“…This technique defines the fluid into a set of particles that interact with each other (Gingold & Monaghan, 1977;Lucy, 1977;Monaghan, 1992), and also makes it easier to model the interface between the two phases than the Euler method. It is widely used in fluid mechanics problems, including free surface flows (Omidvar, et al, 2015), wave-body interactions , and multiphase flow (Hosseinkhani & Omidvar, 2018) as well as non-Newtonian fluid flows, which are defined by various viscoplastic models such as Bingham, Herschel-Buckley, Cross, etc. (Shakibaeinia & Jin, 2011;Khanpour, et al, 2016;Omidvar, et al, 2018;Fourtakas & Rogers, 2016;Nikeghbali & Omidvar, 2018).…”