We predicted the attenuated, undesired secondary scattered, and undesired harmonic components of measured X-ray intensities from synchrotron X-ray radiographic visualizations of liquid water in an operating polymer electrolyte membrane (PEM) fuel cell. The undesired secondary scattered component of the measured intensity increased as a function of the liquid water thickness (traversed by the X-ray beam). This increase in the secondary scattered component led to a decrease in the calibrated attenuation coefficient for liquid water, decreasing the accuracy of water quantification. We recommend calibrating the attenuated coefficient with a range of water thicknesses defined by the maximum expected water thickness present in the PEM fuel cell. The undesired harmonic component of the measured intensity also increased as a function of liquid water thickness, which led to a decrease in the accuracy of the measured liquid water thickness. Operating the polymer electrolyte membrane (PEM) fuel cell at high current densities is a strategy for achieving effective catalyst utilization and decreasing the cost of power.1 However, high current density operation corresponds to high rates of water production, and excess liquid water can lead to the inhibition of reactant transport and poor overall fuel cell performance. Therefore, effective water management is an important design objective for the PEM fuel cell.Synchrotron X-ray radiography, with its high spatial and temporal resolutions, has been used as a diagnostic tool to directly visualize liquid water transport in PEM fuel cells in operando.2-21 Radiographic images of the operating fuel cell during open circuit voltage (OCV) are termed dry-state images because we assume that excess liquid water is not present during this operating regime. For all non-zero current densities, radiographic images are termed wet-state images because of the possible appearance of additional liquid water with respect to the reference dry-state images (obtained at OCV). The cumulative liquid water thickness traversed by the X-ray beam, t w [cm], is quantified for each pixel of a collected two-dimensional (2D) wet-state image using the following relationship 22 derived from the Beer-Lambert law:where μ at [cm −1 ] is the linear attenuation coefficient for a monoenergetic X-ray beam and is a function of the photon energy, and the subscript "w" identifies the material as water. Herein, the measured intensity of the X-ray beam after traversing the sample is referred to as the attenuated intensity. I m,dr y is the measured attenuated intensity of a reference dry-state image (in the absence of liquid water), and I m,wet is the measured attenuated intensity of a wet-state image.The accuracy of liquid water thickness quantities determined from Equation 1 corresponds to the accuracies of the measured attenuated * Electrochemical Society Student Member. 23 determined that the vertical position of the incident beam oscillated with a significant amplitude of 25 μm, which resulted in image artifacts. The auth...