Gao Xuefeng Wetting JPCL 2014

Ecient Self-Propelling of Small-Scale Condensed Microdrops byClosely Packed ZnO NanoneedlesJian Tian,, Jie Zhu, Hao-Yuan Guo, Juan Li, Xi-Qiao Feng, and Xuefeng Gao*,

Advanced Thermal Nanomaterials and Devices Research Group, Nanobionic Division, Suzhou Institute of Nano-Tech andNano-Bionics, Chinese Academy of Sciences, Suzhou 215123, Peoples Republic of ChinaDepartment of Engineering Mechanics, Tsinghua University, Beijing 100084, Peoples Republic of ChinaUniversity of Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing 100049, Peoples Republic of China

*S Supporting Information

ABSTRACT: Realizing the ecient self-propelling of small-scale condensed microdropsis very challenging but extremely important to design and develop advanced condensationheat transfer nanomaterials and devices, for example, for power generation and thermalmanagement. Here, we present the ecient self-propelling of small-scale condensedmicrodrops on the surface of closely packed ZnO nanoneedles, as-synthesized by facile,rapid, and inexpensive wet chemical crystal growth followed by hydrophobic modication.Compared with at surfaces, the nanostructured surfaces with the same low-surface-energychemistry possess far higher time-averaged density of condensed droplets at themicroscale, among which those with diameters below 10 m occupy more than 80% ofthe total drop number of residual condensates. Theoretical analyses clearly reveal that thisremarkable property should be ascribed to the extremely low solidliquid adhesion of thesurface nanostructure, where excess surface energy released from the coalescence ofsmaller condensed microdrops can be sucient to ensure the self-propelled jumping ofmerged microdrops.

SECTION: Surfaces, Interfaces, Porous Materials, and Catalysis

Condensed microdrop self-propelling surfaces have at-tracted great interest due to their values in basic researchand technological innovations, for example, enhancingcondensation heat transfer for high-eciency power generationand thermal management.13 The self-propelling of condensedmicrodrops on the nanostructured surfaces can be realized byexcess surface energy released from their mutual coalescencewithout requiring external forces such as gravity and steamshear force.4 In principle, the self-propelling of condensedmicrodrops can reduce heat resistance and increase renewalfrequency (performing more cycles of nucleation, growth, anddeparture per unit area), which is useful to enhance the totaldropwise condensation heat transfer performance.3 Recently,great breakthrough has been made in realizing the self-propelling of condensed microdrops with random diameterdistribution from tens to hundreds of micrometers by dierentmaterials of nanostructures513 and hierarchical struc-tures4,1417 modied with low-surface-energy chemicals.Compared with the costly top-down nanofabrication meth-ods,47,14,15 the bottom-up wet chemical nanosynthesismethods813,17 show obvious advantages in low-cost large-area processing and equipment accessibility. However, it is stilla great challenge to realize the high-eciency self-propelling ofsmall-scale (e.g.,

C for 30 min (see the Experimental Methods section). Theseself-standing ZnO nanoneedles are arranged in a closely packedway, having the characteristic interspace (p) of 60 17.1 nm,top diameter (dt) of 20.3 4.8 nm, end diameter of 98.3 5.5nm, and height of 2.85 0.14 m. The controllable synthesisof tapered nanoneedles with minimized top areas is based onthe principle of diusion-limited wet chemical crystal growth ina strong alkali system, where zinc ions can be rapidly consumedby violent reactions in the bulk to oer the chance of adjustingthe diusion rate of growth units transported to crystal facets ata proper growth condition of reaction temperature, time, and

concentration.18 Accordingly, we can easily obtain large-areaZnO nanoneedle lms in a short duration.Our experiments demonstrate that the as-synthesized

nanostructured surfaces own a remarkable condensed micro-drop self-propelling property after modifying low-surface-energy uorosilane molecules. Figure 2a and b shows distinctdropwise condensation behavior of the nanostructured surfaceand the contrast at surface, which are taken at the substratetemperature of 1 C, ambient temperature of 25 C, andrelative humidity of 90%. It is evident that condensates on thenanostructured surface can continuously emerge, grow, andself-departure, always keeping their sizes at the micrometerscale (Figure 2a). With the time extending, the drop numberdensity of condensates presents a rst decreasing and thenuctuating trend. In contrast, condensates on the at surfacecan continuously grow, accompanied by their sizes increasingfrom the micrometer scale to the millimeter (Figure 2b), andonly can slide o under gravity as their diameters reach thecapillary length (see Supporting Information Figure S1). Nodoubt that the aligned nanoneedles can dramatically reduce theresidence durations and diameters of condensed dropletsthrough self-departure.To better oer insight into the self-propelling phenomena of

