Abstract. Atomistic simulations of bicrystal samples containing a grain boundary are used to examine the effect of hydrogen atoms on the nucleation of intergranular cracks in Ni. Specifically, the theoretical strength is obtained by rigid separation of the two crystals above and below the GB and the yield strength (point of dislocation emission) is obtained by standard tension testing normal to the GB. These strengths are computed in pure Ni and Ni with H segregated to the grain boundaries under conditions typical of H embrittlement in Ni, and in highly-H-saturated states. In all GBs studied here, the theoretical strengthσ is not significantly reduced by the presence of the hydrogen atoms. Similarly, with the exception of the NiΣ27(115) 110 boundary, the yield strength σy is not significantly altered by the presence of segregated H atoms. In all cases, the theoretical strengths are ∼25 GPa and the yield strengths are ∼10 GPa, so that (i) the theoretical strength is always well above the yield strength, with or without H, and (ii) both strengths are far above the bulk plastic flow stress, σ B y of Ni and Ni alloys. Complementing recent work showing that H does not change the ability of GB cracks to emit dislocations and blunt, the present work indicates that hydrogen atoms segregated to the GB have little effect on lowering the GB strength and so do not significantly facilitate nucleation of intergranular cracks.