International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 Effects of External Magnetic Field on Mechanical properties of a welded M.S metal through Metal Shield Arc Welding *Ajit Senapati¹ Siba brata Mohanty² *1.Asso.Professor, Department of Mechanical Engineering, G.I.E.T, Gunupur, Rayagada, Odisha, India 2. Research scholar, Department of Industrial Engineering, G.I.E.T, Gunupur. Rayagada, Odisha, India I. INTRODUCTION Welding is a process in which materials of the same characteristic changes obtained by the deflection of fundamental type or class are brought together and caused to welding arc in the presence of external magnetic field. The join (and become one) through the formation of primary chemical bonds under the combined action of heat and magnetic field has been applied from various orientations pressure . The definition found in IS0 standard is “Welding is upon the weld bead. The welding process which has been an operation in which continuity is obtained between parts for assembly, by various means”. Hence, the welding is the fusion considered under study is shielded metal arc welding on of two or more pieces of metal together by using the heat Mild steel plate. The objective of this paper is to study produced from an electric arc welding machine. Arc welding dates back to the late 1800’s, when a man was welding with a effect of magnetic field on the weld quality and geometry bare metal rod on iron, the sparks from the welding caught a when the field is applied longitudinal to the electrode stack of newspapers on fire near him and while welding, he noticed that his welds started looking a lot better. The reason travel i.e. the field lines are perpendicular to the electrode for this was the smoke took the oxygen out of its welding travel. However there is lack of information for optimum environment and decreased porosity. The arc is struck between the electrode and the metal. It then heats the metal to parameters, very little work has been reported in this a melting point. The electrode is then removed, breaking the direction. A magnetic field externally applied to the arc between the electrode and the metal. This allows the molten metal to “freeze” or solidify. The arc is like a flame of welding arc, deflects the arc by electromagnetic force in intense heat that is generated as the electrical current passes the plane normal to the field lines. The magnetic field through a highly resistant air gap. During welding, magnetic field is set up in the plane of the parts being joined and exerts force on the electrons and ions within the arc, which circumferentially around the electrode and the plate as shown causes the arc to be deflected away from the normal arc in Fig 1. The field, F1, is set up around the electrode; the field F2, around the plate plates being joined and the field, F3, in path. The welding arc can be deflected forward, backward, the plates adjacent to the arc and in a direction similar to that or sideways with respect to electrode and welding of field F1. Since it is not possible to remove these fields from welding operation, it is necessary to use external control as a direction depending upon the direction of an external means to overcome these magnetic effects [1]. A magnetic magnetic field. In this paper various mechanical field externally applied to the welding arc deflects the arc by electromagnetic force (Lorentz force) in the plane normal to properties tests such as tensile strength, hardness, impact the field lines. The magnetic field exerts force on the electrons test etc. are conducted to see the effect of external and ions within the arc, which causes the arc to be deflected away from the normal arc path. Deminskii, et al. [3], magnetic field on it. It is observed that weld pool conducted experiments using a GMAW process on an penetration reduces while the weld bead width increases aluminum-magnesium alloy while a longitudinal magnetic field was applied to the welding arc. The magnetic fields thereby affecting the parameters of the process. The applied were alternating and of the order of 40 gauss. results and conclusions are discussed as per the They reported the arc oscillated across the weld axis. observations while the tensile strength and hardness of Subjecting the welding arc to transverse magnetic fields has beneficial effects only when the arc is deflected forward with parent materials are observed as well. respect to the direction of electrode travel [4] [5]. Applying an optimum magnetic field to a welding arc on both nonmagnetic and magnetic materials increases welding speed Keywords— Arc Instability, Magnetic Effects, Metal several times at which undercut-free and no porosity welds shield arc Welding, Weld Beads. can be made It is known the extent of arc deflection is Abstract— The aim of this study is to show the ISSN: 2231-5381 http://www.ijettjournal.org Page 297 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 