D.H. Lammlein PhD Dissertation - Vanderbilt University

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Figure 133: (conical tool) Lateral contours of velocity magnitude (m/s) showing the thermo-mechanical affected zone (TMAZ). Figure 134: (conical tool) Lateral macrosection corresponding (1000rpm, 7.8ipm) to the CFD simulated weld showing the TMAZ(bright), parent metal(dark), and transitional HAZ (intermediate). Figure 132 and Figure 133 show the HAZ and TMAZ respectively forming transposed bowl shaped regions around the weld tool in the experimental model and this shape is verified in the macrosection. Conclusions 146
The results presented here show that aluminum alloy hemispheres can be reliably joined by FSW. Additionally, the control techniques used in this experiment show that system eccentricities can be accounted for via multiple methods. The relative height of the material surface can be taken at various points around the circumference of the sphere and a preplanned path can be taken by the tool to maintain the appropriate penetration depth. The unique geometry of the conical tool can be used advantageously in torque based feedback control of weld penetration depth, as measured weld toque proved to be a strong and reliable indicator of weld depth. Additionally, it was shown that for cases where the interior of the vessel is inaccessible and internal support is not possible, partial penetration welds of similar proportional strength can be achieved without compromising the material interior surface. A lack of material distortion at the joint base is required for external compression applications. The conical tool produced, 50% penetration welds in an unsupported configuration which ranged from 20-26% parent material strength in a practical comparison using their apparent stress. The cupped shoulder tool produced full penetration welds with interior support which ranged from 54-68% of the parent material strength comparing apparent stress. The maximum strength could be improved by testing a wider range of parameters, as welds made with both setups were stronger at higher travel and rotational settings. Additionally, a penetration ligament of 0.014” was used in the full-penetration portion of the experiment. A more aggressive penetration ligament (i.e. one closer to 0.006”) would likely increase weld strength by eliminating any joint remnant at the weld root. Partial penetration welds continued to increase in strength with depth outside the matrix depth of 0.10”, however with the introduction of some distortion at the weld root. In this experiment it was assumed that this distortion was unacceptable and the experiment was done at a depth where no distortion occurred. Future work could explore the depth to which this relationship continues to hold should a suitable application be identified. Additionally, modifications to the tooling used in the experiment would likely result in strength increases as only a single tool geometry was considered for each case. A more complicated probe geometry and scrolled shoulder design could improve test strengths for the supported welds. Adjustments to the inclusive angle of the conical tool 147
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FRICTION STIR WELDING OF SPHERES, C
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TABLE OF CONTENTS TABLE OF FIGURES
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Appendix ..........................
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Figure 16: Left(FE streamline), Mid
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Figure 51: A thermal camera image t
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for a similar conventional weld (3/
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Figure 102: Tapered retraction proc
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setting are indicated. Note that st
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Unsupported welds of this kind with
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Figure 157: A thermal camera image
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ottom sample is a tungsten inert ga
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N - newton (force unit) n - visco-p
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INTRODUCTION Friction Stir Welding,
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educed conduction lengths. In small
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CHAPTER I LITERATURE REVIEW: COMPUT
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frictional condition at the interfa
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contact. The contact area can inclu
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For horizontal sections, a heat inp
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(1.11) where r p is the probe (pin)
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This efficiency term, η pd , is kn
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The heat input on the tool surface
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The added complication of these met
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Figure 5: Lateral cross sections of
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Flow stress in aluminum alloys is d
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Figure 8: Three flow fields a) rota
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and post-weld cool-down. This model
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Williams et al. [60] use a 2D-axisy
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Figure 16: Left(FE streamline), Mid
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Figure 18: Temperature contour over
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Figure 22: Temperature distribution
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Figure 24: Lateral velocity contour
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Figure 26: Experimental(white) vers
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Figure 28: Top view schematic of tu
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[5] Taylor RE, Groot H, Goerz T, Fe
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[41] Heinz B., Skrotzki B., Eggler
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CHAPTER II COMPUTATIONAL ANALYSIS O
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Figure 30: Blind t-joint setup with
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Figure 33: Process forces and later
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Figure 35: Experimental Welds, Axia
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Figure 37: FEA boundary conditions
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A 4500 N axial force is applied eve
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axial force with lateral offset dur
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Figure 42: Contour plot of von Mise
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Figure 44: Deformation contour for
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Figure 46: Quarter-plate model for
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Figure 49: Contour plot of deflecti
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where P is the weld power (W), Q is
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Figure 52: Fluent CFD model zones.
