Effect of Electrochemical Reactions on Submerged Arc Weld Metal Compositions Weld metal composition is controlled by chemical reactions in four separate areas during welding BY J. H. KIM, R. H. FROST, D. L. OLSON AND M. BLANDER ABSTRACT. The purpose of this work is to investigate the relative influence of electrochemical and thermochemical reactions on the weld metal chemistry in a direct current submerged arc welding process. Chemical analyses were carried out on the melted electrode tips, the detached droplets and the weld metal for both electrode-positive (reverse) polarity where the welding wire is anodic and electrode-negative (straight) polarity where the welding wire is cathodic. The results suggest that both thermochemical and electrochemical reactions are important in altering the composition of the weld metal. The anodic electrochemical reactions include the oxidation of iron and alloy elements, and the discharge and pickup of oxygen anions from the molten flux. Cathodic electrochemical reactions include the reduction of iron and alloy elements from the flux to the metal phase, and the refining of oxygen. Thermochemical reactions occur and move the overall composition toward the thermochemical equilibrium. Introduction The submerged arc welding process uses a protective flux cover with a consumable welding wire. The welding current is carried largely by the submerged arc and to some extent by conduction in the molten flux layer. Information on the interaction between slag and weld metal is significant for a better understanding of the arc welding process. Although slag/ metal reactions are of importance in many fusion welding processes and are often referred to in the literature, comparatively /. H. KIM, R. H FROST and D. L. OLSON are with the Center for Welding Research, Department of Metallurgical Engineering, Colorado School of Mines, Golden, Colo. M. BLANDER is with Argonne National Laboratory, Chemical Technology Division/Materials Science and Technology Program, Argonne, 111. Paper presented at the 68th Annual AWS Meeting, held March 22-27, 1987, in Chicago, III. 446-s | DECEMBER 1990 little is known about the mechanisms that control them. The chemistry in steel making tends to be dominated by thermochemical reactions because they generally involve large surface areas, low current densities and alternating current power. But a direct current submerged arc welding process involves small surface areas and high current densities. Therefore, it is expected that electrochemical reactions, as well as thermochemical reactions, will exert a significant influence over the final chemistry of the weld. The overall composition of the weld is controlled by the composition of the metal droplets that enter the weld pool and by the amount of dilution of the weld pool by the base plate. These compositions are controlled by chemical reactions at four separate zones: the melted electrode tip, the detached droplet, the hot weld pool immediately below the arc, and the cooling and solidifying weld pool behind the arc. Thermochemical reactions occur at all four zones and move the chemistry in the direction of chemical equilibrium. But electrochemical reactions occur only at the melted electrode tip and in the hot weld pool immediately below the arc. The electrochemical reactions would result from ionic conduction of a portion of the welding current through the molten slag layer. Therefore, only thermochemical reactions are expected to occur at the surface of the detached KEY W O R D S Submerged Arc Welding Weld Metal Composition Electrochemical Reaction Thermochemical Reaction Chemical Analyses SAW Alloy Elements Flux Composition Electrode Composition Welding Speed Effect droplets and solidifying weld pool since these parts are no longer carrying current. The most important chemical considerations for submerged arc welding include the control of oxygen, oxidation losses of alloy elements, and the pickup of undesirable elements from the slag. A number of investigations have been made concerning the interaction between the slag and the metal in submerged arc welding of steel. Most of these investigations were based solely on thermochemical reactions (Refs. 1-9), although lately a few investigators have considered the electrochemical reactions that occur when direct current is used in welding. Frost (Ref. 10) considered the different chemical effects at the anode and cathode in electroslag welding. Blander and Olson (Ref. 11) postulated an electrochemical mechanism for the alteration of weld metal chemistry in submerged arc welding. Electrochemical and Thermochemical Reactions Electrochemical reactions could be an important factor governing the chemistry of weld metal in direct current welding. Electrochemical effects can occur at the interfaces of the slag with the hot weld pool and the melted electrode tip. The relative numbers of ions and electrons in the slag govern the importance of these effects, which could be major factors controlling weld metal chemistry. When liquid slag has an interface with the molten metal, the electrochemical reactions are relatively simple to understand. This type of interface is present in submerged arc