Magnetic resonance imaging is a popular non-invasive technique for investigating soft tissue structures within the human body. Many design methods now exist for their principle hardware components, such as the radio frequency (RF) coils. A popular RF coil type is the RF phased array, comprised of many closely spaced coils covering a large volume. A time harmonic inverse method is presented for the theoretical design of RF phased arrays. The method allows any array size to be considered where the focus is on optimal coil geometry and position of individual coils. An ill-conditioned integral equation is solved using a regularisation strategy in which the error between induced and target magnetic fields is minimised along with an additional constraint related to the curvature of the coil windings. The method is demonstrated for a number of design considerations and includes the ability to focus the RF field to arbitrary locations within the coil volume. The effect of the choice of magnetic field polarisation direction is also investigated using the model. References Jin J. 1999. Electromagnetic Analysis and Design in Magnetic Resonance Imaging, Florida: CRC Press. Lawrence B. G., Crozier S., Yau D. D. and Doddrell D. M. 2002. A time-harmonic inverse methodology for the design of rf coils in mri, IEEE Transactions on Biomedical Engineering 49(1), 64--71. doi:10.1109/10.972841 Li B. K., Liu F. and Crozier S. 2005. Focused, eight-element transceive phased array coil for parallel magnetic resonance imaging of the chest --- theoretical considerations, Magnetic Resonance in Medicine 53, 1251--1257. doi:10.1002/mrm.20505 Ramo S., Whinnery J. R. and van Duzer T. 1967. Fields and waves in communication electronics, New York: John Wiley and Sons, Inc. Roemer P. B., Edelstein W. A., Hayes C. E., Souza S. P. and Mueller O. M. 1990. The nmr phased array, Magnetic Resonance in Medicine 16(2), 192--225. doi:10.1002/mrm.1910160203 Sodickson D. K., McKenzie C. A., Ohliger M. A., Yeh E. N. and Price M. D. 2002. Recent advances in image reconstruction, coil sensitivity calibration, and coil array design for SMASH and generalized parallel mri, Magnetic Resonance Materials in Physics, Biology and Medicine 13, 158--163. Turner R. 1986. A target field approach to optimal coil design, Journal of Physics D: Applied Physics 19, L147--L151. doi:10.1088/0022-3727/19/8/001 While P. T., Forbes L. K. and Crozier S. 2005a. A time-harmonic target-field method for designing unshielded rf coils in mri, Measurement Science and Technology 16, 997--1006. doi:10.1088/0957-0233/16/4/012 While P. T., Forbes L. K. and Crozier S. 2005b. A time-harmonic target-field method for designing shielded rf coils in mri, Measurement Science and Technology 16, 1381--1393. doi:10.1088/0957-0233/16/6/021 While P. T., Forbes L. K. and Crozier S. 2006. An inverse method for designing loaded rf coils in mri, Measurement Science and Technology 17, 2506--2518. doi:10.1088/0957-0233/17/9/019 Brideson M. A., Forbes L. K. and Crozier S. 2002. Determining complicated winding patterns for shim coils using streamfunctions and the target-field method, Concepts in Magnetic Resonance 14(1), 9--18. doi:10.1002/cmr.10000 While P. T., Forbes L. K. and Crozier S. 2007. An inverse method for designing rf phased array coils in mri --- theoretical considerations, Measurement Science and Technology 18, 245--259. doi:10.1088/0957-0233/18/1/031 Delves L. M. and Mohamed J. L. 1985. Computational methods for integral equations, Cambridge: Cambridge University Press. Forbes L. K. and Crozier S. 2002. A novel target-field method for finite-length magnetic resonance shim coils: II. tesseral shims, Journal of Physics D: Applied Physics 35, 839--849. doi:10.1088/0022-3727/35/9/303 Hardy C. J., Cline H. E., Giaquinto R. O., Niendorf T., Grant A. K. and Sodickson D. K. 2006. 32-element receiver-coil array for cardiac imaging, Magnetic Resonance in Medicine 55, 1142--1149. doi:10.1002/mrm.20870