The electrode microstructure plays an integral role in the performance of the non-aqueous Li-air battery. Computational modeling has proven to be an indispensible tool in the analysis of battery systems, but previous macroscale, volume-averaged models that consider the porous electrode as a homogenous medium of uniform geometric properties are insufficient to probe the effect of precise electrode microstructures. Utilizing a pore-scale transport-resolved model of the Li-air battery, the complex electrode and Li 2 O 2 morphologies can be directly incorporated and their effects on the system-level performance can be evaluated. A thickness-dependent electrical conductivity of Li 2 O 2 is considered in the model based on inputs from the density functional theory. Model validation is presented along with a sensitivity study of the applied current density and the reaction rate coefficient. The effect of electrode geometry (e.g., nanostructure spacing and height) on cell performance, including its influence on pore blocking compared against electrical insulation, is investigated. Pore blocking is observed for cathodes with nanostructure spacing less than twice a critical insulating thickness of Li 2 O 2 , suggesting the loss of active surface area as the mechanism for decreased cell performance. While for cathodes with larger nanostructure spacing, the discharge capacity is dictated by the electrical insulation of Developing a battery with the energy density of fossil fuel has been an elusive goal that will likely usher in the widespread implementation of high-energy storage applications, such as electrified transportation 1 . Current Li-ion batteries (100 -480 Wh kg −1 practical 2-4 ) have only 5-28% of the specific energy of gasoline (1700 Wh kg −1 practical 5 ); in order to drive 300 miles, an electric car would need a 500 kg Liion battery.4 Alternatively, the non-aqueous Li-air (or more precisely Li-oxygen) batteries (1800 -2700 Wh kg −1 practical 6-10 ) have up to 5 times the energy density of Li-ion batteries, putting them well within the range of gasoline 1 . Several factors contribute to the high energy density of Li-air battery: (i) there is no heavy transition metal in the cell, 11 (ii) lithium is the lightest and most electronegative anode metal, and (iii) the gaseous reactant O 2 is not contained within the cell but instead can be drawn from the surroundings. However, the relatively new Li-air battery still underperforms in several key factors when compared to the more established Li-ion battery, such as low round trip efficiency (70% 9,12 vs. >95% 13 ), low drawing current density (0.1-1.0 mA cm −28,14 vs. 30 mA cm −214 ) and poor cycle life (∼100 15,16 vs. 5000 17 ). The source of these problems can be traced to a number of key issues, including the electric insulation of the reaction products, [18][19][20][21][22] parasitic irreversible side reactions, 23-26 electrolyte instability, 12,23,24 and electrode degradation. 12,27 These shortcomings must be overcome in order for the Li-air battery to become via...