condensates at the microscale, we investigate their details usinghigh-speed, high-resolution three-dimensional optical micro-scopic imaging technology (Keyence VW-9000). Figure 2cshows representative optical top views of the self-departureinstant of several small-scale condensed microdrops on thesurface of vertically placed nanostructured samples. Thejumping events are realized by the in-plane coalescence ofadjacent quasi-static microdrops, which is implemented by theirrespective growth due to preferential condensation of ambientvapor on the surface of microdrops.19 As shown in Figure 2d,the merged microdrop can eject from the nanostructuredsurface and then fall along a parabolic trajectory. It should be

Figure 1. SEM top view (top) and side view (bottom) of the as-synthesized ZnO nanoneedles.

Figure 2. Time-lapse optical images showing distinct dropwise condensation behaviors of the nanostructured surface (a) and the contrast at surface(b). Optical top views (c) and side view (d) showing the typical coalescence-induced self-propelling details of condensed microdrops on thenanostructured surface. All images are taken on the vertically placed sample surfaces.

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pointed out that for the horizontally placed nanostructuredsamples, the ejected microdrops can fall back to the samplesurface and trigger the new dynamic impact-inducedcoalescence events, resulting in continuously coalescence-induced jumping events (see Supporting Information FigureS2), with their diameters scaling up from micrometers tosubmillimeters. In fact, the continuous jumping events arenonexistent for the vertically placed nanostructured samplesbecause the ejected microdrops no longer fall on their surface.To quantify and highlight the intrinsic dropwise condensa-

tion performance of our nanosamples at the microscale, wefurther analyze the drop number distribution of residencemicrodrops with diameters (d) of 50 m canform only after 500 s, where their maximum fraction is notmore than 10%. In contrast, the sizes of condensates on the atsurface can rapidly increase over 100 m during very shortduration (e.g., 200 s). Besides, condensates with sizes from themicrometer size to the millimeter cannot jump on the atsurface even after mutual coalescence (see SupportingInformation Figure S1). Compared with the contrast atsurfaces, the aligned nanoneedle lms can eciently control thesizes of condensates at the microscale, especially below 10 m,in which the drop number distribution is larger than 80%during the whole condensation process. It should also bepointed out that, compared with the previously reported casespresenting similar data descriptions,4,1012,1417,20 our nano-structured samples possess the apparently higher time-averageddensity of small-scale condensed microdrops, to the best of ourknowledge.In principle, the self-propelling dynamics of merged

microdrops is governed by the balance of released surfaceenergy (Es), kinetic energy (Ek), viscous ow-induceddissipation energy (Evis), and interfacial adhesion-induced

dissipation energy (Eint), obeying the expression Ek = Es Evis Eint.2022 The gravitational potential energy may beneglected for the condensed microdrops with diameters farsmaller than the capillary length (LV/g)

0.5 2.7 mm, whereLV is the liquidvapor interface tension (0.075 N m1 at 5C). To simplify theoretical analysis, we only consider themerged case of two static microdrops with the same diameter(D) and apparent contact angle () as a model (note that thisanalysis method is also applicable to the coalescence process ofmultiple condensed microdrops after modication). As shownin Figure 4a, the quasi-static condensed microdrops can

gradually grow until closing to each other. Once the mergingevent occurs (Figure 4b), the excess surface energy wouldrelease, following Es LVA, where A is the dierence ofsurface area. It is known that Evis D1.5LV0.5/0.5, where isthe water viscosity and is the water density.23 Exemplied byD = 10 m, we can obtain Es 1 1011 J and Evis 6 1012J. Thus, to ensure the jumping of merged microdrops, thekinetic energy (Ek) must be positive, which means Eint < 4 1012 J.Our previous studies have indicated that surface adhesion of

superhydrophobic nanostructures is determined by theirgeometrical morphologies and solidliquid contact ways.24,25As shown in Figure 4c and d, the retracting and detachingprocess of microscopic water lms on the tops of alignednanoneedles is governed by the liquidsolid van der Waalsattraction24 and line tension.26 Accordingly, we can obtain Eint 0.25D2 sin2( )(1 + cos )LV(dt/p)2 + 0.252D2 sin2(

Figure 3. Drop number distribution of condensed microdrops withdiameters (d) of 0,where Ek is the kinetic energy of the jumping microdrop, Es thereleased surface energy, Evis the viscous ow-induced energydissipation, and Eint the interfacial adhesion-induced energydissipation. (c) A magnied image (corresponding to the blackrectangle in panel b) showing the retracting and detaching process ofwater lms on the top of nanoneedles (with a characteristic topdiameter of dt and interspace of p) in the coalescence-induced jumpinginstant. (d) Schematic of the top of a single nanoneedle contactingwith water, where surface adhesion comes from solidliquid van derWaals attraction and line tension.

