“…The phase diagram extends the phase diagram for isothermal droplet deposition (Ste = 0), determined experimentally by Ref. [67]. For the isothermal case, the simulated results agree reasonably well with previously obtained results.…”
Section: Regime Mapsupporting
confidence: 89%
“…For the isothermal case, the simulated results agree reasonably well with previously obtained results. A transition from the deposition to rebound is seen between 0.5 < We < 2, when the remaining kinetic energy in the droplet is sufficiently high to overcome surface and potential energy [67]. A transition into the rebound with ejection regime, when even higher kinetic energy remains in the retracting droplet, is seen between 11 < We < 13.5 here and at We = 14 in the experiments by Ref.…”
Section: Regime Mapsupporting
confidence: 55%
“…A transition into the rebound with ejection regime, when even higher kinetic energy remains in the retracting droplet, is seen between 11 < We < 13.5 here and at We = 14 in the experiments by Ref. [67]. The slight difference might be due to the slightly lower contact angle of 150°in the experiments.…”
Section: Regime Mapsupporting
confidence: 48%
“…• First, at slight surface undercooling, 0.1 < Ste < 0.4, similar to isothermal impact, for We < 4, complete deposition of the droplet on the surface takes place. This happens at We < 2 in the isothermal case [67]. There is not enough inertia for (partial) re-bounce to occur.…”
“…The phase diagram extends the phase diagram for isothermal droplet deposition (Ste = 0), determined experimentally by Ref. [67]. For the isothermal case, the simulated results agree reasonably well with previously obtained results.…”
Section: Regime Mapsupporting
confidence: 89%
“…For the isothermal case, the simulated results agree reasonably well with previously obtained results. A transition from the deposition to rebound is seen between 0.5 < We < 2, when the remaining kinetic energy in the droplet is sufficiently high to overcome surface and potential energy [67]. A transition into the rebound with ejection regime, when even higher kinetic energy remains in the retracting droplet, is seen between 11 < We < 13.5 here and at We = 14 in the experiments by Ref.…”
Section: Regime Mapsupporting
confidence: 55%
“…A transition into the rebound with ejection regime, when even higher kinetic energy remains in the retracting droplet, is seen between 11 < We < 13.5 here and at We = 14 in the experiments by Ref. [67]. The slight difference might be due to the slightly lower contact angle of 150°in the experiments.…”
Section: Regime Mapsupporting
confidence: 48%
“…• First, at slight surface undercooling, 0.1 < Ste < 0.4, similar to isothermal impact, for We < 4, complete deposition of the droplet on the surface takes place. This happens at We < 2 in the isothermal case [67]. There is not enough inertia for (partial) re-bounce to occur.…”
“…To date, much work has been conducted on the crushing characteristics of a droplet hitting a wall 5–7 . Researchers have studied the spreading movement of a single droplet through experimental phenomena and numerical simulations 8–10 . Rioboo 11 et al .…”
Exploring the behaviour of sprayed water droplets on dairy cow hair during the spraying process is of great significance to improve the effects of this process on cooling a dairy cow’s body. In this paper, we use a high-speed camera to examine the sprayed droplets of different diameters and then analyse the experimental results. The results show that the movements of sprayed droplets on the simulated dairy cow (SDC) surface can be divided into four categories: random scattering, aggregation, multiple deformations and flow slipping. Sprayed droplets with diameters of 0.56 mm and 0.8 mm exhibit more frequent random scattering than do other droplets. However, this behaviour is unfavourable for cooling the dairy cow body. By analysing the dimensionless parameter B, we find that sprayed droplets with a diameter of 1.1 mm, which have a higher frequency of aggregation, is not conducive for cooling the dairy cow body. However, multiple deformations can contribute to the cooling process of a SDC. By analysing the relationship between We and γ, we can find the range of We and γ in which the behaviour of random scattering and multiple deformations may appear more frequently. The results show that sprayed droplets with diameters of 0.8 mm–1.0 mm exhibit multiple deformations more frequently, which is beneficial for the cooling process of a SDC.
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