“…For one-equation transition models, a variety of γ transition models were proposed: Lodefier et al [32], Wang and Fu [33], Durbin [34], Ge et al [35], Menter et al [36] and Juntasaro et al [37]. Besides the intermittency factor γ, Mayle and Schulz [38], Walters and Leylek [39], Walters and Cokljat [40] and Medina et al [41] developed the k L transition model. As an alternative to the kinetic energy of laminar fluctuations k L , Lopez and Walters [42] proposed the ν 2 transition model, where ν 2 is the wall-normal velocity fluctuation made approximately equal to the difference between the turbulent kinetic energy k and the kinetic energy of laminar fluctuations k L , i.e., ν 2 ≈ k − k L .…”