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www.etasr.com Touileb et al.: Mixing Design for ATIG Morphology and Microstructure Study of 316L Stainless Steel 

 

Mixing Design for ATIG Morphology and 

Microstructure Study of 316L Stainless Steel 
 

Kamel Touileb 

Mechanical Engineering Department, 

College of Engineering, Prince Sattam 

Bin Abdulaziz University, 

Al Kharj, Saudi Arabia 

k.touileb@psau.edu.sa 

Abdejlil Hedhibi 

Mechanical Engineering Department, 

College of Engineering, Prince Sattam 

Bin Abdulaziz University, 

Al Kharj, Saudi Arabia 

a.hedhibi@psau.edu 

Rachid Djoudjou 

Mechanical Engineering Department, 

College of Engineering, Prince Sattam 

Bin Abdulaziz University, 

Al Kharj, Saudi Arabia 

r.djoudjou@psau.edu.sa 

Abousoufiane Ouis 

Mechanical Engineering Department, 

College of Engineering, Prince Sattam Bin Abdulaziz 

University, Al Kharj, Saudi Arabia 

a.ouis@psau.edu.sa 

Mohamed Lamjed Bouazizi 

Mechanical Engineering Department, 

College of Engineering, Prince Sattam Bin Abdulaziz 

University, Al Kharj, Saudi Arabia 

my.bouazizi@psau.edu.sa 
 

 

Abstract—This work is a study of the effects of oxides 

combination on the morphology of 316L stainless steel welds. A 

series of thirteen weld lines were carried out using thirteen 

different oxides. Based on the depth and ratio D/W results, three 

candidate oxides were selected: Ti2O, Mn2O3, and SiO2. Mixing 

method available in Minitab 17 software is the most appropriate 

method to find the optimal combinations to get the best depth 

and D/W ratio. According to simplex lattice degree four, nineteen 

combinations of these oxides were prepared. The results show 

that the optimal composition of flux was: 66%SiO2-34% Mn2O3. 

The depth and D/W ratio increased to 8.85mm and 0.98 

respectively for optimal ATIG, whereas for the conventional TIG 

welding, the depth and the ratio D/W didn't exceed 1.65mm and 

0.17 respectively. For TIG weld joint the hardness is about 47 

HRA and it increases to 77 HRA for the optimal ATIG weld 

joint. The absorbed energies in Charpy impact test are 146 and 

138kJ in the weld zone and in the heat affected zone respectively 

for the TIG welding and they dropped to 111 and 74kJ for the 

optimal ATIG welding. The fracture surface examined by 

scanning electron microscope (SEM) shows a ductile fracture for 

TIG weld with small dimples but ductile-brittle fracture for 

ATIG weld. Energy dispersive spectroscopy (EDS/SEM) analysis 

shows the formation of FeS2 and SiO2 in the weld zone causing 

low absorbed energy for ATIG weld. 

Keywords-ATIG; 316L austenitic stainless steel; ATIG welding 

mixing method; ternary flux 

I. INTRODUCTION 

TIG welding process is quite widespread. However, weld 
penetration varies from cast to cast and the maximum weld 
depth in a single pass does not exceed 3mm. Activated TIG 
(ATIG) welding proposed by Paton Institute-Kiev [1, 2] seems 
an appropriate process to overcome these weaknesses. ATIG 
welding uses the same equipment as TIG except a prior weld 
operation layer of activated flux paste is deposited on the 

workpiece. Hypotheses have been made to explain the 
phenomenon favoring a high weld depth. Authors in [3-6] 
proposed that the Marangoni convection is the most important 
factor in determining weld shape. Surfactant elements as S, Se, 
Te, O in weld pool affect the convection of molten metal 
leading to centripetal circulation of weld metal getting a depth 
of weld. Authors in [7, 8] applied the principle of electron 
absorption [9], electronegative elements as halides (fluorine) 
migrate to arc weld and capture outer arc electrons which 
contribute to contract the arc welding. This phenomenon 
increases the density of arc welding and the heat provided to 
weld pool. Authors in [10-12] proposed that high electrical 
resistance of flux components contributes to arc constriction. 
Many works were subsequently carried out using oxides like 
SiO2, TiO2, Cr2O3, Fe2O3, CaO, ZrO2, MgO [13-24], chlorides 
[25-27], and fluorides [28, 29] to improve weld depth. These 
studies showed an increasing in the weld depth without 
affecting the mechanical properties of the specimens [30, 31]. 
Other studies were dedicated to microstructure and mechanical 
properties [32-33]. In this work, 13 oxides were investigated on 
316L austenitic stainless steel. Design of experiments was used 
to predict the best combination of the tested oxides. Mixing 
method based on a simplex lattice degree four was the key tool 
to optimize the flux combination in order to enhance the depth 
and D/W ratio. 

