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This study provides a comprehensive comparative analysis of Conventional Friction Stir Welding (CFSW) and Bobbin Tool Friction Stir Welding (BTFSW) for AA6061-T6 aluminum alloy plates. A factorial experimental design was employed to systematically investigate the effects of rotational speed, feed rate, tilt angle or pinching gap, plunge depth, and tool pin profile on joint performance. Regression models for ultimate tensile strength (UTS) and Vickers micro-hardness (HV) were developed and validated through analysis of variance (ANOVA), with all models exhibiting excellent fit (R2 > 0.99) and strong predictive capability. The results demonstrate that both CFSW and BTFSW can achieve high-quality, defect-free welds, with CFSW yielding a maximum UTS of 241.52 MPa and BTFSW achieving comparable strength and superior hardness (up to 101.26 HV with a threaded pin). ANOVA revealed rotational speed and tool profile as the most significant factors for UTS, while feed rate and pin geometry predominantly governed hardness. Response surface analysis identified pronounced interaction and quadratic effects, highlighting the importance of simultaneous optimization of multiple process parameters. BTFSW outperformed CFSW in terms of process flexibility, hardness, and defect mitigation, attributed to its symmetrical heat input and elimination of the backing plate. The study delivers validated predictive equations and detailed process maps to guide industrial practitioners in optimizing Friction Stir Welding (FSW) parameters for AA6061-T6, ultimately enabling the tailored achievement of superior mechanical properties and weld integrity.
Highlights
• This study systematically compares the mechanical performance and process response of Conventional FSW and Bobbin Tool FSW configurations for AA6061-T6 aluminum alloy, using identical experimental protocols and advanced statistical modeling.
• Regression models validated by ANOVA and diagnostic plots (R² > 0.99) accurately predict ultimate tensile strength and hardness based on key process variables, providing a reliable framework for process optimization.
• Results reveal that BTFSW offers superior hardness, process flexibility, and defect mitigation over CFSW, while both methods achieve comparable peak tensile strengths when optimally configured.
• Optimized process maps and validated models are provided as practical tools for industry practitioners to achieve tailored mechanical properties and high-quality welds in AA6061-T6, supporting flexible implementation in advanced manufacturing.
Introduction
Friction stir welding (FSW) is a solid-state, tool-driven joining process that produces defect-free, fine-grained welds in aluminum and other lightweight alloys by severe plastic deformation and frictional heating, remaining below the base metal's melting temperature [58]. Its solid-state mechanism yields joints with slight distortion and enhanced fatigue and corrosion resistance compared with several fusion techniques, facilitating swift adoption in the aerospace, automotive, rail, and marine industries [2, 29, 45, 59].
Two principal variants of the process are now generally reported. Conventional friction stir welding (CFSW) utilizes a singular rotating shoulder and pin often necessitating backing support to prevent root defects; it is the prevailing industry standard for welding sheets and plates. In contrast, bobbin-tool friction stir welding (BTFSW) employs a twin shoulder configuration that moves along the joint without a backing plate, facilitating symmetric through-thickness heat input, eradicating root defects, and minimizing machine fixturing needs. Recent experimental investigations outline the comparative advantages and practical constraints of BTFSW, encompassing heightened tool complexity, cooling requirements, and tool longevity considerations [7, 11, 34, 51].
The mechanical outcomes such as ultimate tensile strength (UTS), yield strength (YS), hardness distribution, and fatigue life for both CFSW and BTFSW largely depend on interacting parameters including tool rotational speed, traverse speed, tool geometry, plunge depth and tilt angle [10, 12, 14, 22, 41, 49, 53]. Recently, a marked growth in investigations employing Design of Experiments (DOE) and Response Surface Methodology (RSM) to model, quantify, and optimize process–response relationships [1, 6, 33, 60, 62]. These studies range from single-response RSM models and Taguchi-based screening designs to multi-response RSM, Grey Relational Analysis, developing a fuzzy logic to optimize the FSW process parameters, and hybrid approaches that incorporate metaheuristic optimizers or machine learning surrogates to solve multi-objective trade-offs between strength, ductility, and microhardness [9, 15, 20, 23, 24, 28, 31, 35, 37, 40, 41, 43, 44, 50, 52, 61].
Despite this increase of use of the DOE and RSM studies for CFSW in studies conducted by [18, 19, 21], and an growing body of BTFSW optimization work (including bobbin-tool friction stir processing/welding studies on Aluminum alloy (AA-series alloys), comparatively few investigations have implemented equivalent DOE/RSM experimental frameworks that directly benchmark CFSW and BTFSW under matched conditions. The comparative literature that does exist remains limited to a small number of side-by-side experimental reports and very recent comprehensive evaluations [5, 8, 16, 25, 27, 30, 32, 47, 54]. Systematic multi-response RSM studies that explicitly contrast process sensitivity, robustness, and Pareto-optimal parameter regions for both tool concepts remain uncommon, limiting generalizable conclusions about when BTFSW provides statistically significant improvements in joint performance and process stability over conventional configurations [8, 38, 41, 55, 57]. In line with the studies summarized in the Table 1, this research presents a comprehensive comparative investigation of the CFSW and BTFSW process for the AA6061-T6 alloy with a plate thickness of 6 mm.