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)(dt/p2) + 2D sin( )(dt/p), where is the apparentcontact angle of the condensed microdrop, the advancedcontact angle of water in contact with the silane modied atsurface (125), dt the top diameter of the nanoneedles, p theinterspace, and the line tension with the value of 4 1010 Jm1 for the top size of 20 nm (for the detailed deduction, seeSupporting Information section S3).26 Clearly, the Eint value isclosely related to the top diameter and interspace of thenanoscale building blocks. In this case of dt = 20 nm and p = 60nm, the calculated Eint is 3 1013 J, which is an order ofmagnitude lower than the requirement of 1012 J. Therefore,Eint is suciently low to ensure the ecient self-departure ofcondensed microdrops with a diameter of 10 m, poweringby excess surface energy released from their coalescence. Notethat the minor inconsistency with experimental ndings that asmall quantity (10 m) can still be resident on thenanostructure surface should be ascribed to the nonuniformityof characteristic interspaces and top diameters of the as-synthesized ZnO nanoneedles. Besides, our calculationindicated that the contributions of the van der Waals attractionand line tension to Eint occupied 70 and 30%, respectively.Accordingly, to realize more ecient self-propulsion, ones needto tailor a more delicate structure with reduced dt and increasedp for ensuring the lower adhesion of condensed microdrops in asuspended Cassie state.In summary, we report a type of closely packed ZnO

nanoneedles with ecient self-propelling function of small-scale condensed microdrops, which can be fabricated by veryfacile, rapid, and inexpensive wet chemical crystal growthfollowed by hydrophobic treatment. In contrast to the atsurfaces and previous reports, our samples can eectivelycontrol the diameters of condensates at the microscale,especially below 10 m with a drop number distribution ofmore than 80%. This striking property is ascribed to theminimal solidliquid adhesion of closely packed nanoneedles,where excess surface energy released from the coalescence ofsmaller condensed microdrops can be sucient to ensure theself-propelling of merged microdrops. These ndings aresignicant to develop novel microscale self-propelling dropwisecondensation surfaces toward applications in high-eciencyheat transfer devices13 and functional coatings, for example,moisture self-cleaning27 and subcooled water antifreezing.2831

EXPERIMENTAL METHODSSample Preparation. Arrayed ZnO nanoneedles were rapidlysynthesized by facile chemical bath deposition. To removeorganic contaminants, glass slides with the sizes of 2 cm 2 cmwere rst ultrasonically rinsed in acetone, ethanol, anddeionized water for 20 min and subsequently dried by N2ow. Then, the cleaned glass slides were coated with crystalseeds through dip-coating in an ethanol solution of zinc acetate(0.005 mol L1) followed by annealing at 350 C for 20 min,which were repeated three times for obtaining the uniformseeding layers. Aligned nanoneedles were obtained byimmersing the seeded glass slides in the aqueous solution of0.5 mol L1 zinc nitrate hexahydrate and 4 mol L1 sodiumhydroxide (V:V = 1:1) at 60 C for 30 min, where the seededfaces were set downward. After rinsing with water and dryingby N2 ow, all nanostructured samples and contrast glass slideswere immersed in the 1.0 wt % ethanol solution ofheptadecauorodecyltrimethoxysilane (Shin-Etsu Chemical

Co., Japan) for 2 h at room temperature and then taken outto heat at 80 C for 1 h.Structure and Property Characterization. The as-synthesized

nanostructures were observed using a high-resolution scanningelectronic microscope (Hitachi S4800, Japan). The high-speedcharge-coupled device camera (CCD) of the Motion AnalysisMicroscope system (Keyence VW-9000, Japan) was used forobserving the rapid behaviors of microdrops under magnica-tions of 301000 with frame rates of 304000 fps. Thesamples were fastened on the cooling stage (1 C) at thecontrolled environment of an ambient temperature of 25 Cand relative humidity of 90%. The sample stage, CCD, andlight source were set coaxially in the optic path, where the CCDholder could be rotated for capturing the top views, tilted views,and side views of optical images and video. A special measureusing optical grating structure lms as substrates and 45-tiltedillumination was used for capturing the images in Figures 2, S1,and S2 (Supporting Information), which enhance the stereo-scopic and colorful eects of condensed microdrops tohighlight the distinction of two condensation modes.