dependent upon the flux density of the applied magnetic field, the arc current, arc length, and so on [4,6 ,7]. be used as automatically regulating the depth of penetration. Hicken and Jackson found beneficial effects of constant transverse magnetic field when the arc was deflected forward with respect to the electrode travel speed. It was possible to increase the welding speed four times and steel obtains the welds free from undercuts. Weld width was found to reduce with increase in magnetic field. Sheinkin found the application of transverse magnetic field to increase the productivity of the submerged arc welding process used for making butt joints between prepared edges Fig 1.Shows Planes of Magnetic Field Set-up 2. Application of magnetic field 2.1 Longitudinal magnetic field: A magnetic force acts on the arc, in this system when the angle between the direction of the electron stream and magnetic lines of force are not zero. As the arc has a conical shape and the current carrying electrons also moves along the surface of the arc, their motions can be resolved in two components, one along the axis of the arc and other perpendicular to it. The component along the arc does not contribute to the magnetic movement. The component perpendicular to arc exerts a force on the arc causing the arc to rotate clockwise or anticlockwise depending upon the direction of the magnetic field and polarity used. Fig. 3 Image for Transverse magnetic field set-up 3. Experimental procedure 3.1 Preparation of Specimens: The mild steel pieces of the dimension 200 mm X 20 mm X 6 mm are used as a work-piece for the welding. Each metal piece first cleaned for dust and rust. Before the actual welding process the space between the specimens is fixed with a support. The space between the specimens for the butt welding is depends upon the thickness of the work-piece. For a 6 mm thickness there is no requirement of making groove, so a 3 mm gap is maintained during the whole process of welding. The quality and geometry of weld is much depends on correct and same gap throughout length of the specimen. Fig.2-Image for Longitudinal magnetic field set-up 2.2 Transverse magnetic field:According to the Flemings left hand rule the arc in the influence of transverse magnetic field will be deflected forward or backward depending upon the direction of magnetic field lines force and the polarity of welding system. Work of earlier investigation can be analyzed keeping this in mind .Kovalev showed that the transverse magnetic field can ISSN: 2231-5381 Figure:-4 Image for removing bend from M.S flat set-up http://www.ijettjournal.org Page 298 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 the magnetic field arrangement is removed. The range of current and voltage are remained similar to the magnetic field welding. The weld-pieces obtained after the process is shown in fig. different welding parameters readings associated with the process are tabulated and it is shown in the table no.2. WOR KPIEC E NO. CURREN T (A) VOLTAG E (V) M1. M2. M3. 90 90 90 25 25 25 Figure:-5 Image for cleaning of Specimen 3.2 Welding In Magnetic Field (M): The magnetic field is applied as per the set-up and then the arc welding machine and electrodes are fixed at their respective places. Multi-meter, clamp-meter and gauss-meter are placed and connected to take the readings. As per the semi-automation to the process feed rod is connected with the work-piece motion. The weld-pieces obtained after the process is shown in fig. different welding parameters readings associated with the process are tabulated and it is shown in the table no.1. MAGN ETICFIELD INTENS ITY (GAUSS ) 70 70 70 WELDIN G SPEED (mm/min ) 60 60 60 Fig:-7 Image for welding of specimen without magnetic field WORKPIECE CURRENT(A) VOLTAGE NO. WM1, WM2, WM3 (V) 90 25 Table-2 Shows operating parameters for welding (without magnetic field) Fig:-6 Image shows welding of specimen with magnetic field magnetic field Table-1 Shows operating parameters for welding (with magnetic field) WORKPIECE M1, M2, M3 CURRENT (A) 90-100 VOLTAG E (V) 27-30 3.3 Welding Without Magnetic Field (WM): The similar setting as with magnetic welding is used in without magnetic field process of welding. Only change is that 3.4 Grouping and cutting of weld-pieces: Each weld-piece (with and without magnetic field) cut into three pieces and grouped according to the range of current and voltage and provided a specific code. Now, the total no. of weld-pieces is 9 and their corresponding parametric readings are tabulated as below. Each weld specimen has a code which shows its specifications. The letter shows the weld-piece is from the category of magnetic field or without magnetic field. The letter M shows magnetic field and WM shows without magnetic field. The number provided to the code shows its range of current and voltage. The number 1, 2, 3 shows the range of current 110-120 Ampere and