Table 1. Summary for current research in FSW
# | Citation (short) | Alloy/TH | Tool type | UTS/joint efficiency | Hardness (HV) |
|---|---|---|---|---|---|
1 | [3] | AA6061-T6/2 mm and 1.2 mm | Hemispherical tool | 70% of BM (lap-shear tests) | Not reported |
2 | [39] | Dissimilar butt joints between AA6061-T6 and SS316 | Conventional FSW tool | 162 MPa | Not reported |
3 | [50] | AA6061-T6 Extruded Alloy/TH 8 mm | Bobbin tool | 74% of BM | Not reported |
4 | [48] | AA6061-T6 SiC composite lap joint TH 2 mm | Conventional FSW tool | 137 MPa (lap-shear tests) | 92 HV at stir zone |
5 | [46] | AA6061-T6/TH 2.5 mm | Conventional FSW | 235 MPA/82% of BM | 83 HV at nugget zone |
6 | [10, 12] | AA6082-T6/TH 6 mm | Eccentric tool FSW | 217 MPa/89.7% of BM | Highest value 82HV |
7 | [19] | AA6061/TH 4 mm | Conventional FSW tool | 158 MPa/77% of BM | Highest value 90HV |
8 | [17] | AA7020/TH 4 mm | Conventional FSW tool | 308.5 MPa | Not reported |
9 | [40] | AA7020/TH 4 mm | Conventional FSW tool | 273 MPa/68.25% of BM | Not reported |
10 | [42] | AA7020/TH 4 mm | Conventional FSW tool | 262 Mpa | 116.3 HV |
Collectively, the existing literature highlights a clear research gap. Although DOE and RSM have matured into robust frameworks for parameter selection and optimization in friction stir welding, their application remains largely fragmented. In particular, there is a pressing need for a unified, data-driven optimization strategy that ensures consistency across different aluminum alloys and tool configurations. Only a limited number of studies have employed DOE and RSM within a common experimental and analytical framework for the FSW process, and even fewer have done so in a way that enables systematic comparison between welding approaches.
This gap motivates the development of a comprehensive research methodology involving carefully structured comparative experiments that:
Apply an identical DOE/RSM framework to both CFSW and BTFSW.
Evaluate multiple mechanical performance responses in parallel; and
Explicitly report statistical adequacy indicators including uncertainty, model fit, and predictive reliability so that decision-makers may objectively assess trade-offs based on industrial requirements.
Addressing this gap will yield more generalizable knowledge regarding tool selection, process design, and operating windows, ultimately guiding practitioners toward optimized and application-specific FSW solutions in high-performance manufacturing environments.
Methodology & procedure
This study examined the FSW of AA6061-T6 aluminum alloy utilizing both CFSW and BTFSW, ensuring methodological consistency for reliable evaluation of process parameters and mechanical performance. AA6061-T6 plates (120 mm × 100 mm × 6 mm) were prepared by methanol cleaning and drilling a plunge initiation hole. Welding fixtures were fabricated from carbon steel, with CFSW employing a backing plate and BTFSW a self-reacting fixture. Tools were Computer Numerical Control (CNC) machined from H13 tool steel whose chemical composition if shown in Table 2 and heat treated to (~ 61 HRC), with straight cylindrical (SC) and conical (C) pins for CFSW, and also straight cylindrical (SCB) and cylindrical threaded (CT) pins for BTFSW refer to Fig. 1 for tool samples. Welding was performed on a modified vertical CNC milling machine in position-control mode, involving tool plunge, dwell, traverse, and natural cooling. A factorial Response Surface Optimal (RSO) design captured linear, quadratic, and interaction effects of rotational speed, feed rate, tool profile, tilt angle and plunge depth for CFSW, and rotational speed, feed rate, tool profile and pinching gap for BTFSW. Parameters were selected from literature and preliminary trials to ensure defect-free joints. Welds were inspected visually before testing. Three tensile and micro-hardness specimens were extracted via wire-cut electric discharge machining (EDM), with tensile tests conducted to ASTM E8/E8M standards, Fig. 2 shows a sample of the tensile specimen highlighting the advancing and retreating sides. Vickers hardness measured across the stir zone and the average of the results is reported. All tests were performed at least four weeks after welding to allow microstructural stabilization.
