Interfacial Crystallization Within Liquid Marbles
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Article Interfacial Crystallization within Liquid Marbles Edward Bormashenko 1,* , Pritam Kumar Roy 1 , Shraga Shoval 2 and Irina Legchenkova 1 1 Chemical Engineering Department, Engineering Faculty, Ariel University, P.O. Box 3, Ariel 407000, Israel; [email protected] (P.K.R.); [email protected] (I.L.) 2 Industrial Engineering and Management Department, Engineering Faculty, Ariel University, P.O. Box 3, Ariel 40700, Israel; [email protected] * Correspondence: [email protected] Received: 25 September 2020; Accepted: 12 October 2020; Published: 15 October 2020 Abstract: We report interfacial crystallization in the droplets of saline solutions placed on superhydrophobic surfaces and liquid marbles filled with the saline. Evaporation of saline droplets deposited on superhydrophobic surface resulted in the formation of cup-shaped millimeter-scaled residues. The formation of the cup-like deposit is reasonably explained within the framework of the theory of the coffee-stain effect, namely, the rate of heterogeneous crystallization along the contact line of the droplet is significantly higher than in the droplet bulk. Crystallization within evaporated saline marbles coated with lycopodium particles depends strongly on the evaporation rate. Rapidly evaporated saline marbles yielded dented shells built of a mixture of colloidal particles and NaCl crystals. We relate the formation of these shells to the interfacial crystallization promoted by hydrophobic particles coating the marbles, accompanied with the upward convection flows supplying the saline to the particles, serving as the centers of interfacial crystallization. Convective flows prevail over the diffusion mass transport for the saline marbles heated from below. Keywords: interfacial crystallization; liquid marble; hydrophobic particle; superhydrophobic surface; coffee-stain effect 1. Introduction Interfacial crystallization has attracted much interest of scientists in the field of condensed matter in the past decades [1–6]. Interfacial crystallization enables intelligent control of the morphology of crystals, nucleated in the vicinity of solid/liquid [1–3] or liquid/liquid interfaces [4–6], and some unique crystalline structures have been obtained, including nano-whiskers [4] and hybrid shish–kebab and shish–calabash structures [1,2]. Interfacial crystallization allowed manufacturing of energetic nano-crystals [3] and porous particles [5]. The complicated physico-chemical mechanisms of the interfacial crystallization were addressed in [7–10]. We demonstrate in our communication that evaporated liquid marbles may be used for the interface-driven crystallization. Liquid marbles, introduced in the pioneering investigations of Quéré et al., are non-stick droplets coated with nano- or micron-sized particles, which are usually hydrophobic [11–15]. Liquid marbles are not hermetically coated by the solid particles. The respirability of liquid marbles makes them suitable for the cultivation of microorganisms and cells [16–20]. Liquid marbles may also be used as mini-reactors and bio-reactors [21,22]. Kinetics of the evaporation of liquid marbles was addressed in [23–26]. Use of liquid marbles for non-traditional computing was reported recently [27–30]. Liquid marbles may be actuated by UV and IR light and Marangoni flows [31–33], and demonstrate obvious potential for micro-fluidics applications [34,35]. Actually, liquid marbles opened new horizons for the researchers studying the liquid state of the matter. We report here the use of liquid marbles for controlled interfacial crystallization. Condens. Matter 2020, 5, 62; doi:10.3390/condmat5040062 www.mdpi.com/journal/condensedmatter Condens. Matter 2018, 3, x FOR PEER REVIEW 2 of 11 2. Results Condens. Matter 2020, 5, 62 2 of 11 We carried2. Results out comparative experiments in which droplets of aqueous NaCl solutions were evaporated underWe conditions carried out comparativeof superhydrophobicity experiments in which when droplets (i) ofnaked aqueous aqueous NaCl solutions NaCl were solution droplets were evaporatedevaporated when under placed conditions on ofsuperhydrophobic superhydrophobicity when surfaces, (i) naked aqueous and NaClwhen solution (ii) dropletsmarbles filled with were evaporated when placed on superhydrophobic surfaces, and when (ii) marbles filled with aqueous NaClaqueous solution NaCl and solution coated and coated with with lycopodi lycopodiumum powder powder (a strongly (a strongly hydrophobic hydrophobic yellow-tan yellow-tan dust-like powder,dust-like consisting powder, consisting of the ofdry the dryspores spores of of clubmoss plants) plants) were evaporated were ev whenaporated placed onwhen placed on superhydrophobicsuperhydrophobic substrates, substrates, as depicted as depicted in in Figure Figure1. 