voltage 23-26 volts. Weld-pieces with magnetic field:Table-3 Shows experimental value for current, voltage, magnetic field intensity and welding speed at various stage of experiment. ISSN: 2231-5381 http://www.ijettjournal.org Page 299 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 3.5 Hardness test: Vickers hardness test The Vickers hardness is as an alternative to the Brinell method to measure the hardness of materials. The Vickers test is often easier to use than other hardness tests since the required calculations are independent of the size of the indenter, and the indenter can be used for all materials irrespective of hardness. It is ability to resist plastic deformation from a standard source. The unit of hardness given by the test is known as the Vickers Pyramid Number (HV) or Diamond Pyramid Hardness (DPH). The hardness number can be converted into units of pascals, but should not be confused with a pressure, which also has units of pascals. The hardness number is determined by the load over the surface area of the indentation and not the area normal to the force, and is therefore not a pressure. Fig.9-Image for Vickers Hardness Tester 3.6 Tensile strength test: This test is used to measure the tensile strength of a welded joint. The tensile strength, which is defined as stress in kgf per square meter. It is calculated by dividing the breaking load of the test piece by the original cross section area of the specimen. The test result which is conducted on universal testing machine (UTM) is given in the table. The width thickness of the test specimen are measured before testing, and the area in square inches is calculated by multiplying these before testing , and the area in square inches is calculated by multiplying these two figures. Fig-8:- Image for an indentation left in case-hardened steel after a Vickers hardness test. A diamond in the form of a square-based pyramid of ideal size of a Brinell impression was 3/8 of the ball diameter. As two tangents to the circle at the ends of a chord 3d/8 long intersect at 136°, it was decided to use this as the included angle of the indenter, giving an angle to the horizontal plane of 22° on each side. The angle was varied experimentally and it was found that the hardness value obtained on a homogeneous piece of material remained constant, irrespective of load. Accordingly, loads of various magnitudes are applied to a flat surface, depending on the hardness of the material to be measured. The HV number is then determined by the ratio F/A, where F is the force applied to the diamond in kilograms-force and A is the surface area of the resulting indentation in square millimetres ISSN: 2231-5381 Fig.10-Shows Tensile Testing Process The shearing strength of the weld in pounds per linear inch is determined by dividing the maximum load by the length of fillet weld that ruptured. The shearing strength in pounds per square inch is obtained by dividing the shearing strength in pounds per linear inch by the average throat dimension of the weld in inches. The test specimens are made wider than required and machined down to size. http://www.ijettjournal.org Page 300 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 field applied on vertical the hardness of metal is gradually increases up to 262.11 Table-5 Shows Experimental values for Hardness carried out at various conditions WORK-PIECE NO. PARENT METAL WELD (HV) METAL (HV) 154.754 194.0125 154.754 176.68 154.754 262.11 MILD STEEL(WITHOUT MAGNETIC FIELD) WITH MAGNETIC FIELD. (HORIZONTAL) Fig.11-Image for UTM Used for tensile test WITH MAGNETIC FIELD. (VERTICAL) 3.7 Impact Test: The two kinds of specimens used for impact testing are known as Charpy and Izod. Both test pieces are broken in an impact testing machine. The only difference is in the manner that they are anchored. The Charpy piece is supported horizontally between two anvils and the pendulum strikes opposite the notch. The Izod piece is supported as a vertical cantilever beam and is struck on the free end projecting over the holding vise A Charpy test measures the welds ability to withstand an Impact force 4.2 Effect of external magnetic field on tensile strength In the presence of external magnetic field welding is performed. After that tensile test is carried out by UTM. Three specimens M1, M2&M3 are taken for tensile test. It was observed that tensile strength of weld joints is much more improved. Detail observation datas are shown in the test report-1, 2&3. Fig12-Image for Weld specimen for Charpy test 4. Results and discussion 4.1 Effect of external magnetic field on Hardness The determination of the Rockwell hardness of a material involves the application of a minor load followed by a major load, and then noting the depth of penetration from a dial, on which a harder material gives a higher number. The test result of the hardness test was conducted on both type of weldpieces (with magnetic field and