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Figure 8.5 Map views of (a) step-overs and (b) bends and associated structures (after McClay & Bonora, 2001, Bull. Am. Assoc. Petroleum Geols. AAPG 2001, reprinted by permission of the AAPG whose permission is required for further use). (c) Map and (d) cross-sections of strike-slip duplexes, fans and ower structures developed at bends (after Woodcock & Rickards, 2003, with permission from Elsevier).

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Gronmaier, K Janischowsky, J Kusterer, E Kohn, Diam Rel Mat 14 (2005) u 504 508 [181] X Xiao, J Birrell, J E Gerbi, O Auciello, J A Carlisle, J Appl Phys 96 (2004) 2232 2239 [182] A Kaiser, D Kueck, P Benkhart, A Munding, G M Prinz, A Heittmann, H Huebner, R Sauer, E Kohn, Diam Rel Mat 15 (2006) 1967 1971 [183] H H bner, O Ehrmann, M Eigner, W Gruber, A Klumpp, R Merkel, P Ramm, M Roth, u J Weber, R Wieland, Face-to-face chip integration with full metal interface, Advanced Metallization Conference, AMC (2002), San Diego, CA, USA, MRS Proceedings 18, 5358 [184] A Munding, PhD thesis, University of Ulm, Germany (2007) [185] A Kaiser, PhD thesis, University of Ulm, Germany (2007) [186] P Benkhart, PhD thesis, University of Ulm (2008) [187] R S Okojie, G M Benheim, G J Saad, E.

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tionships suggest that orogenesis and crustal growth in the Lachlan orogen were dominated by magmatism and the recycling of continental detritus during cycles of extension and contraction that lasted from Late Ordovician through early Carboniferous times. Cycles of backarc and intra-arc extension, such as those that occurred in the Lachlan orogen, generate thin, hot lithosphere that may localize deformation during subsequent phases of contraction, collision, and orogeny (Hyndman et al., 2005). Collins (2002b) illustrated this process in a model of orogenesis involving the formation and closure of autochthonous backarc basins (Section 9.10) above a long-lived subduction zone. The model begins with a zone of intra-arc extension that evolves in response to the roll back (Section 9.10) of a subducting slab (Fig. 10.37a). This setting

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Savrun, Characteristics of a hermetic 6HSiC pressure sensor at 600 C, AIAA Space (2001) Conference and Exposition, Albuquerque, NM, USA, Abstract AIAA (2001) 4652 August (2001), 1 8 [188] L Cheng, M Pan, J Sco eld, A J Steckl, J Electr Mat 31 (2002) 361 365 [189] M Mehregany, C A Zorman, Thin Solid Films 355 356 (1999) 518524 [190] E Kohn, W Ebert, M Adamschik, P Schmid, A Denisenko, New Diam Front Carbon Technol 11 (2001) 81 100 [191] M Adamschik, P Gluche, A Fl ter, W Ebert, E Kohn, The potential of CVD diamond o lms for sensor and actuator applications, 9th International Trade Fair and Conference for Sensors Transducers and Systems, 18 20 May (1999), Nuremberg, Germany, Proceedings 287 292 [192] P R Chalker, C Johnston, Phys Stat Sol (a) 154 (1996) 455 466 [193] D R Wur, J L Davidson, J Microelectromech Sys.

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The heat transfer rates at the dry and wet parts of a partly wet coil are related to the resulting changes in the states of the uids by Equation 4.38: qdc = ma Cpa (Ta1 - Tab ) = ma (ha1 - hab ) = mw Cpw (Tw1 - Twb ) qwct = ma (hab - ha2 ) = mw Cpw (Twb - Tw2 ) qct = qdc + qwct = ma (ha1 - ha2 ) = mw Cpw (Tw1 - Tw2 ) (4.38a) (4.38b) (4.38c)

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