welding. The possible anodic reactions include the oxidation of iron and alloy elements, and the discharge and pickup of oxygen anions from the slag M (metal) + n O 2 " (slag) = M O „ (slag) + 2ne~ (D where M is iron or an alloy element at the electrode tip/slag or the weld pool/slag interface. Thus, substantial oxidation losses of alloy elements and pickup of oxygen are expected at the anode. The Table 1—Compositions of Steel Plate and Welding Wire (wt-%) Elements C Mn Si Mo Cr Ni Al Cu Ti P S o N Fe Steel Plate Welding Wire 0.18 1.25 0.05 0.03 0.077 0.06 0.004 0.036 0.001 0.018 0.031 0.002 0.004 balance 0.059 1.38 0.05 0.33 0.073 0.11 0.018 0.77 0.033 0.012 0.015 0.002 0.004 balance possible cathodic reactions include reduction of metallic cations from the slag and, to some extent, the refining of nonmetallic elements such as oxygen and sulfur M 2 + (slag) + 2e~ = M (metal) Si 4+ (slag) + 4e~ = Si (metal) O (metal) + 2 e " = 0 2 ~ (slag) (2) (3) (4) where M and Si represent electrodeposited metals at the interface. The large disparity in areas between the electrode tip and the weld pool results in different current densities. Current density is much higher at the electrode tip interface than at the weld pool interface. Thus, reactions at the electrode tip may exert a greater influence on the final weld metal chemistry than those at the weld pool. In addition to the electrochemical reactions, thermochemical reactions also play an important role in controlling the weld metal chemistry in submerged arc welding. The thermochemical reactions occur very rapidly because of high temperature. These thermochemical reactions include deoxidation reactions, such as those encountered in steel making, and reactions that lead to a closer approach to equilibrium between the flux and metal phase. Examples of such reactions would be silicon pickup from a high silica flux or the oxidation loss of transition elements through a deoxidation reaction. Si0 2 (slag) + 2M (metal) = Si (metal) + 2MO (slag) FeO (slag) + M (metal) = Fe (metal) + M O (slag) <5) (6) where M can be aluminum or calcium in Reactions 5 and 6 and manganese in Reaction 6 for the flux system used in this research. The droplet forms at the electrode tip and then travels through the molten flux and plasma. The entire process occurs in a few milliseconds (Refs. 12,13), and the temperature of the droplet is very high. Due to the high temperature, it is thermodynamically possible for chemical reac- tions to occur. A number of investigations have been made concerning the nature of chemical reactions at the melted electrode tips and the detached droplets (Refs. 5, 8, 12-18), and several investigators indicated that oxygen was transferred to the metal in these t w o zones (Refs. 2, 3, 13, 14, 18). In the hot weld pool immediately below the arc, the detached droplets become "diluted" with molten metal from the base plate. Although the slag/ metal interfacial contact area available for reaction is much smaller than that of the detached droplets, the strong turbulance existing in the hot weld pool creates an effective stirring of the liquid metal. Moreover, pickup of oxygen at this zone is favored by the increased time available for reaction. It is believed that the pickup of oxygen is the result of the oxygen solubility being exceeded in the hot weld pool. The zone of the molten weld pool behind the electrode starts to cool and solidify as the electrode moves away from it. Upon cooling of the metal in the weld pool from a high temperature to the solidification temperature, a supersaturation with respect to silicon and manganese deoxidation reactions occurs initially. Therefore, silicon and manganese will react with dissolved oxygen, and then the composition will move rapidly towards equilibrium. Figure 1 shows the schematic of expected variations in oxygen and silicon contents for an electrode-positive (reverse polarity) submerged arc weld due to electrochemical and thermochemical reactions. The curve shows the oxygen and silicon contents of steel in equilibrium with solid silica at some temperature. Before experiments were done, the composition variation was expected to follow the straight lines for an electrode-positive submerged arc weld. The anodic reaction at the melted electrode tip causes some ox- ygen pickup and silicon loss. The thermochemical reactions cause more oxygen pickup at the melted electrode tip and the detached droplet while the droplet is passed through the molten flux. At the cathodic weld pool, oxygen refining and silica reduction were expected, and then weld composition would vary with travel speed due to the difference in the amount of thermochemical deoxidation reaction. As the welding speed decreases, the amount of thermochemical deoxidation reaction increases because the heat input and the solidification time increase. Therefore, weld pool composition was expected to go to equilibrium composition as the travel speed decreases. Experimental Procedure Direct current electrode-negative (straight) and direct current electrodepositive (reverse) polarity submerged arc welds were made with 2.38 mm (V32 in.) commercial low-carbon steel welding wire on ASTM A36 steel plates