Evidence map›Paper›PMID 27375826›Full record

ArticleBiomicrofluidics2016

AC electrified jets in a flow-focusing device: Jet length scaling.

Elena Castro-Hernández, Pablo García-Sánchez, Javier Alzaga-Gimeno, Say Hwa Tan, Jean-Christophe Baret, Antonio Ramos

Abstract read
In one paragraph

Article in Biomicrofluidics, 2016. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 6 papers.

0numbers the graph read from it
0cells of the map it votes in
6citing papers in PubMed
–field-weighted citation impact
1 · What the graph read from it

What it found

Each row is one number read from the abstract, on the scale the paper reported it, with its interval. Left of the dashed line favours the treatment, right favours the comparator. Under each row is the sentence it came from. New to these charts? A ten-minute tutorial.

The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

2 · The registry

The trial behind it

Trials whose registry record cites this paper, or whose number appears in the abstract. A trial that started after this paper was published is citing it as background, not reporting it.

Neither the registry nor the abstract names a trial number. If this is a trial report, that itself is worth knowing.

3 · Its place in the literature

Who cites it

6 citing papers in PubMed.

  1. Article
  2. Review
  3. Review
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4 · The record

Corrections and comments

PubMed lists nothing against this paper. Absence here is not a guarantee, only a check that was made.

5 · Who and what money

Authors and funding

6 authors.

Elena Castro-HernándezÁrea de Mecánica de Fluidos, Departamento de Ingeniería Aeroespacial y Mecánica de Fluidos, Universidad de Sevilla , Avenida de los Descubrimientos s/n, 41092 Sevilla, Spain.ORCID 0000-0002-9990-1161
Pablo García-SánchezDepartamento de Electrónica y Electromagnetismo, Facultad de Física, Universidad de Sevilla , Avenida de Reina Mercedes s/n, 41012 Sevilla, Spain.
Javier Alzaga-GimenoÁrea de Mecánica de Fluidos, Departamento de Ingeniería Aeroespacial y Mecánica de Fluidos, Universidad de Sevilla , Avenida de los Descubrimientos s/n, 41092 Sevilla, Spain.
Say Hwa TanQueensland Micro- and Nanotechnology Centre, Griffith University , Brisbane QLD 4111, Australia.ORCID 0000-0002-9764-7868
Jean-Christophe BaretCNRS, Univ. Bordeaux , CRPP, UPR 8641, Soft Micro Systems, 115 Avenue Schweitzer, 33600 Pessac, France and Max-Planck Institute for Dynamics and Self-Organization, Droplets, Membranes and Interfaces, Am Fassberg 17, DE-37077 Goettingen, Germany.
Antonio RamosDepartamento de Electrónica y Electromagnetismo, Facultad de Física, Universidad de Sevilla , Avenida de Reina Mercedes s/n, 41012 Sevilla, Spain.ORCID 0000-0002-2190-1188

Funding

European Research Council 306385
6 · The paper itself

Abstract

We use a microfluidic flow-focusing device with integrated electrodes for controlling the production of water-in-oil drops. In a previous work, we reported that very long jets can be formed upon application of AC fields. We now study in detail the appearance of the long jets as a function of the electrical parameters, i.e., water conductivity, signal frequency, and voltage amplitude. For intermediate frequencies, we find a threshold voltage above which the jet length rapidly increases. Interestingly, this abrupt transition vanishes for high frequencies of the signal and the jet length grows smoothly with voltage. For frequencies below a threshold value, we previously reported a transition from a well-behaved uniform jet to highly unstable liquid structures in which axisymmetry is lost rather abruptly. These liquid filaments eventually break into droplets of different sizes. In this work, we characterize this transition with a diagram as a function of voltage and liquid conductivity. The electrical response of the long jets was studied via a distributed element circuit model. The model allows us to estimate the electric potential at the tip of the jet revealing that, for any combination of the electrical parameters, the breakup of the jet occurs at a critical value of this potential. We show that this voltage is around 550 V for our device geometry and choice of flow rates.

Identifiers

PMID27375826
PMCPMC4912565

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.