Table 2. Chemical composition of H13 tool steel
Alloy | Cr (%) | Mo | Si | V | C | Ni | Cu | Mn | Fe |
|---|---|---|---|---|---|---|---|---|---|
H13 | 4.75–6 | 4.75–6 | 1.1–1.75 | 0.8–1.2 | 0.8–1.2 | 0.32–0.45 | 0.3 0.25 | 0.2–0.5 | Rest |
[See PDF for image]
Fig. 1
Sample for manufactured tools SC for CFSW left and SCB for BTFSW right
[See PDF for image]
Fig. 2
Sample of tensile test specimen cut perpendicular to the weld direction
Welding of aluminum alloy 6061-T6
Experimental design and model formulation
For both CFSW and BTFSW, the welding of AA6061-T6 was systematically studied using the experimental matrices provided for CFSW and BTFSW shown in.
Tables 3 and 4 respectively. The response variables measured included ultimate tensile strength and Vickers micro hardness. A regression-based approach was employed to develop mathematical models predicting UTS and HV as functions of the significant process parameters for each configuration and tool profile, supported by Design-Expert software at a 95% confidence level.
Table 3. Design matrix with response results for conventional FSW of AA6061 T6
Run | A | B | C | D | E | UTS | HV |
|---|---|---|---|---|---|---|---|
1 | 800 | 100 | 3 | 0.1 | SC | 167.84 | 94.31 |
2 | 1120 | 100 | 3 | 0.3 | SC | 228.66 | 87.58 |
3 | 800 | 50 | 0 | 0.25 | C | 165.85 | 58.76 |
4 | 800 | 50 | 1.5 | 0.1 | SC | 155.18 | 53.42 |
5 | 800 | 50 | 3 | 0.3 | C | 159.27 | 62.08 |
6 | 1000 | 63 | 0 | 0.1 | SC | 175.69 | 84.86 |
7 | 1120 | 63 | 3 | 0.25 | SC | 241.52 | 92.98 |
8 | 1120 | 100 | 3 | 0.1 | C | 216.29 | 91.25 |
9 | 1120 | 100 | 1.5 | 0.1 | SC | 235.67 | 91.21 |
10 | 1000 | 80 | 1.5 | 0.25 | SC | 190.32 | 94.36 |
11 | 1120 | 80 | 0 | 0.3 | C | 227.43 | 95.87 |
12 | 1300 | 100 | 0 | 0.1 | C | 232.81 | 89.79 |
13 | 800 | 100 | 1.5 | 0.25 | C | 148.25 | 97.43 |
14 | 1300 | 80 | 0 | 0.25 | SC | 236.97 | 92.61 |
15 | 1300 | 50 | 1.5 | 0.25 | C | 228.38 | 85.13 |
16 | 1300 | 50 | 0 | 0.3 | SC | 215.18 | 71.06 |
17 | 1000 | 80 | 1.5 | 0.25 | C | 192.65 | 97.26 |
18 | 1000 | 63 | 3 | 0.1 | C | 190.16 | 83.67 |
19 | 1000 | 50 | 3 | 0.25 | SC | 188.65 | 68.37 |
20 | 1300 | 50 | 0 | 0.1 | C | 210.27 | 69.42 |
21 | 1120 | 63 | 1.5 | 0.3 | C | 233.63 | 87.26 |
22 | 800 | 100 | 0 | 0.3 | SC | 144.58 | 96.09 |
23 | 1120 | 80 | 1.5 | 0.25 | SC | 220.97 | 95.75 |
24 | 1300 | 100 | 3 | 0.25 | C | 235.17 | 92.31 |
25 | 800 | 63 | 1.5 | 0.3 | SC | 157.84 | 75.83 |
26 | 800 | 80 | 0 | 0.1 | C | 159.82 | 91.08 |
Table 4. Design matrix with response results for bobbin FSW of AA6061 T6
Run | A | B | C | D | UTS | HV |
|---|---|---|---|---|---|---|
1 | 800 | 80 | 5.8 | SC | 236.94 | 95.71 |
2 | 400 | 50 | 6 | CT | 188.72 | 93.38 |
3 | 600 | 100 | 5.8 | SC | 212.88 | 95.26 |
4 | 600 | 150 | 5.8 | CT | 208.75 | 95.93 |
5 | 1120 | 150 | 5.8 | SC | 230.66 | 97.56 |
6 | 400 | 50 | 5.6 | SC | 195.16 | 92.94 |
7 | 600 | 150 | 5.6 | SC | 206.15 | 92.34 |
8 | 800 | 63 | 5.6 | CT | 232.85 | 101.26 |
9 | 960 | 100 | 6 | CT | 231.36 | 93.83 |
10 | 960 | 50 | 6 | SC | 225.28 | 94.75 |
11 | 1120 | 80 | 5.6 | SC | 217.67 | 97.98 |
12 | 1120 | 150 | 6 | CT | 218.02 | 97.57 |
13 | 1120 | 50 | 5.8 | CT | 212.26 | 95.36 |
14 | 800 | 50 | 5.8 | SC | 232.78 | 94.49 |
15 | 800 | 100 | 5.8 | SC | 234.62 | 94.97 |
16 | 400 | 100 | 5.6 | CT | 199.99 | 95.35 |
17 | 800 | 150 | 6 | SC | 235.6 | 94.65 |
For the CFSW the UTS and HV regression equations shown in Eq. 1 and Eq. 2 respectively, were modeled as functions of five key process parameters: rotational speed (A), feed rate (B), tool tilt angle (C), plunge depth (D), and tool pin profile (E)
1
2
While for the BTFSW the UTS and HV regression equations shown in Eq. 3 and Eq. 4 respectively, are functions of rotational speed (A), feed rate (B), Pinching gap (C), and tool pin profile (D).
