                        1         !   "# $%% & a ’(’’) b *$#(’ c ’’(’’)   )  +,    ) ,  + ’  Iterative processing, involving sequential deformation and annealing, has been carried out on copper specimens with the aim of grain boundary engineering (GBE) them. The data have provided some interesting insights into the mechanisms of GBE. The results have demonstrated that development of a high proportion of Σ3s is beneficial to properties, as shown by improved strain$to$failure for the same strength. The proportion of Σ3s saturates at approximately 60% length fraction. Analysis of the data indicates that iterative processing is not always necessary for the development of beneficial properties, and it is further suggested that the condition of the starting specimen has a large influence on the subsequent microstructural development. The present, new data are also compared with previous research on copper where all five parameters of the grain boundary network population have been measured.  It is now established that thermomechanical manipulation of grain boundary crystallography improves material properties such as corrosion resistance, intergranular cracking or ductility. This practice has become know as ‘grain boundary engineering’ (GBE). GBE is linked to prolific twinning in low stacking$fault energy metals and alloys. Recently GBE in this class of materials has been reviewed and discussed in detail [1,2]. Areas where GBE research is ongoing include the role of grain boundary planes [3], interface connectivity [4] and modelling and predictions of intergranular failure [5]. Application of cold deformation followed by annealing schedules is at the heart of GBE processing. Usually iterative processing regimes are employed. A typical GBE processing schedule, as quoted in the original patent for GBE [6], would be several iterations (e.g. 3$7) of cold work (e.g. 20%$ 40% reduction) and annealing at a temperature which is approximately 0.6$0.8 of the absolute melting temperature for a few minutes which results in a fine grain size and certain property improvements such as improved intergranular corrosion resistance. For example, for Inconel 600 the requirements for GBE were 3$7 iterations of 5%$30% cold work followed by annealing at 900°C$1050°C for 2$10 minutes [6]. Such a schedule claimed to ensure that the grain size remained small, <30m, and that the fraction of coincidence site lattice (CSL) boundaries increased to 50%$70%. A variant on the original GBE processing specification is strain$anneal processing. This processing involves low levels of cold work, up to 6% strain, followed by anneals of up to many hours at temperatures typically lower than those used for recrystallisation GBE. A similar improvement in properties and/or attributes occurs when strain$annealing is used compared to recrystallisation annealing, although the former may result in larger a grain size [1]. The ‘strain$recrystallisation’ description of GBE processing is probably a misnomer and more accurately it should be termed ‘strain$ recovery’, since TEM evidence has indicated that insufficient strain is localised at grain boundaries to instigate nucleation of recrystallisation during the short annealing cycles [7]. Materials Science Forum Vol. 550 (2007) pp 35-44 Online: 2007-07-15 © (2007) Trans Tech Publications, Switzerland doi:10.4028/www.scientific.net/MSF.550.35 All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of Trans Tech Publications, www.ttp.net. (ID: 137.44.1.174, Swansea University, Swansea, United Kingdom-13/11/15,10:48:51)