Capacity fade in lithium-ion batteries remains an area of active research, with failure of the graphite anode thought to be an important contributor. While the formation of the solid electrolyte interphase and the subsequent loss of cyclable lithium have been well studied, mechanical degradation remains an area where ambiguity remains. While there appears to be little experimental evidence that suggest that macroscopic particle cracking occurs, mathematical models have suggested that this phenomenon is likely. The goal of this paper is to clarify this ambiguity by combining experimental cycling, mathematical stress modeling, and post-mortem microscopy. We experimentally determine an average diffusion coefficient of lithium in graphite using a thin-layer electrode and use this information in a diffusion-induced stress model. Our results suggest that cracking is not likely during lithiation due to the proximity of equilibrium potential to the cutoff potential. On delithiation, at 25 • C, even at 30 C rate cracking is unlikely while at −10 • C, a rate of 10 C can lead to particle cracking. By extrapolating the results of the thin-layer electrode to a thick porous electrode, we found that graphite cracking is unlikely to occur during typical vehicle operations. In recent years, there have been numerous studies on lithium-ion batteries for vehicle applications. [1][2][3][4][5] Of particular interest are the various degradation mechanisms encountered when operating the battery under severe conditions (i.e., wide temperature ranges and high Crates) typical for vehicle applications.6 One likely degradation mechanism is the mechanical breakdown of the active materials. Lithium insertion (or extraction) into (or out of) the lattice of the active materials causes volume change (expansion and contraction), resulting in stress generation and possible fracture of the particles. For example, in graphite anodes, crack generation can expose new surfaces to the electrolyte, leading to further formation of the solid electrolyte interphase (SEI) 7,8 and/or particle isolation from the electronic network, leading to impedance growth, loss of cyclable lithium, and capacity fade.Mathematical models, based on diffusion-induced stress generation, have been used to investigate particle fracture and have suggested that graphite particle cracking is likely under certain conditions. [9][10][11][12][13] For the diffusion-induced stress model, diffusion coefficient in solid phase is a key parameter to determine the concentration gradient in the particle, which in turn affects the stress generated.9 However, there is a wide disparity in the measured diffusion coefficient of lithium in graphite, ranging from 10 −16 to 10 −11 m 2 /s. [14][15][16][17][18][19] This wide range can be attributed to different kinds of graphite used in these studies in addition to different techniques used to extract the diffusion coefficient. Model predictions would suggest that for the lower value of diffusion coefficient (1.0 × 10 −14 m 2 /s) particle cracking durin...