3
4
Model adequacy and validation
The Analysis of variance (ANOVA) results provided in Tables 5 through 8, show robust statistical validation for the regression models in both welding configurations, with model F-values well above the threshold for significance and p-values for the models less than 0.01, indicating less than a 1% chance that the observed variance is due to random error.
Table 5. CFSW ANOVA table for ultimate tensile strength
Source | Sum of squares | df | Mean square | F-value | p-value |
|---|---|---|---|---|---|
Model | 26909.55 | 19 | 1416.29 | 37.34 | 0.0001 |
A-Speed | 8752.18 | 1 | 8752.18 | 230.76 | < 0.0001 |
B-Feed | 65.24 | 1 | 65.24 | 1.72 | 0.2376 |
C-Angle | 759.91 | 1 | 759.91 | 20.04 | 0.0042 |
D-Depth | 2.52 | 1 | 2.52 | 0.0664 | 0.8052 |
E-Tool | 307.46 | 1 | 307.46 | 8.11 | 0.0293 |
AB | 113.15 | 1 | 113.15 | 2.98 | 0.1349 |
AC | 551.64 | 1 | 551.64 | 14.54 | 0.0088 |
AD | 118.26 | 1 | 118.26 | 3.12 | 0.1279 |
AE | 462.42 | 1 | 462.42 | 12.19 | 0.0130 |
BC | 113.76 | 1 | 113.76 | 3.00 | 0.1340 |
BD | 26.42 | 1 | 26.42 | 0.6966 | 0.4359 |
BE | 22.46 | 1 | 22.46 | 0.5923 | 0.4707 |
CD | 397.48 | 1 | 397.48 | 10.48 | 0.0177 |
CE | 1223.29 | 1 | 1223.29 | 32.25 | 0.0013 |
DE | 475.38 | 1 | 475.38 | 12.53 | 0.0122 |
A2 | 67.52 | 1 | 67.52 | 1.78 | 0.2305 |
B2 | 430.48 | 1 | 430.48 | 11.35 | 0.0151 |
C2 | 47.50 | 1 | 47.50 | 1.25 | 0.3059 |
D2 | 476.43 | 1 | 476.43 | 12.56 | 0.0122 |
Std. Dev | 6.16 | R2 | 0.9916 | ||
Mean | 198.43 | Adjusted R2 | 0.9651 | ||
C.V. % | 3.10 | Predicted R2 | 0.7916 | ||
Adeq Precision | 18.1097 |
For CFSW (Tables 5 & 6), UTS was primarily governed by rotational speed (A), tilt angle (C), and tool profile (E), with significant interactions (AC, AE, CE) and quadratic effects (B2, D2) confirming the need for balanced parameter selection. For hardness, feed rate (B) was dominant, followed by rotational speed (A) and interactions (AB, BC), while the quadratic term (B2) emphasized the non-linear dependence on feed rate.
