Eect of Ionic Strength and Surface Charge on Convective Deposition Kedar Joshi, Tanyakorn Muangnapoh, Michael D. Stever, and James F. Gilchrist a) Department of Chemical and Biomolecular Engineering, Lehigh University, Bethlehem, Pennsylvania 18015, United States ABSTRACT: Particle-particle and particle-substrate interac- tions play a crucial role in capillary driven convective self- assembly for continuous deposition of particles. This systematic study demonstrates the nontrivial eects of varying surface charge and ionic strength of monosized silica microspheres in water on the quality of the deposited monolayer. Increase in particle surface charge results a broader range of parameters that result in monolayer deposition which can be explained considering the particle-substrate electrostatic repulsion in solution. Resulting changes in the coating morphology and microstructure at dierent solution conditions were observed using confocal microscopy enabling correlation of order to disorder transitions with relative particle stability. These results, in part, may explain similar results seen by Muangnapoh et al., 2013 in vibration-assisted convective deposition. 1. INTRODUCTION Microsphere arrays have tremendous applications in our day to day life. Convective deposition is a well-known technique for depositing microspheres into closed packed structures 1-3 and has proven very useful tool in elds like coatings for LEDs 4-7 and solar cells, 8 membranes, 9 cell capture devices, 10 and in functionalizing Janus particles. 11 Here the particles are made to form close packed structures using capillary interactions. 12 A meniscus of the suspension is created between a substrate and a blade and by relatively moving a substrate with respect to a blade, the meniscus is stretched into thin lm. 13 The process consists of two physical processes happening simultaneously. First, convection is driven by evaporation, 3,14 similar to the coee ring eect, 15 where ow is generated by the evaporation losses. The other is capillary attraction where particles on liquid interface, were particles are drawn into a close packed structure to minimize the energy, 16-18 similar to that found in the cheerio eect. 19 A ux balance equation relating the evaporating liquid to the substrate velocity and particle volume fraction 2 is given as β ε = Φ −Φ V J dN(1 ) c e S (1) Where V c : the crystallization velocity, J e : the evaporation ux, Φ: is the volume fraction of the suspension, S : the evaporation length that scales with the area of the evaporation region, ε: the porosity of deposited crystal, and d: the particle diameter. N: number of particle layers. When N = 1 we get monolayer coating and corresponding velocity (V c ) is referred as monolayer deposition speed. This equation includes an additional interaction parameter, β, originally described as the particle-substrate interaction, arising from the nonuniform distribution of particles through the thickness of the thin lm. This results in a mismatch between particle and water ux. Particles owing in the thin lm are acted upon by dierent forces 20 such as electrostatic repulsion, Van der Waal forces, and buoyancy. All these interactions govern the particles distribution in thin lm. The following work is done to get more understanding of particle-particle and particle-substrate interactions on monolayer velocity as well as microstructure. Bulk ions concentration as well as charge on colloidal particles can play signicant role in designing the process. The focus of this paper is on the eect of screening and surface charge on monolayer quality during convective deposition (Figure 1). There are numerous studies of the eects of added electrolytes on self-assembly of particles 21-25 and the eects of dierent surface active groups to change particle-substrate interactions. 26-28 Addition of salt decreases Debye length, thereby further screening the eects of electrostatic repulsion. Rö dner et al. have shown the eects of electrolytes on structural changes of monolayer silica particle lms. 23 Similar to evaporation-driven deposition, drop drying is aected by DLVO interactions resulting in varying the shape of dried droplets. 24 In convective deposition, using binary suspensions of large and small microspheres has resulted in higher order with less streaking instabilities, although the mechanism is poorly understood. 29,30 Similarly, added lateral vibration during deposition has been shown to increase the degree of order in deposited monolayers as well as increasing the range of velocities in which monolayers can be obtained from essentially a single ideal velocity, as suggested in eq 1, to a Received: August 19, 2015 Revised: October 25, 2015 Article pubs.acs.org/Langmuir © XXXX American Chemical Society A DOI: 10.1021/acs.langmuir.5b03109 Langmuir XXXX, XXX, XXX-XXX