“…In particular, the deposition and subsequent spreading without forming a crown shape is a basic behavior of droplet impingement on solid surfaces. Theoretical, empirical, and semi-empirical relations that describe this process have been proposed in previous research [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] to predict the maximum spreading factor β m , defined as the ratio d max /d 0 , where d max is the maximum spreading diameter and d 0 is the initial droplet diameter. Correlations between β m , Weber number We (=ρ l u 2 d 0 /σ lg , where ρ l , u, d 0 , and σ lg represent the liquid density, impinging velocity, initial droplet diameter, and surface energy density of the liquid, respectively) and Reynolds number Re (=ρ l ud 0 /µ l , where µ l is the viscosity of the liquid) are mainly discussed considering the balance between the inertia, viscosity, and capillary effects [3,8,9,[22][23][24].…”