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Figure 55: Thermal contour of weld
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Figure 59: Thermal contour of weld
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Figure 61: Velocity vectors for 0.0
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Figure 65: Contour of velocity magn
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CHAPTER III THE APPLICATION OF SHOU
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Figure 66: A shoulder-less, conical
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Figure 68: Typical axial(Z-axis) fo
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Figure 71: 90° conical tool macros
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Figure 75: Run 3, 80° conical tool
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Figure 79: (90º tool) Ultimate ten
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Figure 83: (90º tool) Lateral forc
Page 119 and 120: Figure 87: (80º tool) Lateral forc
Page 121 and 122: The Eulerian, finite volume, CFD so
Page 123 and 124: Figure 92 shows the increasing elem
Page 125 and 126: Figure 91: CFD model geometry consi
Page 127 and 128: Figure 95: Lateral cross-section of
Page 129 and 130: Figure 96: Attempts a probe tapered
Page 131 and 132: CHAPTER IV THE FRICTION STIR WELDIN
Page 133 and 134: applications for its high strength
Page 135 and 136: Figure 97: Experimental weld sample
Page 137 and 138: Figure 99: Split protrusion type de
Page 139 and 140: with a cupped recess. It is however
Page 141 and 142: of tapered retraction (i.e. move th
Page 143 and 144: The adjustments in vertical positio
Page 145 and 146: manners the assigned depth was main
Page 147 and 148: Figure 108: Lateral macrosections f
Page 149 and 150: Figure 110: (Supported, cupped tool
Page 155 and 156: apparent strength of 26% parent whi
Page 157 and 158: with a 100º conical tool (0.025”
Page 159 and 160: Figure 119: Macrosection view of an
Page 161 and 162: and tooling. Torque is highly depen
Page 163 and 164: locally in proportion to the local
Page 165 and 166: Figure 126: (threaded tool) Contour
Page 167 and 168: Figure 128: (conical tool) Geometry
Page 169: Figure 131: (threaded tool) Lateral
Page 173 and 174: Figure 136:(from left: Tapered retr
Page 175 and 176: [8] Metallurgical analysis of ablat
Page 177 and 178: CHAPTER V FRICTION STIR WELDING OF
Page 179 and 180: Collaboration between Advanced Meta
Page 181 and 182: eccentricity, the method of interio
Page 183 and 184: gas tungsten arc welding of small d
Page 185 and 186: Full penetration welds of 4.2” (1
Page 187 and 188: Figure 143: The curvature of the pi
Page 189 and 190: Figure 144: Experimental axial forc
Page 191 and 192: Together, a fine wall thickness tol
Page 193 and 194: Figure 147: Axial force history for
Page 195 and 196: The weld macrosections show complet
Page 197 and 198: Figure 154: Macrosections of welds
Page 199 and 200: Figure 157: A thermal camera image
Page 201 and 202: Figure 159: Average tool shank temp
Page 203 and 204: 471,146 faces. The meshes are fine
Page 205 and 206: Figure 162: A closeup view of mesh
Page 207 and 208: 4 2 3 4 5 16 " 1.745 2 0.24
Page 209 and 210: applied heat locally in proportion
Page 211 and 212: Figure 164: Modeled temperature con
Page 217 and 218: Figure 172: Model pathlines for the
Page 219 and 220: Figure 174: Model pathlines for the
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later speed setting, the tool welds
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Figure 178: Zoom view of a macro ta
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Figure 180: The superficial appeara
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Figure 182: The rotary welding appa
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Figure 185: A diagram illustrating
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CONCLUSION AND FUTURE WORK Conclusi
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new FSW process environment is reso
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D.H. Lammlein PhD Dissertation - Vanderbilt University

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