2016
DOI: 10.1017/jfm.2016.11
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Gravitational extension of a fluid cylinder with internal structure

Abstract: Motivated by the fabrication of microstructured optical fibres, a model is presented for the extension under gravity of a slender fluid cylinder with internal structure. It is shown that the general problem decouples into a two-dimensional surface-tension-driven Stokes flow that governs the transverse shape and an axial problem that depends upon the transverse flow. The problem and its solution differ from that obtained for fibre drawing, because the problem is unsteady and the fibre tension depends on axial p… Show more

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Cited by 12 publications
(16 citation statements)
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“…The velocity scale U is taken to be a representative axial velocity at the die exit related to the characteristic area and flux by Q = SU, while the time scale is L/U = LS/Q. In a typical preform extrusion the temperature varies with both position and time; however, as in previous work on fibre drawing (Stokes et al 2014;Buchak et al 2015;Chen et al 2015) and gravitational extension of a fluid cylinder (Tronnolone et al 2016), we assume that the temperature profile is known. The viscosity depends only on temperature so is thus assumed known and scaled µ = µ 0 µ * for some characteristic viscosity µ 0 .…”
Section: Formulationmentioning
confidence: 99%
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“…The velocity scale U is taken to be a representative axial velocity at the die exit related to the characteristic area and flux by Q = SU, while the time scale is L/U = LS/Q. In a typical preform extrusion the temperature varies with both position and time; however, as in previous work on fibre drawing (Stokes et al 2014;Buchak et al 2015;Chen et al 2015) and gravitational extension of a fluid cylinder (Tronnolone et al 2016), we assume that the temperature profile is known. The viscosity depends only on temperature so is thus assumed known and scaled µ = µ 0 µ * for some characteristic viscosity µ 0 .…”
Section: Formulationmentioning
confidence: 99%
“…A consequence of this is that the region above this, which is retained, may be considered slender for all times. Applying a slenderness approximation to the governing equations (2.1) and boundary conditions (2.2), in a similar manner to that of Tronnolone et al (2016) for a stretching cylinder, results in a one-dimensional model for the axial flow and a two-dimensional model for the transverse flow.…”
Section: Formulationmentioning
confidence: 99%
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