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. 2020 Sep 1;32(9):094101. doi: 10.1063/5.0022858

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Copyright © 2020 Author(s)

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FIG. 7. — Influence of the R–T instability. (a) Acceleration of the thin liquid sheet (A) in m s⁻² as a function of Weber number (We). (b) Number of ligaments formed (N) as a function of Bond number (Bo). Here, $B o = \frac{ρ_{g} R_{b}^{2} A}{σ}$ . (b) signifies $N \sim \sqrt{B o}$ .