A survey of the calculations of the isovector axial vector form factor of the nucleon using lattice QCD is presented. Attention is paid to statistical and systematic uncertainties, in particular those due to excited state contributions. Based on a comparison of results from various collaborations, a case is made that lattice results are consistent within 10%. A similar level of uncertainty is in the axial charge gAuβd, the mean squared axial charge radius β¨rA2β©, the induced pseudoscalar charge gPβ, and the pionβnucleon coupling gΟNN. Even with the current methodology, a significant reduction in errors is expected over the next few years with higher statistics data on more ensembles closer to the physical point. Lattice QCD results for the form factor GA(Q2) are compatible with those obtained from the recent MINERΞ½A experiment but lie 2β3Ο higher than the phenomenological extraction from the old Ξ½βdeuterium bubble chamber scattering data for Q2>0.3 GeV2. Current data show that the dipole ansatz does not have enough parameters to fit the form factor over the range 0β€Q2β€1 GeV2, whereas even a z2 truncation of the z expansion or a low order PadΓ© are sufficient. Looking ahead, lattice QCD calculations will provide increasingly precise results over the range 0β€Q2β€1 GeV2, and MINERΞ½A-like experiments will extend the range to Q2βΌ2 GeV2 or higher. Nevertheless, improvements in lattice methods to (i) further control excited state contributions and (ii) extend the range of Q2 are needed.