrite  Widmanstatten  ferrite  Pearlite  Figure 5. Microstructure of HAZ after welding of an in- dustrial low carbon steel (0.19 wt. % C).  50 μm  Figure 6. Center of weld metal “in the weld fusion zone”.  Figure 7. XRD spectrum of welded low carbon steel in all  the welded zone (Weld metal + HAZ).  and bcc (111), we conclude a presence only of ferrite  phase observed by optical microscopy.  On the other hand, by using EBSD observation (Fig- ure 8) a fusion line is determined. We can observe clearly  the microstructural difference between weld metal zone  and HAZ. This transition zone is characterized by bands  of coarse grains, where each band of grain has quite the  same orientation (Figure 9). In this coarse-grained zone,  it seems that the grains tend to grow along a certain pre- ferred crystallographic directions.  {hkl} large grains  HAZ  70 μm Figure 8. EBSD map (distribution of directions <hkl>//z  superimposed to the Kikuchi pattern quality factor) in  transition zone (4mm from the core of weld metal) after arc  welding of an industrial low carbon steel (0.19 wt. % C).  100 μm Figure 9. Map of the same EBSD analysis of Figure 8 and  corresponding pole figure of the colored grains.  Copyright © 2010 SciRes.                                                                                 ENG   Z. BOUMERZOUG   ET  AL.  Copyright © 2010 SciRes.                                                                                 ENG  506  0 50 100 150 200 250 300 12345678910 1112 13 14 1516 17 18 19 2021 22 distance ( mm ) Hv W.M. HAZ HAZ B.M. B.M 25 mm  Figure 10. Microhardness measurments on surface S (indi- cated in Figure 1) from the base metal across the weld  metal after welding of an industrial low carbon steel (0.19  wt. % C).  Concerning the effect of welding on different regions  of welded steel, it was reported  that a hardness testing  is the usual approach in delineating the properties of  these various zones, but the information obtained is very  limited [13]. For other researchers, a simple rapid way to  obtain important information is by hardness testing [9].  Concerning the present material, the hardness distribu- tion in different zones is shown in Figure 10. The hard- ness values of 178-250 HV in Figure 10 are observed at  location within 1 mm from the base metal, through the  HAZ across the weld metal to the other base plate. These  hardness results are partially in good agreement with  literature. Indeed, Gul et al. [2], have found that maxi- mum hardness values are measured in the area of weld  metal (WM). But in the present study, the maximum  hardness is both in weld metal and heat-affected zones.  The variation in properties across the weld can be attrib- uted to several factors, mainly to residual stresses just  after welding. However, other factors can contribute to  this hardening like grain size, phase composition and  metallic inclusions.  4. Conclusions  This work represents a contribution to the study of the  effect of shielded metal arc welding on industrial low  carbon steel (0.19 wt. % C). The microstructures in dif- ferent zones are determined from the base metal to the  weld metal. The microstructure of the center of weld  zone is completely different from the heat-affected zone.  he HAZ contains Widmanstatten ferrite, large grains of  ferrite and colonies of pearlite. We have observed that  bands of coarse grains grow along a certain preferred  crystallographic directions. Moreover, we have found  that maximum hardness values are situated in the area of  weld metal and HAZ which indicates its specificity.  5. References  [1] E. Bayaraktar, D. Kaplan, L. Devillers and J. P. Chevalier,  “Grain Growth Mechanism during the Welding of Inter- stitial Free (IF) Steels,” Journal of Materials Processing  Technology, Vol. 189, No. 1-3, 2007, pp. 114-125.  [2] A. Güral, B. Bostan and A. T. Özdemir, “Heat Treatment  in Two Phase Region and its Effect on Welding of a Low  Carbon Steel,” Materials and Design, Vol.28, No. 3,  2007, pp. 897-903.  [3] Eroglu and M. Aksoy, “Effect of Initial Grain Size on  Microstructure and Toughness,” Materials Science and  Engineering A, Vol. 286, No. 2, 2000, pp. 289-297.  [4] O. Grong and O. M. Akselsen, “HAZ Grain Growth Me- chanism in Welding of Low Carbon Microalloyed  Steels,”  Acta Metallurgica, Vol. 34, No. 9, 1986, pp.  1807-1815.  [5] C. Thaulow, A. J. Paauw, A. Gunleiksrud and O. J. 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Bayaraktar, “IF-steels and Weldability Research Re- ports Series III,” IRSID (ARCELOR) IRSID-MPM  99/20152/1, 2002.  [11] O. Grong, “Metallurgical Modelling of Welding,” The  Institute of Materials, England, 1994.  [12] J. W. Elmer, J. Wong, T. Ressler and T. A. Palmer, 6th  International Conference on Trends in Welding Research,  Pine Mountain, 6A, April 2002, pp. 15-19.  [13] G. R. Stewart, A. M. Elwazri, R. Varano, N. Pokuty- lowicz, S. Yue and J. J. Jonas, “Shear Punch Testing of  Welded Pipeline Steel,” Materials Science and Engi- neering A, Vol. 420, No. 1-2, 2006, pp. 115-121.  T | 

