“…As revealed by the X-ray computer tomography (CT) image of the pulled glass capillary in Fig. 1a, the inner diameter (r) versus the axial position (x) can be fitted by a catenary curve, 40 of the inner diameter, from ~ 180 μm (edge) to ~ 90 μm (center), are clearly visible (Fig. 1c).…”
Section: Sand's Time In Converging Channelsmentioning
Lithium metal penetrations through the liquid-electrolyte-wetted porous separator and solid electrolytes are a major safety concern of next-generation rechargeable metal batteries. The penetrations were frequently discovered to occur through only...
“…As revealed by the X-ray computer tomography (CT) image of the pulled glass capillary in Fig. 1a, the inner diameter (r) versus the axial position (x) can be fitted by a catenary curve, 40 of the inner diameter, from ~ 180 μm (edge) to ~ 90 μm (center), are clearly visible (Fig. 1c).…”
Section: Sand's Time In Converging Channelsmentioning
Lithium metal penetrations through the liquid-electrolyte-wetted porous separator and solid electrolytes are a major safety concern of next-generation rechargeable metal batteries. The penetrations were frequently discovered to occur through only...
“…Following the analysis of Bernoulli 12 and Freeman 20 (see Appendix S3 †), we concluded that the shape of a partially wet sample can be described as a combination of two catenaries continuously merging at the wetting front.…”
The classical Bernoulli problem of a freely hanging fabric sagged between two posts is used for the analysis of wicking phenomena. We show that wicking of a wetting liquid into a Bernoulli catenary is an instructive nontrivial experiment illustrating an unusual coupling between mechanical and capillary forces. When the liquid wicks into the material, it causes the catenary to sway back and forth. We studied theoretically and experimentally the kinetics of wicking into sagged nonwoven materials. The proposed experiment can be used for the analysis of transport and tensile properties of thin porous films.
“…The last situation can be achieved in experiments, where a freely suspended sample absorbs liquid from one end. For such situation, following the analysis of Bernoulli 19 and Freeman, 23 and integrating the second expression of Equation (3), 17 one can show that the sample profile can be defined using a combination of catenary equations describing dry and wet parts of the sample (Figure 1(b), inset):…”
Section: Fabric Profile and Forces Acting On Wet And Dry Partsmentioning
confidence: 99%
“…The shape of the freely sagged sample contains valuable information about forces F AE acting along the sample profile (Equation ( 4)). According to momentum balance 23 these forces are tangential to the sample profile and their magnitudes are proportional to the vertical coordinate y AE of the cross-section in question (Equation ( 4)). The coefficient of proportionality depends on the linear density of the sample AE , and the total tensile force at each cross-section consists of two components, F AE y , F AE x .…”
When a wetting liquid wicks into a fibrous material, it causes the material to deform. In this paper we discuss the elasto-capillary effect that leads to spontaneous internal stresses in the materials. The elasto-capillary effect produced by menisci in pores can be identified through a specific stress distribution in the fibrous matrix. We show that the classical Bernoulli problem of a freely hanging fabric can be used for the analysis of gravity-induced stresses in textile materials. These stresses change due to elasto-capillary effect. Wicking of a wetting liquid into a freely suspended fibrous material is shown to be an instructive nontrivial experiment illustrating interesting distinguishable stress distributions in the fibrous matrix.
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