Two core-shell materials were made in a continuously stirred tank reactor, one with a Ni(OH) 2 core and a Ni 1/2 Mn 1/2 (OH) 2 shell and the other with a Ni 1/2 Mn 1/2 (OH) 2 core and a Ni 0.17 Mn 0.83 (OH) 2 shell. X-ray diffraction measurements (Cu K α radiation) of the core-shell materials were compared to reference materials which were physical mixtures with the same overall composition. The smaller core peaks in the XRD patterns of the core-shell materials were attributed to absorption of X-rays due primarily to the high manganese contents of the shells. Calculations were performed assuming spherical particles of radius matching results from SEM/EDS measurements. For a 5.5 μm radius particle with a Ni(OH) 2 core, the shell thickness was calculated from XRD patterns to be 0.47 ± 0.03 μm. For a 7.9 μm particle of the material with the Ni 1/2 Mn 1/2 (OH) 2 core, the shell was determined to be 1.77 ± 0.15 μm thick. Both these results were found to agree well with the overall composition of the samples as determined by elemental analysis and with spatial EDS measurements. This X-ray absorption modeling technique provides an experimentally simple way to measure the thickness of micron scale shell coatings while sampling all particles, unlike methods such as EDS. Future applications for lithium-ion batteries will demand higher energy density, improved safety, and improved lifetime all without sacrificing cost. The choice of cathode material used in a cell can have dramatic effects on energy density, safety, cost and lifetime.1 Recently, researchers have been developing new cathode materials called "coreshell" materials.2-8 Core-shell materials are made by encapsulating one composition of a cathode material in a shell of a different composition. This is done to exploit the beneficial characteristics of each of the core and shell materials. Ideally, the core material should have a low cost and high energy density. The shell material should show superior stability with the electrolyte, and hence should have very high coulombic efficiency. Combining two such materials would allow a cathode to have both high energy density and long lifetime. There have been many studies previously completed on homogeneous materials that are excellent candidates for both core and shell materials. 7,[9][10][11][12] Optimizing the core-shell motif requires careful consideration of the thickness of the shell coating. If the shell coating is too thin, coverage may be incomplete such that the core may be exposed to the electrolyte and additional parasitic reactions could then occur between the electrolyte and the core material and reduce the lifetime of the cell.13,11 Alternatively, if the shell is too thick the energy density will not be maximized.Measuring the thickness of the shell has been accomplished by other researchers through spatial spectroscopic composition techniques such as energy disperse spectroscopy (EDS).14 This procedure has been useful in proving that a shell is coating the core particles, however it has several disadvanta...