Table 6. CFSW ANOVA table for hardness
Source | Sum of squares | df | Mean square | F-value | p-value |
|---|---|---|---|---|---|
Model | 4086.06 | 19 | 215.06 | 35.00 | 0.0001 |
A-Speed | 38.99 | 1 | 38.99 | 6.35 | 0.0453 |
B-Feed | 1819.71 | 1 | 1819.71 | 296.16 | < 0.0001 |
C-Angle | 5.82 | 1 | 5.82 | 0.9466 | 0.3682 |
D-Depth | 0.1043 | 1 | 0.1043 | 0.0170 | 0.9006 |
E-Tool | 6.12 | 1 | 6.12 | 0.9964 | 0.3567 |
AB | 446.53 | 1 | 446.53 | 72.67 | 0.0001 |
AC | 22.12 | 1 | 22.12 | 3.60 | 0.1065 |
AD | 0.5076 | 1 | 0.5076 | 0.0826 | 0.7835 |
AE | 5.72 | 1 | 5.72 | 0.9309 | 0.3719 |
BC | 40.96 | 1 | 40.96 | 6.67 | 0.0417 |
BD | 32.59 | 1 | 32.59 | 5.30 | 0.0608 |
BE | 0.2895 | 1 | 0.2895 | 0.0471 | 0.8354 |
CD | 5.80 | 1 | 5.80 | 0.9445 | 0.3686 |
CE | 4.94 | 1 | 4.94 | 0.8045 | 0.4043 |
DE | 18.10 | 1 | 18.10 | 2.95 | 0.1369 |
A2 | 1.88 | 1 | 1.88 | 0.3052 | 0.6006 |
B2 | 301.01 | 1 | 301.01 | 48.99 | 0.0004 |
C2 | 10.83 | 1 | 10.83 | 1.76 | 0.2327 |
D2 | 18.32 | 1 | 18.32 | 2.98 | 0.1350 |
Std. Dev | 2.48 | R2 | 0.9911 | ||
Mean | 84.35 | Adjusted R2 | 0.9627 | ||
C.V. % | 2.94 | Predicted R2 | 0.8198 | ||
Adeq Precision | 20.2651 |
For BTFSW (Tables 7 & 8), UTS was strongly influenced by rotational speed (A) and feed rate (B), with key interactions (AC, AD, BC) and quadratic terms (A2, C2) shaping the response surface. Hardness was affected by all main factors (A, B, C, D), with significant interactions (AB, AC, BD) and quadratic contributions (B2, C2), highlighting the necessity of precise parameter tuning.
Table 7. BTFSW ANOVA table for ultimate tensile strength
Source | Sum of squares | df | Mean square | F-value | p-value |
|---|---|---|---|---|---|
Model | 3744.77 | 13 | 288.06 | 104.73 | 0.0013 |
A-Speed | 1105.29 | 1 | 1105.29 | 401.84 | 0.0003 |
B-Feed | 130.49 | 1 | 130.49 | 47.44 | 0.0063 |
C-Gap | 6.61 | 1 | 6.61 | 2.40 | 0.2189 |
D-Pin | 2.49 | 1 | 2.49 | 0.9070 | 0.4112 |
AB | 11.46 | 1 | 11.46 | 4.17 | 0.1338 |
AC | 136.18 | 1 | 136.18 | 49.51 | 0.0059 |
AD | 144.10 | 1 | 144.10 | 52.39 | 0.0054 |
BC | 113.74 | 1 | 113.74 | 41.35 | 0.0076 |
BD | 108.61 | 1 | 108.61 | 39.49 | 0.0081 |
CD | 30.42 | 1 | 30.42 | 11.06 | 0.0449 |
A2 | 956.65 | 1 | 956.65 | 347.80 | 0.0003 |
B2 | 7.07 | 1 | 7.07 | 2.57 | 0.2073 |
C2 | 61.54 | 1 | 61.54 | 22.37 | 0.0179 |
Std. Dev | 1.66 | R2 | 0.9978 | ||
Mean | 218.81 | Adjusted R2 | 0.9883 | ||
Adeq Precision | 31.2094 | Predicted R2 | 0.8776 |
Table 8. BTFSW ANOVA table for hardness
Source | Sum of squares | df | Mean square | F-value | p-value |
|---|---|---|---|---|---|
Model | 74.14 | 13 | 5.70 | 38.16 | 0.0060 |
A-Speed | 26.73 | 1 | 26.73 | 178.83 | 0.0009 |
B-Feed | 4.54 | 1 | 4.54 | 30.35 | 0.0118 |
C-Gap | 22.43 | 1 | 22.43 | 150.04 | 0.0012 |
D-Pin | 12.82 | 1 | 12.82 | 85.76 | 0.0027 |
AB | 15.42 | 1 | 15.42 | 103.13 | 0.0020 |
AC | 11.53 | 1 | 11.53 | 77.14 | 0.0031 |
AD | 4.55 | 1 | 4.55 | 30.42 | 0.0117 |
BC | 2.67 | 1 | 2.67 | 17.86 | 0.0242 |
BD | 8.53 | 1 | 8.53 | 57.07 | 0.0048 |
CD | 14.13 | 1 | 14.13 | 94.50 | 0.0023 |
A2 | 0.0035 | 1 | 0.0035 | 0.0234 | 0.8881 |
B2 | 1.71 | 1 | 1.71 | 11.47 | 0.0429 |
C2 | 3.27 | 1 | 3.27 | 21.87 | 0.0185 |
Std. Dev | 0.3866 | R2 | 0.9940 | ||
Mean | 95.49 | Adjusted R2 | 0.9679 | ||
Adeq Precision | 25.2306 | Predicted R2 | 0.9138 |
For both CFSW and BTFSW, the regression models exhibited high R2 values (0.991–0.9978), indicating that the models captured over 99% of the variability in the data. Adjusted and predicted R2 values were closely aligned, and adequate precision values far exceeded the minimum desirable value of 4, signifying strong signal-to-noise ratios and confirming model reliability for process optimization.
