(a) Variation of moving distance for targeted systems with various contact angles as a function of Weber numbers.

(a) Variation of moving distance for targeted systems with various contact angles as a function of Weber numbers.

<p>(b) The snapshots of abnormal variation of moving distance at <i><i>We</i></i> = 43.49.</p>

Wedi'i Gadw mewn:

Manylion Llyfryddiaeth
Prif Awdur:	Liwei Sun (109973) (author)
Awduron Eraill:	Ye Han (261096) (author), Wei Shen (149127) (author), Chuiye Meng (22238251) (author), Baocheng Zhan (22238254) (author), Jiachao Gu (22238257) (author)
Cyhoeddwyd:	2025
Pynciau:	Biotechnology Biological Sciences not elsewhere classified Chemical Sciences not elsewhere classified observing free evolution intrinsic contact angles hysteretic bouncing dynamics various practical applications produce various outcomes xlink "> impingement important characteristic parameters exploring impacting systems impacting dynamics various conditions targeted systems practical application control outcomes asynchronous dynamics work reveals weber number suspened nanodroplets suspending droplets spreading behavior solid surface present work digital microfluidics coming ones central implementation central distances central distance binary nanodroplets
Tagiau:	Ychwanegu Tag Dim Tagiau, Byddwch y cyntaf i dagio'r cofnod hwn!

Eitemau Tebyg

Two interesting phenomena of systems with <i>D</i><sub>off</sub>=6.5 nm at (a) low Weber number of <i>We</i> = 18.15 and (b) high Weber number of <i>We</i> = 85.43.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Variation of spreading factor at (a) <i>We</i> = 18.15 and (b) <i>We</i> = 85.43, showing asymmetrical spreading as Weber number increases.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Variation of <i>τ</i><sub>c</sub> of targeted systems with <i>θ</i><sub>Y</sub> = 121° as a function of Weber numbers ranging from about 50 to 250.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

(a) Impacting nanodroplets upon anangled solid surface with increasing Young contact angle to <i>θ</i><sub>Y</sub> = 121°. (b) The variation of the spreading factor as a function of simulated time on the surface.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Snapshots of symmetrical spreading with the formation of the hole at the low off-central distance between two impacting nanodroplets at <i>We</i> = 277.25.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

(a) Free evolution of targeted system with <i><i>D</i></i><sub>off</sub>=1nm and <i>θ</i><sub>Y</sub> = 102° at <i><i>We</i></i> = 85.43.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

(a) Dynamic evolution of impacting binary nanodroplets with <i><i>D</i></i><sub>off</sub>=11nm upon a solid surface with <i>θ</i><sub>Y</sub> = 102° at <i><i>We</i></i> = 18.15.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Simulated system in MD simulations, containing two nanodroplets with a diameter of 8 nm and a solid metal surface comprised of Pt atoms.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Complete data file.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

(a) Variation of contact times as a function of impact <i>We</i> on solid surfaces with various Young contact angles ranging from <i>θ</i><sub>Y</sub> = 125° to <i>θ</i><sub>Y</sub> = 175° and (b) Variation in contact time of single droplets of equal volume under the same conditions.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Especial dynamics of impacting binary nanodroplets for breaking theory limitation of the contact time on superhydrophobic surface at <i>We</i> = 217.5.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

The breakup dynamics of (a) impacting binary droplets and (b) single droplet with controlling volume condition on superhydrophobic surfaces at <i>We</i> = 300. 24, and <i>We</i> = 170. 56.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

The velocity distribution within merged droplet up on surface with <i>θ</i><sub>Y</sub> = 155° at <i>We</i> = 217.5 at (a) <i>t</i> = 7 ps, (b) <i>t</i> = 16 ps, and (c) <i>t</i> = 21 ps.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Maximum spreading factors of impacting binary droplets for both (a) <i>β</i><sub>max, pre</sub> and (b) <i>β</i><sub>max, sec</sub> on solid surfaces with various <i>θ</i><sub>Y</sub> at <i>We</i> = 43.51 and 174.02 as a function of <i>We</i><sup>1/2</sup>.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Snapshots of impacting binary droplets on a superhydrophobic surfaces with <i>θ</i><sub>Y</sub> = 125° at <i>We</i> = 43.51 and 174.02.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Variation of dimensionless spreading factor versus simulated time starting from the secondary spreading at various <i>θ</i><sub>Y</sub> and <i>We.</i>
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Dynamic evolution of impacting binary nanodroplets on a hydrophohilic surface with <i>θ</i><sub>Y</sub> = 85° at (a) <i>We</i> = 4.84, (b) <i>We</i> = 77.34, and (c) <i>We</i> = 271.91.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Simulated configuration which contains two identical nanodroplets with radius of 4 nm and Pt solid surface are placed.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Complete data file.
gan: Liwei Sun (109973)
Cyhoeddwyd: (2025)

Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Cyhoeddwyd: (2025)

Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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Regimes and Breakup Model of Head-On Collisions of Unequal-Sized Water Nanodroplets
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