ASSOCIATED CONTENT*S Supporting InformationDetailed dropwise condensation dynamics on the verticallyplaced at surface (Figure S1) and the horizontally placednanostructured surface (Figure S2) and detailed deduction ofinterfacial adhesion-induced dissipation energy (section S3) areincluded. This material is available free of charge via theInternet at http://pubs.acs.org.

AUTHOR INFORMATIONCorresponding Author*E-mail: xfgao2007@sinano.ac.cn.NotesThe authors declare no competing nancial interest.

ACKNOWLEDGMENTSThis work was supported by the National Basic ResearchProgram of China (2012CB933202, 2012CB934101,2013CB933033), the Key Research Program of the ChineseAcademy of Sciences (KJZD-EW-M01), and SINANO, CAS.

REFERENCES(1) Boreyko, J. B.; Zhao, Y. J.; Chen, C.-H. Planar Jumping-DropThermal Diodes. Appl. Phys. Lett. 2011, 99, 234105.(2) Miljkovic, N.; Wang, E. N. Condensation Heat Transfer onSuperhydrophobic Surfaces. MRS Bull. 2013, 38, 397406.(3) Miljkovic, N.; Enright, R.; Wang, E. N. Modeling andOptimization of Superhydrophobic Condensation. J. Heat Transfer2013, 135, 111004.(4) Chen, C.-H.; Cai, Q.; Tsai, C.; Chen, C.-L.; Xiong, G.; Yu, Y.;Ren, Z. Dropwise Condensation on Superhydrophobic Surfaces withTwo-Tier Roughness. Appl. Phys. Lett. 2007, 90, 173108.(5) Dorrer, C.; Ruhe, J. Wetting of Silicon Nanograss: FromSuperhydrophilic to Superhydrophobic Surfaces. Adv. Mater. 2008, 20,159163.(6) Miljkovic, N.; Enright, R.; Wang, E. N. Effect of DropletMorphology on Growth Dynamics and Heat Transfer duringCondensation on Superhydrophobic Nanostructured Surfaces. ACSNano 2012, 6, 17761785.(7) Enright, R.; Miljkovic, N.; Al-Obeidi, A.; Thompson, C. V.;Wang, E. N. Condensation on Superhydrophobic Surfaces: The Roleof Local Energy Barriers and Structure Length Scale. Langmuir 2012,28, 1442414432.

