The effect of Aluminium on the deformation mechanisms in Titanium
The aim of this experiment is to study the effect of Aluminium (Al) on deformation mechanisms in Titanium (Ti) alloys with a particular emphasis on studying twinning. Titanium alloys are used by the aerospace industry due to their outstanding strength to weight ratio. In order to develop new high strength Ti alloys in the future, a much improved understanding of the effect of alloying elements on deformation mechanisms such as twinning is highly desirable. While Aluminium is often considered to reduce twining activity in Ti alloys, it is in fact relatively unclear if Al reduces either twin nucleation or twin growth or even both. The proposed in-situ loading experiments on ENGIN-X aim at determining twin evolution during loading and to shed light on the nucleation criteria and the role of Aluminium on twinning. The results will be interpreted using crystal plasticity modelling.
- 1210312
- 4x4x15
- Al
- Aluminium
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 1 e 0...
- CP Ti870_ND s 12 e ...
- CP Ti870_ND s 14 e ...
- CP Ti870_ND s 18 e ...
- CP Ti870_ND s 19 e ...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 2 e 0...
- CP Ti870_ND s 20 e ...
- CP Ti870_ND s 21 e ...
- CP Ti870_ND s 21 e ...
- CP Ti870_ND s 24 e ...
- CP Ti870_ND s 27 e ...
- CP Ti870_ND s 3 e 0...
- CP Ti870_ND s 32 e ...
- CP Ti870_ND s 37 e ...
- CP Ti870_ND s 44 e ...
- CP Ti870_ND s 5 e 0...
- CP Ti870_ND s 6 e 0...
- CP Ti870_ND s 9 e 0...
- CPTi750_RD s 111 e ...
- CPTi750_RD s 13 e 0...
- CPTi750_RD s 13 e 0...
- CPTi750_RD s 13 e 0...
- CPTi750_RD s 13 e 0...
- CPTi750_RD s 13 e 0...
- CPTi750_RD s 14 e 0...
- CPTi750_RD s 14 e 0...
- CPTi750_RD s 14 e 0...
- CPTi750_RD s 145 e ...
- CPTi750_RD s 15 e 0...
- CPTi750_RD s 15 e 0...
- CPTi750_RD s 16 e 0...
- CPTi750_RD s 16 e 0...
- CPTi750_RD s 160 e ...
- CPTi750_RD s 18 e 0...
- CPTi750_RD s 201 e ...
- CPTi750_RD s 216 e ...
- CPTi750_RD s 216 e ...
- CPTi750_RD s 218 e ...
- CPTi750_RD s 231 e ...
- CPTi750_RD s 248 e ...
- CPTi750_RD s 268 e ...
- CPTi750_RD s 296 e ...
- CPTi750_RD s 330 e ...
- CPTi750_RD s 343 e ...
- CPTi750_RD s 39 e 0...
- CPTi750_RD s 54 e 0...
- CPTi750_RD s 72 e 0...
- CPTi870_RD s 2 e 0 ...
- CPTi870_RD s 2 e 0 ...
- CPTi870_RD s 42 e 0...
- CPTi870_RD s 43 e 0...
- CPTi870_RD s 44 e 0...
- CPTi870_RD s 45 e 0...
- CPTi870_RD s 47 e 0...
- CPTi870_RD s 47 e 0...
- CPTi870_RD s 48 e 0...
- CPTi870_RD_b s 1 e ...
- CPTi870_RD_b s 1 e ...
- CPTi870_RD_b s 12 e...
- CPTi870_RD_b s 14 e...
- CPTi870_RD_b s 19 e...
- CPTi870_RD_b s 2 e ...
- CPTi870_RD_b s 22 e...
- CPTi870_RD_b s 27 e...
- CPTi870_RD_b s 30 e...
- CPTi870_RD_b s 36 e...
- CPTi870_RD_b s 4 e ...
- CPTi870_RD_b s 5 e ...
- CPTi870_RD_b s 6 e ...
- CPTi870_RD_b s 9 e ...
- CeO2
- Cousins
- ENGINX
- Fitzner
- Honniball
- Prakash
- Preuss
- Quinta da Fonseca
- The
- Thomas
- Ti
- Ti2Al_RD s 119 e 0 ...