1. Figure 1. The evaporationFigure 1. The evaporation processes processes of aof naked a naked aqueous aqueous NaCl NaCl solution solution drop (a) anddrop a liquid (a) and marble a liquid marble filled with aqueous NaCl solution (b) placed on a superhydrophobic surface are depicted. filled with aqueous NaCl solution (b) placed on a superhydrophobic surface are depicted. When naked saline droplets are evaporated on superhydrophobic surfaces, very different scenarios of evaporation are possible, namely, the evaporation may take place under the pinned triple line, When nakedand under saline the slidingdroplets triple line,are asevaporated discussed in [36 on]. Thesuperhydrophobic evaporation may be accompanied surfaces, by very different scenarios of evaporationthe Cassie–Wenzel are wettingpossible, transition namely, and may the take evaporation place within themay Cassie take wetting place regime under [36, 37the]. pinned triple line, and underWe the studied sliding evaporation triple of line, the naked as discusse saline dropletsd in under [36]. ambient The evaporation conditions (t = 25 may◦C) and be also accompanied by under the constant temperature of the substrate of t = 70 ◦C. The characteristic time scales of evaporation the Cassie–Wenzelwere τev wetting 24 min fortransition the “slow” andandτev may 4 min take for the place rapid evaporationwithin the processes. Cassie wetting regime [36,37]. We studied evaporationBoth of temperature of the naked regimes suppliedsaline droplets very similar under results, namely, ambient evaporation conditions occurred ( undert = 25 °C) and also the slight variation in the apparent contact angle, i.e., 142◦ < θapp < 149◦, as shown in Figure2, under the constantwhereas thetemperature contact line was of strongly the pinnedsubstrate as demonstrated of t = in70 Movies °C. S1The and characteristic S2. The low contact time scales of evaporation wereangle hysteresis ≅ 24 and low slidingor f the angles “slow” inherent and for the pristine≅ 4 saline dropletsor f the demonstratedrapid evaporation that the processes. Both of temperatureinitial wetting regime regimes was thesupplied Cassie-like very one. Thesimilar wetting results, regime atnamely, which high evaporation apparent contact occurred under angles are accompanied with the pronounced pinning of the triple line is inherent for the so-called the slight variation“rose petal in e fftheect” [apparent37–40]. However, contact in our angle, experiments, i.e., the 142° situation was much 149° more, complicatedas shown in Figure 2, whereas the contactdue to the line crystallization was strongly of NaCl pinned occurring as in demonstrated a course of evaporation in Movie of the droplets, S1 and and Movie it is S2. The low reasonable to suggest that high pinning of the triple line arises from the high affinity of water to contact angle hysteresisNaCl crystals, and formed low in the sliding vicinity angles of the triple inherent line, as will for be the demonstrated pristine in saline detail below. droplets demonstrated that the initial wetting regime was the Cassie-like one. The wetting regime at which high apparent contact angles are accompanied with the pronounced pinning of the triple line is inherent for the so- called “rose petal effect” [37–40]. However, in our experiments, the situation was much more complicated due to the crystallization of NaCl occurring in a course of evaporation of the droplets, and it is reasonable to suggest that high pinning of the triple line arises from the high affinity of water to NaCl crystals, formed in the vicinity of the triple line, as will be demonstrated in detail below. Condens. Matter 2020, 5, 62 3 of 11 Condens. Matter 2018, 3, x FOR PEER REVIEW 3 of 11 Figure 2.2. (a) Change in the apparent contact angle in in the the course course of of evaporation evaporation of of a a 5 5 µLµL 25.9% 25.9% w/ww/w aqueous NaCl drop placed on a superhydrophobicsuperhydrophobic surface is shown; the temperature ofof evaporationevaporation tt = 25 °C.◦C. ((b)) Sketch Sketch demonstrating demonstrating that the formation of cup-shaped residue in a course evaporation of a naked aqueousaqueous NaClNaCl dropdrop placedplaced onon aa superhydrophobicsuperhydrophobic surfacesurface isis presented.presented. 3. Discussion Evaporation of saline droplets placed on a superhydrophobicsuperhydrophobic surface resulted in thethe formationformation of the cup-shaped millimeter-scaled residues, as as shown shown in in Figures Figures 11aa andand3 3aa andand MoviesMovies S1 S1 and S2, and was observed observed for for both both slow slow and and rapid rapid evaporation evaporation regimes. regimes. It seems It seems that that the theformation formation of this of thiscup-like cup-like deposit deposit may may