“…The theoretical surface heat flux, q'' (kw/m 2 ), can be calculated from coupling the individual droplet heat transfer function of their radius, q d (r), to the droplet number density N(r) as: [2,71]. Since typically during dropwise '' = ∫ ( ) ( ) condensation droplet growth takes place via direct condensation for small droplet with radius below the transition radius r e (r < r e ) and via droplet coalescence for droplets with radius above r e (r > r e ), the total heat flux for dropwise condensation without taking into account droplet shedding or sweeping is expressed as [19,79]: On one hand, the droplet size distribution above the transition radius N(r) can be extracted from Figure 5 or from the different coefficients reported in Table 2, while the droplet size distribution for droplets below the transition radius n(r) can be estimated from the expressions proposed by Graham and Griffith [8], Tanaka [73], Kim and Kim [19], Miljkovic et al [81], Wen et al [71], Chavan et al [18], and Alizadeh-Birjandi [82], amongst others. Nonetheless, in order to solely rely on our experimental data avoiding the use of empirical correlations, in this work we only make use of the N(r) reported in Figure 5 for droplets bigger than r e .…”