- Ti2Al_RD s 12 e 0 0...
- Ti2Al_RD s 13 e 0 0...
- Ti2Al_RD s 13 e 0 0...
- Ti2Al_RD s 14 e 0 0...
- Ti2Al_RD s 14 e 0 0...
- Ti2Al_RD s 14 e 0 0...
- Ti2Al_RD s 14 e 0 0...
- Ti2Al_RD s 140 e 0 ...
- Ti2Al_RD s 15 e 0 0...
- Ti2Al_RD s 15 e 0 0...
- Ti2Al_RD s 15 e 0 0...
- Ti2Al_RD s 15 e 0 0...
- Ti2Al_RD s 16 e 0 0...
- Ti2Al_RD s 17 e 0 0...
- Ti2Al_RD s 195 e 0 ...
- Ti2Al_RD s 209 e 0 ...
- Ti2Al_RD s 249 e 0 ...
- Ti2Al_RD s 252 e 0 ...
- Ti2Al_RD s 282 e 0 ...
- Ti2Al_RD s 307 e 0 ...
- Ti2Al_RD s 309 e 0 ...
- Ti2Al_RD s 310 e 0 ...
- Ti2Al_RD s 342 e 0 ...
- Ti2Al_RD s 371 e 0 ...
- Ti2Al_RD s 416 e 0 ...
- Ti2Al_RD s 458 e 0 ...
- Ti2Al_RD s 513 e 0 ...
- Ti2Al_RD s 57 e 0 0...
- Ti2Al_RD s 68 e 0 0...
- Ti2Al_RD s 92 e 0 0...
- Ti4Al_ND s 114 e 0 ...
- Ti4Al_ND s 125 e 0 ...
- Ti4Al_ND s 15 e 0 0...
- Ti4Al_ND s 150 e 0 ...
- Ti4Al_ND s 191 e 0 ...
- Ti4Al_ND s 198 e 0 ...
- Ti4Al_ND s 225 e 0 ...
- Ti4Al_ND s 250 e 0 ...
- Ti4Al_ND s 260 e 0 ...
- Ti4Al_ND s 278 e 0 ...
- Ti4Al_ND s 285 e 0 ...
- Ti4Al_ND s 295 e 0 ...
- Ti4Al_ND s 308 e 0 ...
- Ti4Al_ND s 328 e 0 ...
- Ti4Al_ND s 359 e 0 ...
- Ti4Al_ND s 419 e 0 ...
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- Ti4Al_ND s 7 e 0 00...
- Ti4Al_ND s 7 e 0 00...
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- Ti4Al_ND s 8 e 0 00...
- Ti4Al_ND s 8 e 0 00...
- Ti4Al_ND s 8 e 0 00...
- Ti4Al_ND s 8 e 0 00...
- Ti4Al_RD s 100 e 0 ...
- Ti4Al_RD s 132 e 0 ...
- Ti4Al_RD s 145 e 0 ...
- Ti4Al_RD s 180 e 0 ...
- Ti4Al_RD s 196 e 0 ...
- Ti4Al_RD s 210 e 0 ...
- Ti4Al_RD s 216 e 0 ...
- Ti4Al_RD s 220 e 0 ...
- Ti4Al_RD s 223 e 0 ...
- Ti4Al_RD s 237 e 0 ...
- Ti4Al_RD s 258 e 0 ...
- Ti4Al_RD s 282 e 0 ...
- Ti4Al_RD s 309 e 0 ...
- Ti4Al_RD s 340 e 0 ...
- Ti4Al_RD s 38 e 0 0...
- Ti4Al_RD s 49 e 0 0...
- Ti4Al_RD s 6 e 0 00...
- Ti4Al_RD s 6 e 0 00...
- Ti4Al_RD s 6 e 0 00...
- Ti4Al_RD s 63 e 0 0...
- Ti4Al_RD s 7 e 0 00...
- Ti4Al_RD s 7 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 8 e 0 00...
- Ti4Al_RD s 9 e 0 00...
- Ti4Al_RD s 97 e 0 0...
- Ti6Al_45 s 120 e 0 ...
- Ti6Al_45 s 139 e 0 ...
- Ti6Al_45 s 183 e 0 ...