and a water-cooled pure copper plate. The compositions of the steel plate and the welding wire are given in Table 1, and the composition of the commercial flux used is shown in Table 2. Figure 2 is a schematic drawing of a cross-section of the submerged arc welding process showing the melted electrode tips, the detached droplets and the base plate for both electrode-positive and electrode-negative polarities. The melted electrode tips, detached droplets and weld metal were collected and analyzed. The water-cooled copper plate was used as a base plate to collect the melted electrode tips and the detached droplets. The welding process was operated at a constant welding current of 585 A and a constant potential of 28.5 V. The constant current Expected Composition Variations for a DCEP Submerged Arc Weld Cathodic Weld Pool Fig. 1 — Schematic of expected variations in oxygen and silicon contents for an electrode-positive polarity submerged arc weld. i a Thermochemical Reactions in t h e Weld Pool <D &0 l>» X o Thermochemical Equilibrium Silicon (wt.%) WEEDING RESEARCH SUPPtEMENT 1447-s Table 2—Composition of Welding Flux (wt-%) Substance Amount Si0 2 AI2O3 MgO CaF2 CaO MnO Ti02 Na203 Fe 2 0 3 C 11.22 18.14 33.23 25.26 6.92 1.15 0.90 0.82 1.99 0.37 was obtained by adjusting the electrode velocity, which was 72 mm/s (170 in./ min) for the anodic wire, and 99 mm/s (235 in./min) for the cathodic wire. The electrode tips were collected by stopping the welding process, pulling the electrode away from the weld pool and cutting off the tip. The liquid metal droplets are released from the electrode tip and travel through the molten flux. The detached droplets were collected from welds made at a high velocity over a water-cooled copper plate so that the droplets are suspended in the molten flux. The detached droplets were extracted from the ground slag by magnetic separation. The speed of quenching attained is sufficient to freeze the metal composition established at high temperature. Single pass, bead-on-plate welds were made on steel plates at several welding speeds (1.5534.67 mm/s) with constant voltage (28.5 V) and current (580 A) for both polarities. The wire feed speed was adjusted to maintain the constant current. using a LECO interstitial analyzer, i.e., fusion in a graphite crucible under inert atmosphere. A Baird — Atomic emission spectrometer was used to determine manganese, silicon and other alloy elements in weld metals, welding wire and electrode tips. The electrode tips and wires were flattened in a rolling mill to get enough area for analysis. The detached droplets were analyzed using the wavelength dispersive analyzer on a JEOL scanning electron microscope. A metallurgical model by Their (Ref. 5) is adopted to show the extent of element transfer between the weld metal and flux. Its application gives quantitative data for the gain or loss of elements arising from slag/metal reactions. The transfer efficiency into the weld can be expressed in terms of the difference between analytical and nominal compositions. The difference between analytical and nominal compositions is defined as delta (A) quantity. The analytical composition is obtained by chemical analysis methods and the nominal composition can be obtained by calculations based on the detached droplet and plate compositions and dilution. A positive concentration change (A > 0) indicates a gain or pickup of a particular element, i.e., transfer of element from the slag to the weld metal. A negative change (A < 0) indicates a loss, i.e., transfer from the weld metal to the slag. of the high current densities, and thermochemical reactions are expected because of the high temperature and the generally large temperature-dependent differences in chemical potentials of the various reactants and products in the flux and metal phases. An examination of the welding wire, steel plate and flux compositions in Tables 1 and 2 shows that the wire and steel plate have very low silicon and oxygen concentrations, and a relatively high manganese concentration, while the flux has a high silica activity and a relatively low manganese-oxide/iron-oxide ratio, which is far from equilibrium with the welding wire and steel plate. Thus, the manganese content of the welding wire and steel plate would be expected to drop as a result of thermochemical oxidation losses to the flux, and the silicon and oxygen content would be expected to increase because of the reaction with the flux. The reactions at the melted electrode tip, the detached droplet and the weld pool were considered. The chemical analysis results show that a substantial difference exists between the chemistries of anode and cathode. These differences are the result of electrochemical reactions. Figure 3 shows the plot of the average oxygen contents of the welding wire, the melted electrode tips, and the detached droplets for both electrode-negative and electrode-positive polarity welding modes. This plot shows a very low oxygen Results and Discussion content in the welding wire (20 ppm) and a very significant oxygen pickup in the The purpose of this investigation is to melted electrode tips for both polarities. consider the relative