TY - JOUR
T1 - Viscous droplets impact on rough surfaces
AU - Liu, Lihui
AU - Cai, Guobiao
AU - Jiang, Bohan
AU - He, Bijiao
AU - Tsai, Peichun Amy
N1 - Publisher Copyright:
© 2025 The Authors
PY - 2025/11
Y1 - 2025/11
N2 - We experimentally investigate the dynamics of viscous droplets impacting on rough surfaces under a broad range of Weber number (2≤We≤1,194), Ohnesorge number (0.002≤Oh≤2.630), and average surface roughness (9.7μm≤Ra≤19.5μm). Three primary impact outcomes—jetting, spreading, and splashing—are observed. Our findings reveal that surface roughness promotes splashing by amplifying perturbations, while liquid viscosity counters this effect by dissipating the kinetic energy of the advancing lamella. We empirically describe the splashing threshold with the relation as OhReχ(Ra)=K(Ra), where the fitting parameter K(Ra) increases and χ(Ra) decreases with greater surface roughness. Moreover, the maximum spreading factor (βm), defined as the ratio of the droplet's maximum spreading diameter to its initial diameter, shows a pronounced dependence on surface roughness in low-viscosity conditions (Oh<0.050), but this dependence diminishes in high-viscosity regimes (Oh≥0.050). This trend results from the interplay between viscous dissipation induced by surface roughness and the intrinsic liquid viscosity. In the low-viscosity regime, the experimental βm is consistent with the empirical scaling law of βm=a(We/Oh)b, with the fitting constants, a and b, varying with surface roughness and liquid properties. In the regime of 0.050m approximates (We/Oh)1/6. These findings elucidate the significant role of surface roughness and liquid viscosity in governing droplet impact dynamics and spreading.
AB - We experimentally investigate the dynamics of viscous droplets impacting on rough surfaces under a broad range of Weber number (2≤We≤1,194), Ohnesorge number (0.002≤Oh≤2.630), and average surface roughness (9.7μm≤Ra≤19.5μm). Three primary impact outcomes—jetting, spreading, and splashing—are observed. Our findings reveal that surface roughness promotes splashing by amplifying perturbations, while liquid viscosity counters this effect by dissipating the kinetic energy of the advancing lamella. We empirically describe the splashing threshold with the relation as OhReχ(Ra)=K(Ra), where the fitting parameter K(Ra) increases and χ(Ra) decreases with greater surface roughness. Moreover, the maximum spreading factor (βm), defined as the ratio of the droplet's maximum spreading diameter to its initial diameter, shows a pronounced dependence on surface roughness in low-viscosity conditions (Oh<0.050), but this dependence diminishes in high-viscosity regimes (Oh≥0.050). This trend results from the interplay between viscous dissipation induced by surface roughness and the intrinsic liquid viscosity. In the low-viscosity regime, the experimental βm is consistent with the empirical scaling law of βm=a(We/Oh)b, with the fitting constants, a and b, varying with surface roughness and liquid properties. In the regime of 0.050m approximates (We/Oh)1/6. These findings elucidate the significant role of surface roughness and liquid viscosity in governing droplet impact dynamics and spreading.
KW - Drop impact
KW - Maximum spreading diameter
KW - Rough surface
KW - Splashing
KW - Viscous droplet
UR - https://www.scopus.com/pages/publications/105010523994
U2 - 10.1016/j.ijmultiphaseflow.2025.105345
DO - 10.1016/j.ijmultiphaseflow.2025.105345
M3 - 文章
AN - SCOPUS:105010523994
SN - 0301-9322
VL - 192
JO - International Journal of Multiphase Flow
JF - International Journal of Multiphase Flow
M1 - 105345
ER -