- Ti6Al_45 s 241 e 0 ...
- Ti6Al_45 s 250 e 0 ...
- Ti6Al_45 s 274 e 0 ...
- Ti6Al_45 s 309 e 0 ...
- Ti6Al_45 s 319 e 0 ...
- Ti6Al_45 s 324 e 0 ...
- Ti6Al_45 s 331 e 0 ...
- Ti6Al_45 s 338 e 0 ...
- Ti6Al_45 s 351 e 0 ...
- Ti6Al_45 s 375 e 0 ...
- Ti6Al_45 s 413 e 0 ...
- Ti6Al_45 s 440 e 0 ...
- Ti6Al_45 s 7 e 0 00...
- Ti6Al_45 s 7 e 0 00...
- Ti6Al_45 s 7 e 0 00...
- Ti6Al_45 s 7 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 8 e 0 00...
- Ti6Al_45 s 91 e 0 0...
- Ti6Al_ND s 120 e 0 ...
- Ti6Al_ND s 150 e 0 ...
- Ti6Al_ND s 159 e 0 ...
- Ti6Al_ND s 200 e 0 ...
- Ti6Al_ND s 264 e 0 ...
- Ti6Al_ND s 299 e 0 ...
- Ti6Al_ND s 300 e 0 ...
- Ti6Al_ND s 322 e 0 ...
- Ti6Al_ND s 343 e 0 ...
- Ti6Al_ND s 355 e 0 ...
- Ti6Al_ND s 366 e 0 ...
- Ti6Al_ND s 376 e 0 ...
- Ti6Al_ND s 403 e 0 ...
- Ti6Al_ND s 426 e 0 ...
- Ti6Al_ND s 457 e 0 ...
- Ti6Al_ND s 490 e 0 ...
- Ti6Al_ND s 522 e 0 ...
- Ti6Al_ND s 7 e 0 00...
- Ti6Al_ND s 7 e 0 00...
- Ti6Al_ND s 7 e 0 00...
- Ti6Al_ND s 7 e 0 00...
- Ti6Al_ND s 7 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 8 e 0 00...
- Ti6Al_ND s 80 e 0 0...
- Ti6Al_RD s 113 e 0 ...
- Ti6Al_RD s 119 e 0 ...
- Ti6Al_RD s 172 e 0 ...
- Ti6Al_RD s 227 e 0 ...
- Ti6Al_RD s 249 e 0 ...
- Ti6Al_RD s 256 e 0 ...
- Ti6Al_RD s 279 e 0 ...
- Ti6Al_RD s 296 e 0 ...
- Ti6Al_RD s 303 e 0 ...
- Ti6Al_RD s 309 e 0 ...
- Ti6Al_RD s 312 e 0 ...
- Ti6Al_RD s 328 e 0 ...
- Ti6Al_RD s 348 e 0 ...
- Ti6Al_RD s 373 e 0 ...
- Ti6Al_RD s 396 e 0 ...
- Ti6Al_RD s 423 e 0 ...
- Ti6Al_RD s 68 e 0 0...
- Ti6Al_RD s 7 e 0 00...
- Ti6Al_RD s 7 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 8 e 0 00...
- Ti6Al_RD s 87 e 0 0...
- Ti6Al_RD s 9 e 0 00...
- Ti6Al_RD s 9 e 0 00...
- Ti6Al_RD s 9 e 0 00...
- Titanium
- Zr_R300 s 10 e 0 00...
- Zr_R300 s 10 e 0 00...
- Zr_R300 s 100 e 0 0...
- Zr_R300 s 119 e 0 0...
- Zr_R300 s 120 e 0 0...
- Zr_R300 s 120 e 0 0...
- Zr_R300 s 125 e 0 0...
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- Zr_R300 s 151 e 0 0...
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- Zr_R300 s 158 e 0 0...
- Zr_R300 s 163 e 0 0...
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- Zr_R300 s 174 e 0 0...
- Zr_R300 s 178 e 0 0...
- Zr_R300 s 179 e 0 0...
- Zr_R300 s 181 e 0 0...
- Zr_R300 s 181 e 0 0...
- Zr_R300 s 183 e 0 0...
- Zr_R300 s 184 e 0 0...
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- Zr_R300 s 187 e 0 0...