influence of thermoThe influence of thermochemical oxygen chemical and electrochemical reactions pickup is shown by the fact that significant on the weld metal chemistry. Electrooxygen pickup is observed in both elecchemical reactions are expected because Analyses for oxygen were carried out trode-positive and electrode-negative configurations. This excess oxygen came from the surrounding atmosphere and (-) decomposition of oxide components in the flux. The influence of electrochemical reactions is shown by the fact that the oxwire ygen content of the anode in the elec(2.4mm) trode-positive polarity power mode (591 ppm) is over twice that of the cathode in molten arc the electrode-negative polarity power flux plasma mode (277 ppm). This oxygen content difference is due to oxygen pickup at the anode and oxygen refining at the cathode. The real difference is somewhat less since more wire is fed and melted at the cathode for a fixed current, thus diluting the total electrochemical and thermochemical effect at the cathode. If the electrochemical and thermochemical reactions were considered as separate steps, the average melted electrode tip oxygen concentration for the t w o polarities could be considered to crudely represent the thermochemical contribution, and the separation of t w o concentrations from this mean (a) Reverse Polarity (DCEP) (b) S t r a i g h t Polarity (DCEN) would represent the electrochemical efFig. 2 — Schematic of the cross-section of a submerged arc welding process showing the melted fects. However, the different wire feed welding wire tips, the detached droplets and the base plate for both electrode-positive and elecrates cloud this interpretation. After the trode-negative polarities. (+) 448-s | DECEMBER 1990 0 6 1400 1200 1000 S 0. 5 EHM 1 | 53 Anode Wire Cathode Z tu | | Wire EZH Anode V////\ Cathode 2 a. O 0.4 800 x a 0 3 oc < o o 600 - 0 2 400 o 0. I ' 200 • 0 0 Wire Electrode Tip Wire Droplet Figures 4 a n d 5 s h o w the average silicon a n d manganese c o n t e n t s in the initial e l e c t r o d e , the m e l t e d e l e c t r o d e tip and the d e t a c h e d d r o p l e t . The m e l t e d elect r o d e tips s h o w t h e increases in silicon c o n c e n t r a t i o n (less increase at the a n o d e a n d m o r e increase at the c a t h o d e ) a n d the decreases in manganese c o n c e n t r a t i o n (less decrease at the c a t h o d e a n d m o r e decrease at the a n o d e ) for b o t h polarities. This is e v i d e n c e that b o t h t h e r m o c h e m i c a l a n d electrochemical reactions o c c u r r e d at the m e l t e d e l e c t r o d e tip. T h e initial w e l d ing w i r e has a v e r y l o w silicon c o n t e n t , w h i l e the flux has a high silicon-oxide c o n tent. This causes the t h e r m o c h e m i c a l p i c k u p of silicon f r o m the flux. T h e elect r o c h e m i c a l influence is significant, as indic a t e d by the fact that the c a t h o d i c elect r o d e tip silicon c o n t e n t is a b o u t 0.06 w t % higher than that of the anodic e l e c t r o d e tip, a n d by t h e fact that t h e c a t h o d e f e e d rate is higher than the a n o d e f e e d rate, w h i c h means the t o t a l a m o u n t of silicon in t h e c a t h o d i c e l e c t r o d e tip is relatively higher than indicated in Fig. 4. Both ther- Electrode I Droplet OC a. O _i Ui > Ul a Tip Fig. 4 —Average silicon contents of the initial wire, the electrode tips, and the detached droplets for both electrode-negative (cathodic wire) and electrode-positive (anodic wire) polarities. Fig. 3—Average oxygen contents of the welding wire, the electrode tips and the detached droplets for both electrode-negative (cathodic wire) and electrode-positive (anodic wire) polarities. m o l t e n d r o p l e t separates f r o m t h e w i r e , the electrochemical reaction ceases. But the t h e r m o c h e m i c a l reaction continues w h i l e the d r o p l e t is falling t h r o u g h the m o l t e n slag. T h e r e f o r e , t h e d e t a c h e d d r o p l e t s h o w s higher o x y g e n c o n t e n t t h a n the m e l t e d e l e c t r o d e tip d u e t o the increase in o x y g e n c o n t e n t b y the c o n t i n uous d e c o m p o s i t i o n of flux. Even t h o u g h electrochemical reaction d o e s not occur in d e t a c h e d d r o p l e t s , the results o f o x y g e n analysis still s h o w the electrochemical reaction e f f e c t at t h e m e l t e d e l e c t r o d e tips as indicated b y the d i f f e r e n c e in o x y gen c o n t e n t s b e t w e e n a n o d i c a n d cat h o d i c droplets. ;',',• Ul V) Ul m o c h e m i c a l a n d electrochemical reactions are also indicated in t h e case o f manganese; h o w e v e r , t h e high manganese c o n t e n t in t h e e l e c t r o d e a n d the l o w manganese-oxide (MnO)/iron-oxide (Fe203) ratio in t h e flux lead t o t h e r m o chemical manganese loss at the m e l t e d e l e c t r o d e tip. T h e r e f o r e , manganese o x i d a t i o n a n d silicon r e d u c t i o n reactions are m a j o r t h e r m o c h e m i c a l reactions in this system. T h e changes in the silicon a n d manganese c o n c e n t r a t i o n s f r o m the elect r o d e