without magnetic field) are shown in the table-5 below. From experimental data the hardness increases within the magnetic field. When magnetic ISSN: 2231-5381 http://www.ijettjournal.org Page 301 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 4.3 Effect of external magnetic field on impact test The toughness values of the weld-pieces are tabulated below. Weld-pieces are placed at the impact testing machine as simply supported Table-6 Shows Experimental values for Toughness (J) carried out at various conditions WORK-PIECE NO. TOUGHNESS (J) WITHOUT MAGNETIC FIELD 20.5 WITH MAGNETIC FIELD (VERTICAL) 36.0 WITH MAGNETIC FIELD (HORIZONTAL) 12.5 4.4 Comparison of all the mechanical properties with and without application of external magnetic field The effect of magnetic field on the tensile strength is increased. The change in the properties is calculated in terms of percentage and there is an increase of 6.6% on an average. This shows that a magnetic field applied longitudinal to weld bead, deflected the arc such that the tensile properties of the weld-pieces increases Table-7 Shows Percentage change in value for without magnetic field and Magnetic field vertical for various mechanical properties PROPERTIES TENSILE STRENGTH HARDNESS TOUGHNESS WITHOUT MAGNETIC FIELD 399 MAGNETIC FIELD (VERTICAL) 442 CHANGE 194.012 262.11 20.5 36.0 25.98% INCREASE 43.05% INCREASE 9.72% INCREASE Table-8 Shows Percentage change in value for without magnetic field and Magnetic field Horizontal for various mechanical properties PROPERTI ES WITHOUT MAGNETI C FIELD MAGNET IC FIELD (HORIZO CHANGE NTAL) TENSILE STRENGTH ISSN: 2231-5381 http://www.ijettjournal.org 399 357 10.52% DECRESES Page 302 International Journal of Engineering Trends and Technology (IJETT) – Volume 10 Number 6 - Apr 2014 HARDNESS 194.012 176.68 8.93% DECRESES [8] M. S. U. R. Mahadi, N. A. and M. S. I. Rasel (ICME2011) 18-20 TOUGHNESS 20.5 12.5 39.02% DECRESES December 2011, Dhaka, Bangladesh. [9]Yunia Ahmad dar,charanjeet singh,Younish Farooq,Indian journal of applied ,research,vol;4,issue vol-4 April 2014,ISSN-2249-555X 5. CONCLUSIONS [10]R.P singh et al. RESEARCH INVENTY: International Journal of On the basis of different experiments welding process and effect of magnetic field in the longitudinal direction the following conclusions are derived: Effect of magnetic field applied longitudinal to welding direction affects the bead width of joint and decreases it. Undercuts, spatter etc. welding defects are reduced. The tensile strength of the weld joint is on improvement side due the refinement of grains. Hardness of the weld Increases as compared with the weld-pieces which are welded without magnetic field. Reinforcement height of weld reduces as the weld bead width is increasing. Toughness of the weld metal increases. When solenoid is introduce in the transverse direction then the mechanical properties such as Hardness, Toughness and Tensile strength are decreases. If travel speed is increased, tensile strength of weld generally increases. If magnetic field is increased, tensile strength of weld generally increases. Engineering and Science ISBN: 2319 6483, ISSN: 2278 4721, Vol. 2, Issue 1(January2013), PP 53-57 Application of Artificial Neural Network to Analyze and Predict the Tensile Strength of Shielded Metal Arc Welded Joints under the Influence of External Magnetic Field [11]Basic Manufacturing Process by P.N.Rao. [12] A Course In Workshop Technology by B.S.Raghuwanshi. [13] Engineering Principles of Welding- processes, physics, chemistry and metallurgy by Robert, Wissler 2004, and welding journal. [14] Manufacturing Technology by P.C.Sharma. [15]Principles of Magnetism and Stray Currents in Rotating Machinery By Paul I. Nippes, P.E., President of Magnetic Products and Services, Inc. Hence, we can say that the use of external magnetic field longitudinal to the welding direction is helping in improvement of weld quality and weld geometry. It can also affect the weld quality. 6. REFERENCES [1] Rossi, BE, 1954, “Welding Engineering”, McGraw-Hill Book Co. Inc., New York, USA. [2] Hughes, R. V., and Walduck, R. P. 1987. “Electromagnetic arc path control in robot plasma welding.” Robotic Welding. IFS Publication and Springer-Verlag, pp. 243–263. [3] Deminskii, Y. A., and Dyatlov, V. I. 1963. “Magnetic control during gas shielded arc welding with a consumable electrode.” Automatic Welding (4): 67–68. [4] Hicken, G. K., and Jackson, C. E. 1966. “The effect of applied magnetic fields on welding arcs.” Welding Journal 45(11): 515-s to 524-s. [5] Jayarajan, T. N., and Jackson, C. E. 1972. “Magnetic control of gas tungsten arc welding process.” Welding Journal 51(8): 377-s to 385-s. [6] 8. Ecer, G. M. 1980. “Magnetic deflection of the pulsed current welding arc.” Welding Journal 59(6): 183-s to 191-s. [7] 9. Lancaster, J. F. 1986. “The Physics of Welding”. Oxford, Pergamon. ISSN: 2231-5381 http://www.ijettjournal.org Page 303