5.1 IntroductionCoated conductors are electrical conductors prepared with YBa 2 Cu 3 O 7 -x ( YBCO ) superconducting material coatings deposited on metallic substrates along with several other intermediate buffer layers. Buffer layers are deposited sequentially on the metallic substrates prior to YBCO deposition to serve as barrier layers. They are selected such that epitaxial relationships are maintained throughout the thickness of the coated conductors to obtain highly -textured YBCO coatings. To process conductors with high critical current density ( J c ), highly -textured YBCO coatings with both in -plane and out -of -plane alignment of grains are required with grain boundary misorienation angles below 5 o . More details of the texture requirements, processing, and different types of coated conductor architectures can be found in other chapters of this book as well as in the references [1 -5] . Two primary industrial approaches are used to manufacture the coated conductors. One approach uses a rolling assisted biaxially textured (RABiTS ™ ) metallic substrate such as N -5 at.% W with sputtered Y 2 O 3 /YSZ/Ce 2 O 3 buffer layers and YBCO layer deposited by the metallo -organic deposition ( MOD ) technique [3] . In the second approach, a polycrystalline Hastealloy ™ substrate is coated with textured MgO buffer layer grown by ion beam assisted deposition ( IBAD ) and other subsequent buffer layers [4] . YBCO is deposited by metallo -organic chemical vapor deposition ( MOCVD ) on these substrates. In recent years, impressive progress has been made in the manufacturing of long lengths of YBCO coated conductors processed by using both the RABiTS ™ substrates as well as IBAD substrates [6,7] . Such longlength coated conductors are needed to make coils for rotating machinery and cables for electrical transmission. However, in high magnetic fi eld applications such as MRI (Magnetic Resonance Imaging), SMES (Superconducting Magnetic Energy Storage), superconducting magnets and generators, etc., high J c at high magnetic fi elds needs to be maintained. In the absence of fl ux pinning centers in the coated conductors, the magnetic fl ux lines will move due to Lorenz forces acting upon them at high fi elds. This motion causes dissipation, and losses will occur as a result. This lowers the J c in coated conductors. Hence, it is important High Temperature Superconductors. Edited by Raghu Bhattacharya and M. Parans Paranthaman