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Table · dataset · 2026

Decoupling Wetting from Swelling in Electrospun Fibrous Mats: Predicting Saturation Time, Swelling Time, and Dimensional Change from Solubility Parameters

Listed in ZivaHub and Deakin Research Online — shown once because both records carry DOI 10.1021/acs.langmuir.6c05201.s001

Electrospun mats are used wet, yet the transition from the characterized dry mat to the functioning wet one is rarely quantified.

Description

The Hansen solubility parameters of a polymer and a liquid generate two distinct metrics rather than one, and so two independent gates: the Flory–Huggins parameter follows from the Hansen distance, while the polymer–liquid interfacial tension collapses <b>exactly</b> onto a second squared distance on volume-scaled coordinates, weighting dispersion differently by 4<i>β</i> ≈ 2.5.

Wetting and swelling are consequently separable, and four regimes exist rather than two. The pore-scale Laplace pressure and a Kozeny–Carman permeability reduce capillary imbibition to one coefficient, <i>D</i><sub>imb</sub> = <i>ε</i><sub>0</sub><i>R</i><sub>f</sub><i>σ</i> cos <i>θ</i>/[<i>k</i><sub>K</sub>(1 – <i>ε</i><sub>0</sub>)<i>μ</i>], which saturates a mat through its thickness in 10 to 50 ms. Fiber orientation makes in-plane wicking anisotropic, so an aligned mat wets into an ellipse of axis ratio √2.

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A closed gate instead imposes a 14 kPa intrusion pressure; the mat stays dry unless the interior drive is favorable, in which case it resists a droplet yet imbibes once entry has occurred. Fiber swelling completes within 10<sup>2</sup> s, and a jamming argument closes the dimensional-change problem, giving a porosity linear in the fiber swelling ratio and an exact decomposition of gravimetric uptake into network and void terms.

Against published data, a cellulose acetate (CA) mat-and-film pair returns a mat porosity of 0.90 with no adjustable parameter, and a cross-linked poly(vinyl alcohol) (PVA) series a monotonic cross-link density reproducing the reported cross-linker ranking. A swelling ratio reported without the dry porosity is not interpretable: for one hydrophilic mat, 54% of the uptake is capillary water between the fibers, not water in the polymer.

Two independent datasets test the two branches separately: the wetting gate against poly(ε-caprolactone) (PCL) mats that absorb a water droplet completely despite an apparent contact angle of 137.9°, and the Kozeny–Carman baseline against absolute permeability measurements on poly(lactic acid) (PLA) scaffolds several times coarser in fiber diameter. The framework applies unmodified to microfluidic and tissue-engineering scaffolds as well as to wound dressings, drug-releasing membranes, separators and filtration media.

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Provenance · 2 source records, 15 field assertions
SourceKeyLast seenRaw
ZivaHuboai:figshare.com:article/3403118612 d agoJSON v1
Deakin Research Onlineoai:figshare.com:article/3403118612 d agoJSON v1
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