“…Formally, a least-squares principle for (1) can be easily extended to handle (47) by modifying (4) and (3) to min u∈S J G (u; f, g), where J G (u; f, g) = Lu + G(u) − f 2 HΩ + Ru − g 2 HΓ (48) and then define a LSFEM by restricting (48) to a family S h ⊂ S. While the extension of LSFEMs to (47) is trivial, its analysis is not and remains one of the open problems in LSFEMs. Compared with the well-developed mathematical theory for linear elliptic problems [2,13,18,21,23,24,26,32,38], analyses of LSFEMs for nonlinear problems are mostly confined to the Navier-Stokes equations [7][8][9]. It can be shown that the Euler-Lagrange equation associated with the leastsquares principle (48) for the Navier-Stokes equations has the abstract form…”