II. EXPERIMENTAL PROCEDURE 

A. Materials 

The material used was the 316L stainless steel whose 
chemical composition is shown in Table I. Experiments 
consisted of welding a 20cm line on a rectangular plate of 6mm 
thickness. Before welding, the plates were cleaned with 
acetone. Flux powders were dried in furnace to eliminate 
humidity, and then mixed with methanol in 1:1 ratio. A flux 

Corresponding author: Kamel Touileb 



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layer less than 0.2mm thick was deposited on the surface to be 
welded. 

TABLE I.  316L CHEMICAL COMPOSISTION 

Element Percentage (%) 

C 0.018 

Mn 1.30 

Si 0.43 

P 0.034 

S 0.0029 

Cr 16.78 

Ni 10.00 

Mo 2005 

Ti 0.0042 

Cu 0.2082 

Co 0.226 

N (ppm) 321 

 

B. Welding Procedure 

A Tungsten Inert Gas welding machine was used. A water-
cooled torch with a standard 2% thoriated tungsten electrode 
rod having diameter of 3.2mm has been used for the 
experiments. The torch was mounted on a motorized carriage 
as shown in Figure 1. A series of tests were carried out with 
150A welding current and 15cm/min welding speed leading to 
a provided energy of 540kJ/m. The welding parameters for the 
TIG welding are listed in Table II. 

 

 

Fig. 1.  Experimental setup of TIG welding with flux paste (a motorized 
carriage, torch–workpiece). 

TABLE II.  WELDING PARAMETERS 

Welding speed 15cm/min 

Welding current 150A 

Arc length 2mm 

Electrode Tip Angle 45  ͦ

Shield gas on work piece Argon with flow rate 12l/min 

Shield gas back side Argon with flow rate 5l/min 

Welding mode Direct current electrode negative 

 

C. Mechanical Testing 

After welding, the samples were cut as shown in Figure 2 to 
acquire test samples for mechanical testing and weld 
morphology. The Rockwell hardness measurement was 
performed with a Digital Hardness Tester Model HRS-150. 
The hardness tests were conducted in the bulk of weld bead, 
and the results were the average of four indentations as shown 
in Figure 3. 

 

Fig. 2.  Different test specimens on welded TIG and ATIG plate 

 

Fig. 3.  Hardness test locations on weld bead 

Impact tests were carried out with the impact testing 
machine model JBS-500. The specimens were cut according to 
ASTM E23 and the impact tests were conducted in the weld 
bead and in the HAZ as shown in Figure 4. 

 

 

(a) 

 

(b) 

Fig. 4.  Test specimen for impact test (a) weld zone, (b) HAZ 

D. Experiment by Mixing Method Design (DOE) 

For the DOE, mixing method in mini tab 17 was applied 
and consequently the number of experiments to be conducted 
was reduced. In order to compare the effect of the flux on the 
tensile strength, 13 oxides (SiO2, TiO2, Fe2O3, Cr2O3, ZnO, 
ZrO2, CaO, Mn2O3, V2O5, MoO3, SrO2, CoO3, and MgO) were 



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tested. Among these oxides, 3 gave the best depth and D/W 
ratio and were selected to be used in the mixing design method. 
Based on the simplex lattice degree four designs, 19 
combinations have been selected. Nineteen weld lines were 
executed and samples for morphology, hardness and impact 
tests were cut. The optimizer module available in mini tab 17 
was used to get the optimal formulation of flux which is 
expected to give the best depth and D/W ratio of weld. Finally, 
using the optimal formulation, ATIG weld line has been carried 
out along with another weld line without flux (TIG). 

