1882
DOI: 10.1080/14786448208628425
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XX. On the equilibrium of liquid conducting masses charged with electricity

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Cited by 1,656 publications
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“…Because the liquid is conductive, charge migration can occur up to the scission point (d sp ) at which the connection ruptures. For deriving eq 1, Rayleigh [32] assumed that fragmentation is triggered by shape oscillations. Droplet deformations were described in terms of spherical harmonics, and he concluded that the fragmentation channel having the lowest ⌬E ts is associated with quadrupole (prolate-oblate [9]) oscillations, whereas higher order deformations are less effective at mediating disintegration [42].…”
Section: Introductionmentioning
confidence: 99%
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“…Because the liquid is conductive, charge migration can occur up to the scission point (d sp ) at which the connection ruptures. For deriving eq 1, Rayleigh [32] assumed that fragmentation is triggered by shape oscillations. Droplet deformations were described in terms of spherical harmonics, and he concluded that the fragmentation channel having the lowest ⌬E ts is associated with quadrupole (prolate-oblate [9]) oscillations, whereas higher order deformations are less effective at mediating disintegration [42].…”
Section: Introductionmentioning
confidence: 99%
“…In addition, proposals for scenarios involving elements of both models have been put forward [30,31]. A solvent droplet is said to be at the Rayleigh limit when its net charge reaches a value Q R that is given by [1,32] where 0 is the permittivity of the vacuum, and ␥ is the surface tension. In the ESI-MS literature the relationship between Q R and droplet stability is often treated somewhat casually, using statements such as [33] "[it was] found that as the solvent evaporated the density of charges on the droplet surface would increase to a critical value, now known as the 'Rayleigh limit', at which Coulomb repulsion would overcome surface tension.…”
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confidence: 99%
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