Response surface analysis and optimization
RSM was employed to visualize the combined effects and interactions of process parameters on UTS and HV. Figures 3 and 4 represent the response surfaces for UTS and HV of the CFSW technique, respectively, while Figs. 5 and 6 represent the response surfaces for UTS and HV of the BTFSW technique, respectively.
[See PDF for image]
Fig. 3
CFSW Response surface plots for UTS against (a)BA (b)CA (c)DA (d)DC
[See PDF for image]
Fig. 4
CFSW Response surface plots for HV against (a)BA (b)CB (c)DB (d)CD
[See PDF for image]
Fig. 5
BTFSW Response surface plots for UTS against (a)BA (b)CA (c)CB
[See PDF for image]
Fig. 6
BTFSW Response surface plots for HV against (a)BA (b)CA (c)CB
CFSW response surfaces
UTS
Three-dimensional plots revealed that UTS was maximized at high rotational speeds and tilt angles, with the strongest improvement due to their synergistic effect. The surfaces also showed that, while feed rate had some effect, its impact was less pronounced compared to rotational speed and tilt angle. Plunge depth interacted with rotational speed, where excessive plunge could diminish UTS, likely due to over-stirring or excessive downward force causing defects.
HV
The optimal hardness was achieved at high feed rates combined with lower rotational speeds. This condition likely fosters finer grain structures due to shorter thermal cycles and less grain growth, as excessive heat at high rotational speeds can coarsen microstructures and reduce hardness. Tilt angle and plunge depth had relatively minor effects on HV, with surfaces appearing relatively flat along those axes, suggesting secondary importance.
BTFSW response surfaces
UTS
The response surfaces showed a parabolic relationship between UTS and both rotational speed and pinching gap, with distinct optima for each. UTS initially increased with rotational speed and pinching gap but declined past their optimal values, reflecting the need to balance heat input and mechanical constraint. The interaction between feed rate and pinching gap indicated that lower values of both parameters yielded higher UTS, likely due to improved material flow and consolidation.
HV
For hardness, response surfaces demonstrated that maximum HV was obtained at high feed rates and high rotational speeds, especially when combined with minimal pinching gaps and threaded tool profiles. The threaded profile intensified the stirring action and promoted dynamic recrystallization, yielding finer microstructures and higher HV values.
Optimal FSW parameters and validation tests
To evaluate the validity of the developed regression models, three confirmation experiments were performed using input values within the studied range but distinct from those in the original design matrix for both CFSW and BTFSW. The corresponding experimental and predicted responses are presented in Tables 9 and 10. The observed deviations between the measured and predicted values remained within the 95% confidence interval, thereby confirming the adequacy and predictive capability of the regression models.
Table 9. Confirmation test parameters and results for CFSW of AA6061-T6
Experiment | A | B | C | D | E | ||
1 | 800 | 63 | 3 | 0.1 | SC | ||
2 | 1000 | 100 | 3 | 0.1 | SC | ||
3 | 1120 | 50 | 1.5 | 0.25 | C | ||
Experiment | Out Response | First Reading | Second Reading | Third Reading | Average | Predicted | % Error |
1 | UTS | 190.25 | 192.73 | 188.14 | 190.37 | 182.936 | 4.06 |
Hardness | 78.97 | 78.62 | 76.58 | 78.05 | 74.55 | 4.69 | |
2 | UTS | 220.14 | 221.63 | 225.36 | 222.37 | 228.1 | 2.51 |
Hardness | 95.47 | 96.59 | 93.21 | 95.09 | 92.94 | 2.31 | |
3 | UTS | 203.85 | 203.56 | 201.39 | 202.93 | 196.74 | 3.14 |
Hardness | 73.25 | 72.69 | 73.57 | 73.17 | 75.23 | 2.73 | |
Table 10. Confirmation test parameters and results for BTFSW of AA6061-T6
Experiment | A | B | C | D | |||
1 | 960 | 50 | 6 | CT | |||
2 | 400 | 63 | 5.8 | SC | |||
3 | 600 | 50 | 5.8 | CT | |||
Experiment | Out Response | First Reading | Second Reading | Third Reading | Average | Predicted | % Error |
1 | UTS | 225.29 | 222.57 | 225.38 | 224.41 | 231.59 | 3.1 |
Hardness | 92.61 | 88.25 | 91.59 | 90.81 | 89.78 | 1.14 | |
2 | UTS | 180.98 | 181.37 | 178.15 | 180.16 | 174.96 | 2.97 |
Hardness | 94.68 | 94.84 | 95.36 | 94.96 | 97.24 | 2.34 | |
3 | UTS | 226.9 | 226.35 | 225.11 | 226.12 | 234.72 | 3.66 |
Hardness | 88.99 | 89.01 | 89.36 | 89.12 | 93.26 | 4.43 | |
Discussion
The statistical and response surface results were consistent with the underlying physical principles of FSW. Increased rotational speed enhanced frictional heat generation, promoting plasticization and material flow, whereas excessively high speeds risked overheating, grain coarsening, and accelerated tool wear. In CFSW, the tool tilt angle facilitated downward forging and improved material mixing, while in BTFSW the pinching gap primarily influenced vertical constraint and heat dissipation. Variations in tool pin profile further governed stirring efficiency, with threaded and conical designs providing superior grain refinement compared to straight cylindrical geometries.
