“…with µ l the liquid viscosity and σ the surface tension coefficient. As the bubble grows outside of the cavity, Ca can be large enough to impede liquid motion at the wall and trap a thin liquid layer underneath the bubble: the liquid microlayer -see experimental evidence by Moore & Mesler (1961), Hendricks & Sharp (1964), Hospeti & Mesler (1965), Jawurek (1969), Foltz & Mesler (1970), Judd (1975), Judd & Hwang (1976), Koffman & Plesset (1983), Moghaddam & Kiger (2009), Golobic et al (2009), Kim & Buongiorno (2011), Gao et al (2013), Jung & Kim (2014), Jung & Kim (2015), Bigham & Moghaddam (2015), Yabuki & Nakabeppu (2014), Yabuki & Nakabeppu (2016), and Zou et al (2016a). Once the bubble has reached a certain size, referred to as departure diameter, the bubble departs from its initial position at the heated wall and additional cooling mechanisms can occur.…”