- Zr_R300 s 189 e 0 0...
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- Zr_R300 s 195 e 0 0...
- Zr_R300 s 200 e 0 0...
- Zr_R300 s 200 e 0 0...
- Zr_R300 s 204 e 0 0...
- Zr_R300 s 206 e 0 0...
- Zr_R300 s 213 e 0 0...
- Zr_R300 s 218 e 0 0...
- Zr_R300 s 223 e 0 0...
- Zr_R300 s 227 e 0 0...
- Zr_R300 s 233 e 0 0...
- Zr_R300 s 238 e 0 0...
- Zr_R300 s 247 e 0 0...
- Zr_R300 s 256 e 0 0...
- Zr_R300 s 264 e 0 0...
- Zr_R300 s 40 e 0 00...
- Zr_R300 s 60 e 0 00...
- Zr_R300 s 80 e 0 00...
- Zr_RT s 10 e 0 00 p...
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- Zr_RT s 11 e 0 00 p...
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- Zr_RT s 367 e 0 00 ...
- Zr_RT s 389 e 0 00 ...
- Zr_RT s 394 e 0 00 ...
- Zr_RT s 400 e 0 00 ...
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- Zr_RT s 405 e 0 00 ...
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- Zr_RT s 50 e 0 00 p...
- Zr_RT s 523 e 0 00 ...
- Zr_RT s 548 e 0 00 ...
- Zr_RT s 595 e 0 00 ...
- Zr_cool s 10 e 0 00...
- Zr_cool s 10 e 0 00...
- deformation
- du Zr Os 120 07p 10...
- du Zr Os 121 10p 10...
- du Zr Os 165 51p 10...
- du Zr Os 206 62p 10...
- du Zr Os 24 13p 10 ...
- du Zr Os 241 40p 10...
- du Zr Os 266 41p 10...
- du Zr Os 283 10p 10...
- du Zr Os 295 53p 10...
- du Zr Os 297 87p 10...
- du Zr Os 306 84p 10...
- du Zr Os 360 29p 10...
- du Zr Os 390 54p 10...
- du Zr Os 4 42p 10 6...
- du Zr Os 40 11p 9 3...
- du Zr Os 417 48p 9 ...
- du Zr Os 444 25p 9 ...
- du Zr Os 454 39p 9 ...
- du Zr Os 462 67p 9 ...
- du Zr Os 47 77p 10 ...
- du Zr Os 475 71p 9 ...
- du Zr Os 484 56p 9 ...
- du Zr Os 492 53p 9 ...
- du Zr Os 502 70p 9 ...
- du Zr Os 513 13p 9 ...
- du Zr Os 526 93p 9 ...
- du Zr Os 530 36p 9 ...
- du Zr Os 541 18p 9 ...
- du Zr Os 553 07p 9 ...
- du Zr Os 563 35p 9 ...
- du Zr Os 577 37p 9 ...
- du Zr Os 586 49p 9 ...
- du Zr Os 72 22p 10 ...
- du Zr Os 9 89p 9 33...
- du Zr Os 95 43p 10 ...
- effect
- mechanisms
- xscan x 192 480
- xscan x 192 980
- xscan x 193 480
- xscan x 193 980
- xscan x 194 480
- xscan x 194 980
- xscan x 195 480
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- xscan x 200 980
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- xscan x 206 980
- xscan x 207 480
- yscan y 222 980
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- yscan y 242 850
Provenance | |
---|---|
Creator | Dr Joao Quinta da Fonseca; Dr Michael Preuss; Mr Arnas Fitzner; Dr Leo Prakash; Dr Matthew Thomas; Mr Benjamin Cousins; Mr Peter Honniball; Dr Dinesh Srivastava |
Publisher | ISIS Neutron and Muon Source |
Publication Year | 2015 |
Rights | CC-BY Attribution 4.0 International; https://creativecommons.org/licenses/by/4.0/ |
OpenAccess | true |
Contact | isisdata(at)stfc.ac.uk |
Representation | |
---|---|
Resource Type | Dataset |
Discipline | Photon- and Neutron Geosciences |
Temporal Coverage Begin | 2012-05-21T08:51:09Z |
Temporal Coverage End | 2012-05-25T13:05:54Z |