III. RESULTS AND DISCUSSION 

A. Depth D and D/W Ratio 

Figure 5 shows the weld depth results of ATIG weldment of 

the tested preliminary 14 oxides. The highest value of depth is 

6.04mm which is obtained for the sample welded with Mn2O3 

flux, followed by the sample welded with SiO2 flux (5.29mm), 

and then by the sample welded with TiO2 (4.81mm). So the 

oxides Mn2O3, SiO2, and TiO2 were selected. The results of the 

depth and D/W ratio for different proportions of the 3 selected 

oxides are shown in Table III. 

 

 

Fig. 5.  Depth of ATIG welds. 

TABLE III.  DIFFERENT COMPOSITIONS OF FLUXES, DEPTH AND D/W 

Exp. No. SiO2 % TiO2 % Mn2O3 % Depth (mm) D/W 

1 75 25 0 4.23 0.54 

2 75 0 25 6.72 0.92 

3 0 75 25 4.47 0.58 

4 25 75 0 4.61 0.61 

5 25 0 75 3.77 0.49 

6 0 25 75 3.95 0.53 

7 0 50 50 5.66 0.77 

8 50 0 50 6.63 0.90 

9 50 50 0 6.36 0.83 

10 50 25 25 6.66 0.86 

11 25 50 25 4.85 0.63 

12 25 25 50 3.48 0.43 

13 33.3 33.3 33.3 4.93 0.66 

14 66.67 16.67 16.67 5.01 0.72 

15 16.67 66.67 16.67 5.27 0.72 

16 16.67 16.67 66.67 4.70 0.64 

17 100 0 0 5.29 0.74 

18 0 100 0 4.81 0.66 

19 0 0 100 6.04 0.82 

 

B. Mixture Contour Plot 

Mixture contour plots for depth D and D/W were generated 
using Minitab software and are shown in Figure 6. The iso-
contour lines and the regions confined between them indicate 
different levels of depth or D/W. Different colors represent the 

different levels of the two properties. The interesting zone lies 
where the values of depth and D/W were higher. Optimizer 
module available in Minitab was used to predict the responses 
of depth and D/W ratio. The composite desirability is equal to 1 
(100%). It indicates that the parameters achieve favorable 
results for all responses, which means that both responses are 
within acceptable limits, as shown in Figure7. The predicted 
values are listed in Table IV. The optimal combination of flux 
is represented in Table V. 

 

 
(a) 

 
(b) 

Fig. 6.  Mixture contour of plot for (a) Depth and (b) D/W ratio. 

 

Fig. 7.  Optimization plot 

TABLE IV.  PREDICTED RESPONSES (UTS, HRA) OF WELD EXECUTED 
WITH OPTIMAL FLUX 

Responses Predicted responses Desirability 

Depth(mm) 7.01 100% 

D/W 0.96 100% 

TABLE V.  OPTIMAL COMPOSITION OF FLUX. 

variables SiO2 TiO2 Mn2O3 

Percentage (%)s 
66 0 34 

100 

 

C. Confirmation Test 

The confirmation test is the last step in the experimental 
process. Confirmation tests were conducted based on the 
optimum flux composition obtained in the mixing design 
method of Minitab. The experimental values of depth and D/W 
ratio of the optimal flux ATIG weld are reported in Table VI. 



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The results show the depth of optimized flux is greater than 
TIG weld by 5 times. The ratio D/W improved 6 times. The 
experimental values obtained for depth in ATIG and TIG welds 
are shown in Figure 8. The penetration weld of optimized flux 
(8.85mm) is greater than the maximum value predicted by the 
software (7.01mm). Furthermore, the D/W value obtained for 
ATIG weld (0.98) is very close to the maximum predicted 
value of 0.96 as shown in Figure 9. TIG molten metal behaves 
as pure metal with centrifugal convection leading to wide and 
sallow weld bead contrariwise. ATIG weld metal has a 
centripetal movement related to oxygen liberated from oxides 
during welding operation. The quantity of liquid melted in 
ATIG (51.51mm2) is higher than in TIG weld bead (14.2mm2) 
as shown in Figures10-11. 

TABLE VI.  MORPHOLOGY OF TIG AND ATIG WELDS. 