Cross-comparative summary
A comprehensive cross-comparison of CFSW and BTFSW reveals nuanced similarities and differences in parameter sensitivity, process robustness, and achievable mechanical properties. The statistical analyses (ANOVA and regression modeling) and response surface methodologies provide a strong foundation for this comparative assessment.
Influence of key process parameters
Rotational speed
Both CFSW and BTFSW demonstrate a dominant sensitivity of UTS to rotational speed, as substantiated by the high F-values and extremely low p-values (CFSW: p < 0.0001, BTFSW: p = 0.0003). In both cases, UTS increases with speed up to an optimal point, beyond which overheating or material degradation can occur which align with the findings of [7, 8, 19]. However, response surfaces in BTFSW showed a more pronounced parabolic effect, indicating that excessive rotational speed leads to a sharper decline in UTS compared to CFSW, likely due to BTFSW’s higher thermal efficiency and more symmetric heat input.
Feed rate/traverse speed
For CFSW, feed rate was not a significant main effect for UTS (p = 0.2376), but was extremely significant for hardness (HV, p < 0.0001) as concluded by the work of [4, 13], with both linear and quadratic effects. In contrast, in BTFSW, feed rate was significant for both UTS (p = 0.0063) and HV (p = 0.0118), with strong interaction effects (AB, BC, BD for HV). This suggests BTFSW is more sensitive to variations in feed rate across all mechanical properties, possibly due to the combined effect of enhanced stirring and through-thickness constraint.
Tool geometry (Pin Profile)
In both methods, pin profile was statistically significant (CFSW UTS: p = 0.0293; BTFSW HV: p = 0.0027) aligning with the work of [16], but the effect was more pronounced and consistently beneficial in BTFSW, where threaded/conical pins delivered superior HV and improved UTS through intensified stirring and dynamic recrystallization. Response surfaces for BTFSW showed that threaded profiles consistently produced higher and more uniform hardness values compared to the straight cylindrical counterpart. In CFSW, the pin profile effect was significant but less pronounced, often modulated by interactions with rotational speed and tilt angle.
Tilt angle (CFSW) vs. pinching gap (BTFSW)
Tilt angle in CFSW had a strong primary (p = 0.0042) and synergistic effect (AC, CE), enhancing UTS by promoting forging action and material flow as mentioned by [36]. In BTFSW, the pinching gap exerted quadratic and interaction effects (C2, AC, BC), with an optimal range enhancing both strength and hardness, but too wide a gap reducing mechanical constraint and weld quality. CFSW’s tilt angle effect manifests more as a “shaping” parameter, while BTFSW’s gap acts as a “confinement” control.
Robustness and predictive accuracy
Model adequacy
Both methods yielded highly robust regression models (CFSW: R2 = 0.9916 for UTS, 0.9911 for HV; BTFSW: R2 = 0.9978 for UTS, 0.9940 for HV). The close agreement between adjusted and predicted R2, and the high adequate precision values for both processes, indicate that the predictive models are both accurate and reliable across broad parameter windows.
3. Response surface topography and process optimization
UTS surfaces
CFSW UTS surfaces were characterized by clear ridges along the axes of rotational speed and tilt angle, with minor curvature in the feed rate direction. BTFSW UTS surfaces, however, exhibited more pronounced peaks and valleys, particularly along the rotational speed and gap axes, indicating a narrower optimal process window and heightened risk of strength loss outside these bounds.
HV surfaces
In CFSW, the highest HV was achieved at high feed rates and lower rotational speeds, with minimal effect from tilt angle or plunge depth. In BTFSW, hardness optimization was more complex, depending strongly on high feed rates, high rotational speeds, minimal pinching gap, and the use of threaded pins. The surfaces were steeper, suggesting BTFSW is more sensitive to parameter variations in hardness optimization.