The Journal of Physical Chemistry Letters Letter

dx.doi.org/10.1021/jz500798m | J. Phys. Chem. Lett. 2014, 5, 208420882087

(8) Miljkovic, N.; Preston, D. J.; Enright, R.; Wang, E. N.Electrostatic Charging of Jumping Droplets. Nat. Commun. 2013, 4,2517.(9) Dietz, C.; Rykaczewski, K.; Fedorov, A. G.; Joshi, Y. Visualizationof Droplet Departure on a Superhydrophobic Surface and Implicationsto Heat Transfer Enhancement during Dropwise Condensation. Appl.Phys. Lett. 2010, 97, 033104.(10) Feng, J.; Qin, Z.; Yao, S. Factors Affecting the SpontaneousMotion of Condensate Drops on Superhydrophobic Copper Surfaces.Langmuir 2012, 28, 60676075.(11) Feng, J.; Pang, Y.; Qin, Z.; Ma, R.; Yao, S. Why CondensateDrops Can Spontaneously Move Away on Some SuperhydrophobicSurfaces but Not on Others? ACS Appl. Mater. Interfaces 2012, 4,66186625.(12) Enright, R.; Miljkovic, N.; Dou, N.; Nam, Y.; Wang, E. N.Condensation on Superhydrophobic Copper Oxide Nanostructures. J.Heat Transfer 2013, 135, 091304.(13) Miljkovic, N.; Enright, R.; Nam, Y.; Lopez, K.; Dou, N.; Sack, J.;Wang, E. N. Jumping-Droplet-Enhanced Condensation on ScalableSuperhydrophobic Nanostructured Surfaces. Nano Lett. 2012, 13,179187.(14) Chen, X.; Wu, J.; Ma, R.; Hua, M.; Koratkar, N.; Yao, S.; Wang,Z. Nanograssed Micropyramidal Architectures for ContinuousDropwise Condensation. Adv. Funct. Mater. 2011, 21, 46174623.(15) Rykaczewski, K.; Paxson, A. T.; Anand, S.; Chen, X.; Wang, Z.;Varanasi, K. K. Multimode Multidrop Serial Coalescence Effectsduring Condensation on Hierarchical Superhydrophobic Surfaces.Langmuir 2013, 29, 881891.(16) Boreyko, J. B.; Chen, C.-H. Self-Propelled DropwiseCondensate on Superhydrophobic Surfaces. Phys. Rev. Lett. 2009,103, 184501.(17) He, M.; Zhang, Q.; Zeng, X.; Cui, D.; Chen, J.; Li, H.; Wang, J.;Song, Y. Hierarchical Porous Surface for Efficiently ControllingMicrodroplets Self-Removal. Adv. Mater. 2013, 25, 22912295.(18) Tian, J.; Zhang, Y.; Zhu, J.; Yang, Z.; Gao, X. Robust NonstickySuperhydrophobicity by the Tapering of Aligned ZnO Nanorods.ChemPhysChem 2014, 15, 858861.(19) Beysens, D. The Formation of Dew. Atmos. Res. 1995, 39, 215237.(20) Nam, Y.; Kim, H.; Shin, S. Energy and Hydrodynamic Analysesof Coalescence-Induced Jumping Droplets. Appl. Phys. Lett. 2013, 103,161601.(21) Peng, B.; Wang, S.; Lan, Z.; Xu, W.; Wen, R.; Ma, X. Analysis ofDroplet Jumping Phenomenon with Lattice Boltzmann Simulation ofDroplet Coalescence. Appl. Phys. Lett. 2013, 102, 151601.(22) He, M.; Zhou, X.; Zeng, X.; Cui, D.; Zhang, Q.; Chen, J.; Li, H.;Wang, J.; Cao, Z.; Song, Y.; et al. Hierarchically Structured PorousAluminum Surfaces for High-Efficient Removal of Condensed Water.Soft Matter 2012, 8, 66806683.(23) Chandra, S.; Avedisian, C. T. On the Collision of a Droplet witha Solid Surface. Proc. R. Soc. London, Ser. A 1991, 432, 1341.(24) Lai, Y.; Gao, X.; Zhuang, H.; Huang, J.; Lin, C.; Jiang, L.Designing Superhydrophobic Porous Nanostructures with TunableWater Adhesion. Adv. Mater. 2009, 21, 37993803.(25) Gao, X.; Yao, X.; Jiang, L. Effects of Rugged Nanoprotrusionson the Surface Hydrophobicity and Water Adhesion of AnisotropicMicropatterns. Langmuir 2007, 23, 48864891.(26) Wong, T.-S.; Ho, C.-M. Dependence of Macroscopic Wettingon Nanoscopic Surface Textures. Langmuir 2009, 25, 1285112854.(27) Wisdom, K. M.; Watson, J. A.; Qu, X.; Liu, F.; Watson, G. S.;Chen, C.-H. Self-Cleaning of Superhydrophobic Surfaces by Self-Propelled Jumping Condensate. Proc. Natl. Acad. Sci. U.S.A. 2013, 110,79927997.(28) Chen, X.; Ma, R.; Zhou, H.; Zhou, X.; Che, L.; Yao, S.; Wang, Z.Activating the Microscale Edge Effect in a Hierarchical Surface forFrosting Suppression and Defrosting Promotion. Sci. Rep. 2013, 3,2515.(29) Yao, X.; Song, Y.; Jiang, L. Applications of Bio-Inspired SpecialWettable Surfaces. Adv. Mater. 2011, 23, 719734.

(30) Boreyko, J. B.; Collier, C. P. Delayed Frost Growth on Jumping-Drop Superhydrophobic Surfaces. ACS Nano 2013, 7, 16181627.(31) Zhang, Q.; He, M.; Chen, J.; Wang, J.; Song, Y.; Jiang, L. Anti-Icing Surfaces Based on Enhanced Self-Propelled Jumping ofCondensed Water Microdroplets. Chem. Commun. 2013, 49, 45164518.

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