tip t o t h e d e t a c h e d d r o p l e t are mostly t h e r m o c h e m i c a l . W i t h silicon, h o w e v e r , t h e r e is a decrease rather than an e x p e c t e d increase in silicon c o n t e n t of t h e d e t a c h e d d r o p l e t c o m p a r e d t o the m e l t e d e l e c t r o d e tip, indicating that a large fract i o n of the silicon in the d r o p l e t has back reacted w i t h m o r e n o b l e metal oxides in the flux {e.g., Fe203). O n e o f t h e possible driving forces f o r this reaction is related t o the possibility that the d r o p l e t is at a l o w e r t e m p e r a t u r e and has a higher o x y g e n c o n t e n t than t h e tip. T h e average manganese c o n t e n t is f u r t h e r decreased b y t h e r m o c h e m i c a l reactions w i t h m o r e n o ble metal oxides in t h e flux w h e n g o i n g f r o m t h e e l e c t r o d e tip t o the d e t a c h e d d r o p l e t , w h i c h falls t h r o u g h a n d reacts w i t h the flux. Figure 6 c o m p a r e s the d e t a c h e d d r o p let c o m p o s i t i o n s f o r the various alloy elements. Silicon, a l u m i n u m and manganese 3.0 2.5 I 1 Wire ESS3 r tn UJ z <t o Cathode 2.0 Fig. 5 —Average manganese contents of the initial wire, the electrode tips and the detached droplets for both electrode-negative (cathodic wire) and electrode-positive (anodic wire) polarities. o tr < ui CO Ul cc z Ul S a. O I a oc < ui (/> Ul oc a. O _i UJ > 4 Ul in ui CE z I .5 ui 1.0 3> 2 a. ui a u cc < UJ <n 0.5 Wire Electrode Tip Droplet W E L D I N G RESEARCH SUPPLEMENT 1449-s 2.50 0.50 DROPLET COMPOSITION ^ 0.40 2.00 fc? o Anode Wire Cathode 0.30 1.50 DJ in <D C D CT C D < 0.20- 1.00 o o o 0.10 0 ILJI Si Al Ni -0.50 jtt Cr Ti Mo 0 Mn Fig. 6 Average droplet compositions for silicon, aluminum, nickel, chromium, molybdenum, titanium and manganese for electrode-negative and electrode-positive polarities compared with the initial welding wire compositions. s h o w higher c o n c e n t r a t i o n s in the cathodic d r o p l e t s than in the anodic d r o p lets. This is largely caused b y oxidation losses t o the flux at the a n o d e and electrochemical r e d u c t i o n f r o m the flux at the c a t h o d e d u r i n g the reaction at the m e l t e d e l e c t r o d e tip. T h e differences for nickel, titanium a n d c h r o m i u m are of the o r d e r of t h e analytical uncertainties a n d are thus inconclusive. M o l y b d e n u m s h o w s the o p posite t r e n d . That is, the c o n c e n t r a t i o n in the a n o d e is higher t h a n that o f the catho d e . This b e h a v i o r is difficult t o explain in terms of m o l y b d e n u m r e a c t i o n alone, b u t if iron reaction is also taken into a c c o u n t , it can b e explained easily. Iron is the m a jor e l e c t r o d e constituent and it is m o r e easily o x i d i z e d t h a n m o l y b d e n u m . T h e r e f o r e , the loss of iron at t h e a n o d e and the gain of i r o n at t h e c a t h o d e are relatively greater than those o f m o l y b d e n u m , a n d these cause an increase in m o l y b d e n u m c o n c e n t r a t i o n at the a n o d e and a d e crease at the c a t h o d e . Thus, this b e h a v i o r of m o l y b d e n u m is also the result o f electrochemical reaction. Figures 7 t h r o u g h 14 s h o w the results of chemical analyses of the a n o d e a n d catho d e w e l d metal f o r silicon, manganese, a l u m i n u m , m o l y b d e n u m and o x y g e n as a f u n c t i o n of w e l d i n g s p e e d . T h e results for the a n o d e a n d c a t h o d e of each element are p l o t t e d t o g e t h e r . These results s h o w that electrochemical reactions cause substantial changes in w e l d metal chemistry. Figure 7 illustrates t h e variations in delta silicon d u e t o polarity. High transient c o n c e n t r a t i o n of o x y g e n m a y exist in the liquid metal at t h e hot w e l d p o o l as a result of high solubility at e l e v a t e d t e m p e r a t u r e . O n s l o w c o o l i n g d o w n t o the solidification t e m p e r a t u r e , this will lead t o s p o n t a n e o u s reaction a n d losses of dissolved silicon. The silicon loss must be d u e t o the f o r m a t i o n o f s o m e d e o x i d a t i o n reaction p r o d uct. It is generally a c c e p t e d that f o r m a t i o n of silicon o x i d e (Si02) takes place w h e n sufficient o x y g e n is available. But silicon loss is r e c o v e r e d b y electrochemical r e d u c t i o n reaction at the c a t h o d e a n d i n creased at t h e a n o d e b y electrochemical oxidation reaction. T h e r e f o r e , silicon s h o w s m u c h loss at the a n o d e , and a little gain or almost n o change at the c a t h o d e . Figure 8 s h o w s the variations in delta manganese d u e t o polarity. Similar t o silic o n , o x i d a t i o n o f manganese is f a v o r e d b y the l o w e r t e m p e r a t u r e prevailing in the c o o l e r part o f the w e l d p o o l . Here, m a n ganese will react w i t h dissolved o x y g e n t o f o r m slags that exhibit a large loss of m a n ganese in b o t h a n o d e a n d c a t h o d e w e l d metal. T h e reason w h y manganese s h o w s extensive losses