“…[ 17–19,43,46,59,61,63,65,66,69,75,76,80 ] Compared with the Schiller–Naumann model, [ 107 ] the Morsi–Alexander model [ 108 ] is more complete because it expands the Reynolds number to a large range, and this model has also been used by many authors. [ 13,15,38,40–43,45,52,65 ] In addition, the Haider–Levenspiel, [ 109 ] Kuo–Wallis, [ 110 ] Ishii–Zuber, [ 111 ] Tomiyama, [ 112 ] and Liu et al [ 113 ] models, based on bubble deformation, were, respectively, selected to describe the gas–liquid flow in an RH degasser by Chen et al, [ 39 ] Wei et al, [ 56,57 ] Peixoto et al, [ 72 ] Rimbert et al, [ 14 ] and Dong et al [ 51 ] Among them, a shape factor was used to consider the bubble deformation by Chen et al [ 39 ] and Dong et al, [ 51 ] and the bubble shape was not addressed explicitly by Rimbert et al [ 14 ] and Peixoto et al [ 72 ] Recently, Ling et al [ 43 ] investigated the effect of several drag coefficient models on the gas–liquid two‐phase flow in the physical model of an RH degasser, and found that the Schiller–Naumann [ 107 ] and Morsi–Alexander [ 108 ] models, based on spherical bubbles, provided better prediction in terms of the liquid velocity. However, a puzzling result was obtained in the study by Cao et al, [ 52 ] in which the liquid could hardly circulate by using the Schiller–Naumann model, [ 107 ] but the liquid velocity could be well predicted by using the Morsi–Alexander model [ 108 ] for the simulation of the physical model of an RH degasser.…”