TY - JOUR
T1 - Dynamics of oil droplet impacting and wetting on the inclined surfaces with different roughness
AU - Wang, Lingzi
AU - Feng, Jianmei
AU - Dang, Tiendat
AU - Peng, Xueyuan
N1 - Publisher Copyright:
© 2020
PY - 2021/2
Y1 - 2021/2
N2 - This study experimentally investigated the wetting process of an oil droplet impacting on the dry surface with different surface roughness (0.3 μm, 1.6μm, 2.9μm, 5.2 μm) from the front view. Experiments were conducted under three impacting Weber ranges with the inclined angles of 37.0°, 63.0°, and 75.5°. The droplet spread as a ‘pancake’ on the surface when the inclination angle was 37.0°, while the shape of an ‘avocado’ of the flowing oil layer was observed on higher inclined angle surfaces. The upper part of the ‘avocado’ became narrower when the inclined angle increased from 63.0° to 75.5°, which then grew longer with the increase in the impact We. The normalized transverse and longitudinal spreading displacement βxand βywere defined, whose evolution with normalized time was then obtained. Three stages of the βxwere divided and analyzed. Under the same We range and inclined angle, the largest value of the maximum normalized droplet transverse spreading displacement (βxmax) was obtained with the smoothest surface (0.3 μm) followed by the roughest surface (5.2 μm). βxmaxwas affected by the surface roughness, which also influences the contact angle of the surface. When the surface roughness and the contact angle were regarded as two separate factors, it was found that for the transverse spreading, the lower the inclined angle, the more obvious effect of the surface roughness than that of the contact angle.
AB - This study experimentally investigated the wetting process of an oil droplet impacting on the dry surface with different surface roughness (0.3 μm, 1.6μm, 2.9μm, 5.2 μm) from the front view. Experiments were conducted under three impacting Weber ranges with the inclined angles of 37.0°, 63.0°, and 75.5°. The droplet spread as a ‘pancake’ on the surface when the inclination angle was 37.0°, while the shape of an ‘avocado’ of the flowing oil layer was observed on higher inclined angle surfaces. The upper part of the ‘avocado’ became narrower when the inclined angle increased from 63.0° to 75.5°, which then grew longer with the increase in the impact We. The normalized transverse and longitudinal spreading displacement βxand βywere defined, whose evolution with normalized time was then obtained. Three stages of the βxwere divided and analyzed. Under the same We range and inclined angle, the largest value of the maximum normalized droplet transverse spreading displacement (βxmax) was obtained with the smoothest surface (0.3 μm) followed by the roughest surface (5.2 μm). βxmaxwas affected by the surface roughness, which also influences the contact angle of the surface. When the surface roughness and the contact angle were regarded as two separate factors, it was found that for the transverse spreading, the lower the inclined angle, the more obvious effect of the surface roughness than that of the contact angle.
KW - Droplet impact
KW - contact angle
KW - inclined angle
KW - surface roughness
KW - transverse spreading
KW - wetting dynamics
UR - https://www.scopus.com/pages/publications/85096190610
U2 - 10.1016/j.ijmultiphaseflow.2020.103501
DO - 10.1016/j.ijmultiphaseflow.2020.103501
M3 - 文章
AN - SCOPUS:85096190610
SN - 0301-9322
VL - 135
JO - International Journal of Multiphase Flow
JF - International Journal of Multiphase Flow
M1 - 103501
ER -