in b o t h cases is because the flux has a little manganese o x i d e ( M n O ) a n d the base plate has a high m a n ganese c o n t e n t . T h e r e f o r e , manganese can b e o x i d i z e d easily. A n o t h e r reason f o r manganese loss can be a result of t h e e v a p o r a t i o n because v a p o r pressure i n creases strongly w i t h t e m p e r a t u r e . But the difference in delta manganese d u e t o p o larity s h o w s t h e effect of electrochemical reaction. That is, the c a t h o d e s h o w s less loss than the a n o d e because of the elect r o c h e m i c a l r e d u c t i o n reaction at the catho d e , and the electrochemical o x i d a t i o n reaction at the a n o d e . Variations in delta a l u m i n u m are s h o w n in Fig. 9. A l u m i n u m , like silicon and m a n ganese, is also o x i d i z e d w h i l e the t e m p e r ature of t h e w e l d p o o l is l o w e r e d t o t h e 0.15 Manganese Change in the Weld Pool Silicon Change in Weld Pool 0.00 0.10 Cathode -0.05 6? % -0.10 0.05 "5 Cathode <*A a) 171 0) 0.00 -0.15 o cn L -0.20 D -0.05 Anode < -0.25 - -0.10 -0.30 -0.15 I | I I I | I I I | I I I | I I I | I r I i I I I I I—r—i—]—I—i—r- 0.0 0.4 0.8 1.2 Travel 1.6 2.0 Speed 2.4 2.8 (cm/s) 3.2 3.6 Fig. 7 — Gain or loss of silicon due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. 450-s | DECEMBER 1990 -0.35 Anode 0.0 i i i I i i i l i i i I i i i I i i i l i i i I i i i I i i i I i i 0.4 0.8 1.2 Travel 1.6 2.0 Speed 2.4 2.8 (cm/s) 3.2 3.6 Fig. 8 — Gain or loss of manganese due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. 0.15 0.15 Molybdenum Change in the Weld Pool Aluminum Change in the Weld Pool 0.10 - 0.10 »? fc? "J '—' E j? 5 0.05 Anode 0.05 o 0.00 % A E A A 0.00 TJ A Cathode >-• < -0.05 - ° O o o o o o -0.15 -0.10 - -0.15 i l i i i l i i i l i i i l i i i l i i i I i i i I i i i l i i 0.0 0.4 0.8 1.2 Travel 1.6 2.0 Speed 2.4 2.8 (cm/s) 3.2 Figure 10 s h o w s the variations in delta m o l y b d e n u m d u e t o polarity. M o l y b d e - | I I I | I I J 1 I I I ; I I I | i I I [ I i 0.0 3.6 Fig. 9 — Gain or loss of aluminum due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. solidification t e m p e r a t u r e . A l u m i n u m o x ide (AI2O3) is stable at high t e m p e r a t u r e rather than silicon o x i d e (Si02> a n d m a n ganese o x i d e ( M n O ) , as indicated in the Ellingham diagram. Therefore, even t h o u g h the flux contains a large a m o u n t of aluminum o x i d e , it is difficult t o pick u p the a l u m i n u m f r o m the slag b y e l e c t r o c h e m i cal r e d u c t i o n reaction at the c a t h o d e w e l d p o o l . So, t h e results s h o w the a l u m i n u m losses e v e n at t h e c a t h o d e w e l d p o o l . But t h e lesser loss at the c a t h o d e is the e v i d e n c e f o r the electrochemical reaction. -0.05 < Anode -0.10 0.4 0.8 1.2 Travel 1.6 2.0 Speed 1 i i i | i I I | 2.4 2.8 (cm/s) 3.2 3.6 Fig. 10 — Gain or loss oi molybdenum due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. n u m changes s h o w the o p p o s i t e t r e n d as in the m e l t e d e l e c t r o d e tip. This b e h a v i o r of m o l y b d e n u m is the result of iron losses at t h e a n o d e and p i c k u p at the c a t h o d e as discussed previously. Figures 11 t h r o u g h 13 s h o w the variations in delta nickel, c h r o m i u m a n d titan i u m d u e t o polarity. Those elements also s h o w a little electrochemical effect. But t h e differences b e t w e e n a n o d e and catho d e are of the o r d e r of t h e analytical u n certainties and are thus inconclusive. Figure 14 s h o w s the variations in delta o x y g e n d u e t o polarity. O x y g e n losses are s h o w n at b o t h c a t h o d e and a n o d e , a n d the c a t h o d e s h o w s less loss than the a n o d e . This is t h e result of t h e difference in the s l a g / m e t a l interfacial contact area available f o r d e o x i d a t i o n reaction. T h e area of the c a t h o d e is smaller than that of t h e a n o d e . T h e r e f o r e , the separation of d e o x i d a t i o n p r o d u c t s at the a n o d e is easier than that at t h e c a t h o d e . Thus, electrochemical effect may be s w e p t o u t b y t h e r m o c h e m i c a l reaction. Figure 15 is the c o m p o s i t i o n m a p for b o t h electrode-negative and electrodepositive polarity s u b m e r g e d arc w e l d i n g , s h o w i n g the variations in o x y g e n and silic o n c o n t e n t s d u r i n g w e l d i n g . T h e curves are the plots of the silicon a n d o x y g e n c o n t e n t s of steel in equilibrium w i t h solid 0.15 0.15 Chromium Change in the Weld Pool Nickel Change in the Weld Pool 0.10 0.10 K °05 % — a) o Cathode "5 0.05 - Cathode Cathode tb -J&g, A A —A— Qp OQ o 0.00 o A A O O " 0 A 0 0.00 A Anode Anode -0.05 <-> - 0 . 