 ATIG(with optimal flux) TIG 

Depth(mm) 8.85 1.65 

W(mm) 9.04 9.92 

D/W 0.98 0.17 

 

 

Fig. 8.  Depths of ATIG and TIG welds 

 

 

Fig. 9.  D/W of ATIG and TIG welds 

 

 

Fig. 10.  Areas of ATIG and TIG welds 

D. Hardness Test 

The experimental values obtained for hardness are shown in 
Figure 12. ATIG hardness number of HRA=77 is greater than 
TIG hardness number of HRA=47. 

(a) 

 

(b) 

 

Fig. 11.  Morphology of (a) ATIG and (b) TIG welds 

 

Fig. 12.  Hardness HRA in weld zone for ATIG and TIG welds. 

E. Impact Test 

The experimental values obtained from the impact test are 
shown in Figures 13-14.  

 

 

Fig. 13.  Absorbed energy in weld zone for TIG and ATIG welds. 

 

Fig. 14.  Absorbed energy in HAZ for TIG and ATIG welds. 

The energies absorbed either in the weld zones or in HAZ 
of TIG welds are higher than the ones of ATIG welds. Figure 
15 shows the images of fractograph of the “V” notch Charpy 



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impact test conducted on scanning electronic microscope 
(SEM). The images show the formation of micro-voids, with 
multiple dimples which demonstrate that the fracture is in 
ductile mode in the cases of TIG weld zone (a) and in TIG heat 
affected zone (c). Combined ductile (small colonies with finer 
dimples) and brittle fracture mode formation characterizes the 
ATIG weld zone (b) and the ATIG affected zone (d). The 
combined ductile and brittle fracture mode leads to poor 
resistance to sudden impact loads. 

 

(a) TIG welded 
zone (500X ) 

 

(b) ATIG 
welded zone 

(500X ) 

 

(c) TIG heat 
affected zone 

(500X) 

 

(d) ATIG heat 
affected zone 

(500X) 

 

Fig. 15.  Fractograph of SS 316L impact charpy “V” notch 

F. Microstructure Study  

Microstructure study was performed in order to view the 
material properties after the welding in both TIG and ATIG 
weldings. 

1) EDS/SEM Analysis 

The results of EDS/SEM analysis in Figures 16 and 17 
show the presence of silicon, sulphur and oxygen in ATIG 
weld bead and in the heat affected zone, that lead to formations 
of inclusions as FeS2. Moreover, oxygen initiates microvoids 
and propagates by micro void coalescence, which facilitate the 
fracture phenomenon. These results can explain the low impact 
resistance in ATIG weld. The results of EDS/SEM analysis in 
Figures 18 and 19 show the presence of silicon in TIG weld 
zone in quantities close to the quantity in the received plate. 
The weld zone and the HAZ are free from oxygen and sulphur 
which can explain the withstanding of TIG weld to sudden 
impact. The results obtained with EDS/SEM regarding TIG 
weld may explain the high resistance to impact test. 

 

 

 

Fig. 16.  EDS/SEM spectrum analysis of fracture face of ATIG welded zone 

 

 

Fig. 17.  EDS/SEM spectrum analysis of fracture face of ATIG HAZ 



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TABLE VII.  ELEMENTS PRESENT IN FRACTURE FACE OF ATIG 
WELDED ZONE 

Element C Si Cr Mn Fe Ni O S 

Weight% 20.50 0.51 14.43 1.98 53.44 6.41 2.29 0.43 

TABLE VIII.  ELEMENTS PRESENT IN FRACTURE FACE OF ATIG HAZ  

Element C Si Cr Mn Fe Ni O S 

Weight % 21.17 0.56 14.57 1.43 52.93 6.57 2.36 0.42 

 

The results of EDS/SEM analysis in Figures 18 and 19 
show the presence of silicon in TIG weld zone. The weld zone 
and the HAZ are free from oxygen and sulphur which can 
explain the widstand of TIG weld to sudden impact. The results 
obtained with EDS/SEM regarding TIG weld may explain the 
high resistance to impact test. 

