Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces حسب Niju K. Mohammed (22631779)

"…The generation of compound droplets through droplet–particle interactions has garnered significant attention due to its relevance in diagnostics, biomolecule encapsulation, functional coating, and targeted drug delivery. …"

Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces حسب Niju K. Mohammed (22631779)

"…The generation of compound droplets through droplet–particle interactions has garnered significant attention due to its relevance in diagnostics, biomolecule encapsulation, functional coating, and targeted drug delivery. …"

Impact of red blood cell-platelet ratio trajectories in the first four days before ICU admission on prognosis and clinical outcomes in the validation set. حسب Jie Zhao (49409)

Impact of red blood cell-platelet ratio trajectories on prognosis and clinical outcomes in the first four days before ICU admission in the training set. حسب Jie Zhao (49409)

Results for the asymmetric relationship between military expenditures and DOD energy consumption. حسب Ryan P. Thombs (9138968)

الموضوعات:

Coefficient plot of short-run effects. حسب Ryan P. Thombs (9138968)

الموضوعات:

Annual Difference in Energy Consumption Relative to Historical Median Change by 2032. حسب Ryan P. Thombs (9138968)

الموضوعات:

Coefficient plot of long-run effects. حسب Ryan P. Thombs (9138968)

الموضوعات:

Results for the asymmetric relationship between military expenditures and DOD energy consumption. حسب Ryan P. Thombs (9138968)

الموضوعات:

Time series of military expenditures and DOD energy consumption. حسب Ryan P. Thombs (9138968)

الموضوعات:

Classification of panels after the impact test. حسب Tek Raj Gyawali (20550560)

"…Panels reinforced with thinner PVA fibers exhibited superior performance in resisting compressive and impact loads. This enabled a reduction in fiber content to 1.2% (a 60% decrease) and panel thickness to 22 mm (a 4.35% decrease) compared to panels with thicker fibers. …"

Classification of panels after the impact test. حسب Tek Raj Gyawali (20550560)

"…Panels reinforced with thinner PVA fibers exhibited superior performance in resisting compressive and impact loads. This enabled a reduction in fiber content to 1.2% (a 60% decrease) and panel thickness to 22 mm (a 4.35% decrease) compared to panels with thicker fibers. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"

Effect of the Surface Peak–Valley Features on Droplet Impact Dynamics under Leidenfrost Temperature حسب Yunlong Jiao (6672764)

"…When the microtexture area occupancy is 50%, it is worth noting that the micropit and micropillar surfaces have nearly same roughness (<i>Sa</i>), but the Leidenfrost temperature was notably higher on the micropit surface with negative skewness (<i>Ssk</i> < 0), which was related to differences in vapor flow dynamics. We further find that the Weber number (<i>We</i>) significantly influences the Leidenfrost point, with the droplet impact wall behavior going through the states of film bounce back, ejecting tiny droplets and bounce back, and ultimately droplet breakup as the <i>We</i> increases. …"