We explain these imaging results using 𝜇 !_#$# and 𝜇 %_#$# , from Table . The linear coherent scattering, incoherent scattering, and absorption coefficients for these materials are given in Table and are summed to give the total linear coefficients in Table . In accordance with our imaging results, Cu with a 𝜇 %_#$# of ~ 133 cm -1 , which is > 200 times than both graphite and LiOH, should be clearly visible with X-rays in contrast to graphite and LiOH, which will be difficult to distinguish. Moreover, due to the sensitivity of neutrons to LiOH (𝜇 !_#$#_,-./ = 5.82 cm -1 ), regions of the XFC-cycled anode that contain LiOH are clearly visible in neutron images. In addition, since 𝜇 !_#$#_,-./ is ~ five times greater than 𝜇 !_#$#_01 , neutron tomography holds promise for imaging plated Li-species. However, the low relative neutron contrast between Cu and graphite (𝜇 !_#$#_01 : 𝜇 !_#$#_+2345-#6 ~ 2) made it impossible for us to distinguish them from each other in the neutron images.