 

 

 

Fig. 18.  EDS/SEM spectrum analysis of fracture face of TIG welded zone 

TABLE IX.  ELEMENTS PRESENT IN FRACTURE FACE OF TIG WELDED 
ZONE 

Element C Si Cr Fe Ni 

Weight% 21.23 0.48 14.52 56.32 7.44 

 

 

 

Fig. 19.  EDS/SEM spectrum analysis of fracture face of TIG HAZ 

TABLE X.  ELEMENTS PRESENT IN FRACTURE FACE OF TIG HAZ 

Element C Cr Fe Ni 

Weight% 44.04 7.06 36.10 12.81 

 

2) Ferrite Proportions 

The measurement of ferrite content in the austenite matrix 
was conducted using area image processing software of 
Microvision Instruments. The weld zone appearance of ATIG 
and TIG was examined by SEM. The measurements were taken 
in 4 different locations in the weld zone and the results were 
the average of these measurements. Delta ferrite morphology 
has a vermicular network structure in both ATIG and TIG 
welds as shown in Figure 20. Results show ferrite content equal 
to 10.4% for ATIG. Instead, there is a decrease in ferrite 
content to 6.8% for TIG. This can be explained by the fact that 
in the case of ATIG operation, the weld bead is fully penetrated 
with a large weld bead area up to 55mm2. During ATIG weld 
operation, the activated flux has a beneficial effect in 
increasing the heat provided to weld pool and consequently the 
peak temperature in ATIG weld is greater comparatively to 
TIG weld leading to increase the proportion of delta ferrite 
retained in austenite matrix. On the other hand, in TIG welding, 
the bead is wide and shallow so the cooling rate is high. As the 
cooling rate is fast the transformation of delta ferrite to 
austenite is not completed, resulting on the presence of delta 
ferrite in the weld bead.  

 

(a) Delta ferrite 

in ATIG weld 
zone 

(FN=10.4%) 

 

(b) Delta 
ferrite in TIG 

weld zone 

(FN=6.8%) 

 

Fig. 20.  SEM micrograph of (a) ATIG weld zone and (b) TIG weld zone. 
Magnification 250X 

The ferrite content in heat affected zone is up to 4.6% in 
ATIG welding and decreases at 1.4% in TIG heat affected 
zone. In TIG, the delta ferrite is randomly distributed in 
globular form or in small slats as shown in Figure 21(b). 
However, in ATIG heat affected zone, delta ferrite looks-like 
elongated inclined stringers as shown in Figure 21(a). 

 



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(a) Delta ferrite in 

ATIG HAZ 
(FN=4.6%) 

 

(b) Delta ferrite in 
TIG HAZ (FN=1.4%) 

 

Fig. 21.  SEM micrograph of (a) ATIG HAZ and (b) TIG HAZ. 
Magnification 1000X 

IV. CONCLUSION 

This study was conducted on ATIG welding of austenitic 
316L. The results are summarized as follows: 

• Among 13 oxides tested, SiO2, TiO2 and Mn2O3 present the 
highest depth penetration. 

• The optimal flux is composed of 66% SiO2 and 34% 
Mn2O3. 

• The size of ATIG weld bead is bigger than the one of TIG 
weld bead. The activated flux enhances the heat provided to 
the weld pool leading to high proportion of retained delta 
ferrite (10.4%). However, TIG weld is wider and shallower 
so the molten metal cools rapidly in comparison with ATIG 
molten metal. In the case of TIG weld the transformation of 
delta ferrite to austenite is stopped earlier due to the fast 
cooling giving delta ferrite proportions up to 6.8%. 

• The hardness HRA property of ATIG weld is improved 
comparatively to TIG weld. This result is related with the 
high delta ferrite content in ATIG weld zone. 

• EDS/SEM analysis reveals the presence of FeS2, silicon, 
and oxygen in ATIG welded zone which could be the 
reason of the decrease of sudden impact load in comparison 
with TIG weld. 

• Mixing design method is the more appropriate tool to get 
optimal flux composition when depth and D/W ratio 
improvements are desirable. Based on experiments’ results, 
one can say that Minitab software can predict accurately the 
responses.  

ACKNOWLEDGEMENTS 

This work is supported by the Deanship of Scientific 
Research in Prince Sattam Bin Abdulaziz University, Saudi 

Arabia under the research project number 2017/01/7373. 
Authors acknowledge and thank Dr. Nabeel Alharthi, Director, 
Centre of Excellence for Research in Engineering Materials for 
his help in performing SEM/EDS analysis. 

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