0 5 -0.10 -0.10 -0.15 0.0 0.4 0.8 1.2 Travel i i I 1.6 2.0 Speed A o o -0.15 2.4 2.8 (cm/s) 3.2 3.6 Fig. 11 — Gain or loss of nickel due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. i I i i i 0.0 0.4 0.8 1.2 Travel 1.6 2.0 Speed 2.4 2.8 (cm/s) 3.2 3.6 Fig. 12 — Gain or loss of chromium due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. W E L D I N G RESEARCH S U P P L E M E N T 1451-s 0.15 100 Oxygen Change in the Weld Pool Titanium Change in Weld Pool 0.10 Cathode E 0.05 Cathode E A^ 0.00 $$ A Anode CD aP' cn c o P -100- Q. Q. -—'-200C 5^-300X O Anode -0.05 -400 -0.10 - -0.15 0.0 -500 0.4 0.8 1.2 Travel 1.6 2.0 Speed 2.4 2.8 (cm/s) 3.2 -600-|-n 3.6 0.0 Fig. 13 — Gain or loss of titanium due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. silica at 1 6 0 0 ° C (2912°F) a n d 1 8 0 0 ° C (3272°F). T h e c o m p o s i t i o n s of w e l d i n g w i r e , m e l t e d e l e c t r o d e tips, d e t a c h e d droplets and w e l d metal are p l o t t e d o n the diagram f o r b o t h polarities. T h e w i r e has l o w silicon a n d o x y g e n c o n t e n t s . Both anodic a n d c a t h o d i c e l e c t r o d e tips s h o w an increase in silicon c o n t e n t d u e t o the o x i d a t i o n o f i r o n a n d manganese, a n d in oxygen content due to decomposition of flux and c o n t a m i n a t i o n f r o m the a t m o sphere. But the cathodic e l e c t r o d e tip s h o w s a greater increase in silicon a n d less increase in o x y g e n , d u e t o t h e e l e c t r o chemical silicon r e d u c t i o n a n d o x y g e n refining reactions. W h i l e the d e t a c h e d d r o p lets are falling t h r o u g h the m o l t e n flux, the droplets pick u p the o x y g e n b y flux d e c o m p o s i t i o n a n d c o n t a m i n a t i o n f r o m the a t m o s p h e r e . T h e r e f o r e , the o x y g e n c o n - Fig. 15-The composition map for direct current electrode-negative (DCEN) and direct current electrode-positive (DCEP) polarity submerged arc welding showing the variations in oxygen and si/icon contents during welding. 0.20 i i i i i i i i i i i i i i i i i i i i i i i i | i i i 0.4 Conclusions 1) B o t h e l e c t r o c h e m i c a l a n d t h e r m o chemical reactions are significant in subm e r g e d arc w e l d i n g . 2) T h e t h e r m o c h e m i c a l reactions m o v e the flux a n d w e l d metal c o m p o s i t i o n s t o w a r d chemical equilibrium. In this study, manganese activity w a s higher in t h e metal than in the flux; t h e r e f o r e , manga- 0.15 DCEP 0.10 DCEN roplet x O 2.4 2.8 (cm/s) 3.2 3.6 nese oxidation loss f r o m t h e metal t o t h e flux w a s o b s e r v e d . Silicon activity w a s higher in t h e flux; t h e r e f o r e , a t h e r m o chemical silicon p i c k u p b y the w e l d metal was observed. 3) T h e electrochemical reactions at the a n o d e include o x i d a t i o n losses of alloy elements t o the flux and the discharge a n d p i c k u p of o x y g e n anions f r o m t h e flux. T h e electrochemical reactions at the catho d e include the r e d u c t i o n of metal ions f r o m the flux a n d the refining of o x y g e n . 4) T h e r m o c h e m i c a l a n d e l e c t r o c h e m i cal c o m p o s i t i o n changes are greater at a l o w than at a high w e l d i n g s p e e d . Electrochemical reactions are e n h a n c e d b y higher, total current f l o w per unit v o l u m e of w e l d m e t a l . T h e r m o c h e m i c a l reactions at a l o w w e l d i n g speed are e n h a n c e d b y higher t e m p e r a t u r e s a n d longer reaction time b e f o r e solidification. 5) C o m p o s i t i o n paths f o r the silicono x y g e n equilibrium are different for direct current e l e c t r o d e - p o s i t i v e (reverse polarity) a n d direct current e l e c t r o d e - n e g a t i v e (straight polarity) w e l d s . Composition Maps for DCEP and DCEN Submerged Arc Welding Processes ^ 1.6 2.0 Speed Fig. 14 — Gain or loss of oxygen due to the reactions in the weld pool for electrode-negative and electrode-positive polarities as a function of welding speed. tents in the droplets are higher than those in t h e e l e c t r o d e tips f o r b o t h polarities. T h e w e l d metal s h o w s decreases in silicon and o x y g e n c o n t e n t s b y d e o x i d a t i o n r e action a n d c o m p o s i t i o n variation d u e t o w e l d i n g s p e e d . As the w e l d i n g speed d e creases, the c o m p o s i t i o n of the w e l d metal a p p r o a c h e s the equilibrium c o m p o sition. % 0.8 1.2 Travel 6) T h e total gain or loss of alloy elements in w e l d metal is influenced b y t h e c o m p o s i t i o n s of flux, e l e c t r o d e and base plate, a n d b y w e l d i n g process conditions. Further experiments w i t h synthetic fluxes, w h i c h are chosen t o minimize t h e r m o c h e m i c a l reactions, are p l a n n e d and should help t o b e t t e r define the relative i m p o r t a n c e of electrochemical reactions. 0.05 Acknowledgments 0.00 0.00 0.10 Silicon 452-s I DECEMBER 1 9 9 0 0.20 (wt.%) 0.30 J. H. Kim, R. H. Frost and D. L. O l s o n wish t o a c k n o w l e d g e t h e s u p p o r t of the U.S. A r m y Research O f f i c e at the C o l o r a d o School o f M i n e s , a n d M . Blander ack n o w l e d g e s the s u p p o r t o f the O f f i c e o f Naval Research at A r g o n n e National Laboratory under Navy Order No. N0001485-F-0097. References 1. Belton, C. R., Moore, T.)., and Tankins, E. S. 1963. Slag-metal reactions in submerged-arc welding. Welding journal 42(7): 289-s to 297-s. 2. Chai, C. S„ and Eagar, T. W . 