Practical and process design implications
BT-FSW, by design, eliminates the need for a backing plate, enhances vertical constraint, and reduces the risk of root defects, offering advantages for complex geometries and variable-thickness applications [26, 56]. This was confirmed experimentally by the absence of root flaws and improved process stability. CFSW is preferable when maximum UTS is the priority, achieving optimal results with a high rotational speed, appropriate tilt angle, and a straight cylindrical tool. BT-FSW, in contrast, is ideal for applications requiring high surface hardness and defect-free welds, particularly with a threaded tool, high rotational and traverse speeds, and minimal pinching gap. The observed differences in hardness and UTS between CFSW and BT-FSW joints are explained by fundamental strengthening mechanisms: grain refinement in the stir zone impedes dislocation motion (Hall–Petch effect), fine precipitates enhance resistance to plastic flow, and elevated dislocation density and residual stresses from severe plastic deformation influence overall mechanical behavior. In BT-FSW, the higher hardness despite comparable UTS is attributed to more uniform grain refinement and dislocation distribution due to symmetric material flow and confinement in the pinching-gap configuration.
Practical implications and recommendations
The comparative analysis demonstrates that both CFSW and BTFSW are effective for welding AA6061-T6, with BTFSW offering additional process flexibility and higher achievable hardness. The process maps generated can serve as practical guidelines for industrial optimization, with the choice of configuration and parameters depending on the specific performance criteria (strength vs. hardness) and geometric constraints of the application.
Future work should focus on microstructural analysis, fatigue testing, and scaling studies to further elucidate the mechanisms underlying the observed trends, and on refining parameter windows for industrial-scale implementation.
Conclusion
This study provides a comprehensive experimental and modeling framework for friction stir welding of AA6061-T6 using both conventional and bobbin tool approaches. The statistical and comparative analysis not only elucidates the dominant process variables and their interactions but also offers validated predictive models and practical guidelines for process optimization, facilitating improved mechanical performance in industrial applications.
Both CFSW and BTFSW achieved high UTS values in AA6061-T6 welds, with CFSW reaching a maximum of 241.5 MPa and BTFSW achieving up to 236.9 MPa. The results indicate that, when optimally configured, both techniques can produce joints with excellent load-bearing capacity and joint efficiencies above 90%.
BTFSW consistently delivered higher micro-hardness in the weld zone compared to CFSW, attaining peak values up to 101.3 HV versus CFSW’s maximum of 97.3 HV. This increase is attributed to the improved stirring action and more uniform heat distribution provided by the bobbin tool configuration.
BTFSW generally produced narrower mechanical property ranges (higher minimum UTS and HV) compared to CFSW, indicating improved consistency and reduced incidence of severely underperforming joints.
Three confirmation tests were conducted to confirm the predictability of the developed models for CFSW and BTFSW.
ANOVA and response surface methodology identified rotational speed and tool profile as the most influential factors for UTS, while feed rate and pin geometry had the greatest impact on HV. Significant interaction and quadratic effects were observed, confirming that optimal weld quality requires the simultaneous tuning of multiple process variables.
The regression models developed for both UTS and HV in CFSW and BTFSW demonstrated outstanding statistical adequacy (R2 > 0.99). Diagnostic plots validated the models’ reliability, with residuals showing random distributions and no significant outliers or leverage points, ensuring strong predictive and optimization capabilities.
BTFSW not only matched CFSW in joint strength but also surpassed it in micro-hardness and defect mitigation, making it the preferred choice for applications demanding superior wear resistance and weld integrity. However, both processes yielded excellent results when process parameters were systematically optimized according to the established models.
BTFSW can achieve excellent mechanical performance in AA6061-T6, but requires more precise parameter optimization due to its heightened process sensitivity.
Significant interaction terms underscore that optimal mechanical properties cannot be achieved by varying a single parameter in isolation; rather, simultaneous optimization of multiple variables guided by response surface maps and validated regression models is essential.
Acknowledgements
The authors gratefully acknowledge the support provided by the German University in Cairo.
Authors’ contributions
George G. Yacout: Research and investigation. A.Y.Shash: Conceptualization of the study and Methodology. Hesham A. Hegazi: Methodology. Mahmoud G. ElSherbiny: Methodology and supervision.
Funding
Not Applicable.
Data availability
The data supporting these findings are included in this article, and further details can be obtained from the corresponding author upon reasonable request.
Declarations
Competing interests
The authors declare no competing interests.
Abbreviations
Friction stir welding
Conventional friction stir welding
Bobbin tool friction stir welding
Ultimate tensile strength
Yield strength
Design of experiments
Response surface methodology
Aluminum alloy
Computer Numerical Control
Response surface optimal
Electric discharge machine
Hardness Vickers
Analysis of variance
Publisher’s Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
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