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significant decrease » significant increase (Expand Search), significantly increased (Expand Search)
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i decrease » _ decrease (Expand Search), a decrease (Expand Search), _ decreased (Expand Search)
significant decrease » significant increase (Expand Search), significantly increased (Expand Search)
significant i » significant _ (Expand Search), significant co (Expand Search), significant 17 (Expand Search)
i decrease » _ decrease (Expand Search), a decrease (Expand Search), _ decreased (Expand Search)
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4121
Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces
Published 2025“…The droplet extension on a concave surface follows the relation <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>We</i><sup>1/4</sup>. …”
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4122
Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces
Published 2025“…The droplet extension on a concave surface follows the relation <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>We</i><sup>1/4</sup>. …”
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4123
Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces
Published 2025“…The droplet extension on a concave surface follows the relation <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>We</i><sup>1/4</sup>. …”
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4124
Dynamics of Solid–Liquid Compound Droplets on Cylindrically Concave Superhydrophobic Surfaces
Published 2025“…The droplet extension on a concave surface follows the relation <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>f</i>(<i>We</i>, δ, Bo), and for a flat plate, when δ → 0, the correlation reduces to the established scaling law <i>D</i><sub><i>z</i></sub><sup>max</sup>/<i>D</i><sub>0</sub> ≈ <i>We</i><sup>1/4</sup>. …”
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4125
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4126
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4127
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4128
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4129
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4130
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4131
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4132
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4133
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4134
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4135
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4136
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4137
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4138
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4139
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4140