1982. Slagmetal reactions in binary CaF2-metal oxide welding fluxes. Welding journal 61(7): 229-s to 232-s. 3. Chai, C. S„ and Eagar, T. W . 1981. Slagmetal equilibrium during submerged arc welding. Metall. Trans. B 12B(9): 539 to 547. 4. Indacochea, ). E., Blander, M., Christensen, N., and Olson, D. L. 1985. Chemical reactions during submerged arc welding with FeOMnO-Si0 2 fluxes. Metall. Trans. B 16B(6): 237 to 245. 5. Their, H. 1980. Metallurgical reactions in submerged arc welding. Proc. Intl. Conf. on Weld Pool Chemistry and Metallurgy. The Welding Institute, London, England, pp. 271 to 278. 6. North, T. H., Bell, H. B., Nowicki, A., and Craig, I. 1978. Slag/metal interaction, oxygen and toughness in submerged arc welding. Welding lournal 57(3): 63-s to 75-s. 7. Davis, M. L. E„ and Coe, F. R. 1977. The chemistry of submerged arc welding fluxes. The Welding Institute. 3 9 / 1 9 7 7 / M . 8. Mitra, U. 1984. Kinetics of slag metal reactions during submerged arc welding of steel. Ph.D. dissertation. MIT, Cambridge, Mass. 9. Blander, M., and Olson, D. L. 1984. Thermodynamic and kinetic factors in the pyrochemistry of submerged arc flux welding of iron-based alloys. Proc. Intl. Symp. on Metallurgical Slags and Fluxes. The Met. Soc. of AIME. 10. Frost, R. H., Olson, D. L, and Edwards, C. R. 1983. The influence of electrochemical reactions on the chemistry of the electroslag welding process. Engineering foundation conferences. Modeling of Casting and Welding Processes II. eds. |. A. Dantzig and I. T. Berry. The Met. Soc. of AIME. 11. Blander, M., and Olson, D. L. 1986. Electrochemical effects on weld pool chemistry in submerged arc and D. C. electroslag welding. Proc. Intl. Conf. on Trends in Welding Research. 12. Pokhodnya, I. K„ and Kostenko, B. A. 1965. Fusion of electrode metal and its interaction with the slag during submerged arc welding. Avt. Svarka 10: 16 to 22. 13. Potapov, N. N., and Lyubavski, K. V. 1971. Oxygen content of weld metal deposited by automatic submerged arc welding. Svar. Proiz. 1: 11 to 15. 14. North, T. H. 1977. The distribution of manganese between slag and metal during submerged arc welding. Welding Research Abroad 23: 2 to 13. 15. Potapov, N. N., and Lyubavski, K. V. 1971. Interaction between the metal and slag in the reaction zone during submerged arc welding. Svar. Proiz. 7: 9 to 11. 16. Norin, P. A., and Malyshev, N. I. 1982. Losses of manganese from electrode droplets in arc welding in air. Svar. Proiz. 2: 21 to 33. 17. Grong, O., and Christensen, N. 1982. Factors controlling weld metal chemistry. Final Report Contract No. DATA 376-81-C-0309. European Research Office of the U.S. Army. 18. Lau, T „ Weatherly, G. C , and McLean, A. 1985. The source of oxygen and nitrogen contamination in submerged arc welding using CaO-Al203 based fluxes. Welding lournal 64(12): 343-s to 347-s. WRC Bulletin 352 April 1990 In October 1987, t h e PVRC Steering and Technical C o m m i t t e e s on Piping Systems established a task g r o u p on independent support m o t i o n (ISM) t o evaluate t h e technical merits of using t h e ISM m e t h o d of spectral analysis in t h e design and analysis of nuclear power plant piping systems. The results of t h e task group evaluation c u l m i n a t e d in a unanimous technical position t h a t t h e ISM m e t h o d of spectral seismic analysis provides m o r e accurate and generally less conservative response predictions t h a n t h e c o m m o n l y accepted envelope response spectra (ERS) m e t h o d , and are r e p o r t e d in this WRC Bulletin. The price of WRC Bulletin 3 5 2 is $ 2 5 . 0 0 per copy, plus $ 5 . 0 0 for U.S., or $ 1 0 . 0 0 for overseas, postage and handling. Orders should be sent w i t h p a y m e n t t o t h e Welding Research Council, 3 4 5 E. 4 7 t h St., Room 1 3 0 1 , New York, NY 1 0 0 1 7 . WRC Bulletin 354 June 1990 The t w o papers contained in this bulletin provide definitive information concerning t h e elevated t e m perature r u p t u r e behavior of 2 V 4 C r - l M o weld metals. ( 1 ) Failure Analysis of a Service-Exposed Hot Reheat Steam Line in a Utility Steam Plant By C. D. Lundin, K. K. Khan, 0. Yang, S. Hilton and W. Zielke ( 2 ) The Influence of Flux Composition of the Elevated Temperature Properties of Cr-Mo Submerged Arc Weldments By J. F. Henry, F. V. Ellis and C. D. Lundin The first paper gives a detailed metallurgical failure analysis of cracking in a longitudinally welded h o t reheat pipe w i t h 184,000 hours of operation at 1 0 5 0 ° F . The second paper defines t h e role of t h e welding flux in submerged arc welding of 2 V 4 C r - l M o steel. Publication of this r e p o r t was sponsored by t h e Steering and Technical C o m m i t t e e s on Piping Systems of t h e Pressure Vessel Research Council of t h e Welding Research Council. The price of WRC Bulletin 3 5 4 is $ 5 0 . 0 0 per copy, plus $5.00 for U.S. and $ 1 0 . 0 0 for overseas postage and handling. Orders should be sent w i t h p a y m e n t to t h e Welding Research Council, 3 4 5 E. 4 7 t h St., Room 1 3 0 1 , New York, NY 1 0 0 1 7 . WELDING RESEARCH SUPPLEMENT 1453-s
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