Abstract:We study the deposition mechanisms of polymer from a confined meniscus of volatile liquid. In particular, we investigate the physical processes that are responsible for qualitative changes in the pattern deposition of polymer and the underlying interplay of the state of pattern deposition, motion of the meniscus, and the transport of polymer within the meniscus. As a model system we evaporate a solution of poly(methyl methacrylate) (PMMA) in toluene. Different deposition patterns are observed when varying the… Show more
“…The confinement is advantageous for rendering physical parameters in the experiment, for example, temperature, rate of water evaporation, linear geometry of the three phase contact line between the liquid, vapor, and solid substrate and its position (where the majority of the deposit is usually found), well defined. [34,[45][46][47][48] In this work, a rectangular micro-chamber is employed, which is composed of silica as a substrate (<100 >, 550 µm thickness, with 1 µm wet thermal oxide layer, Silicon Materials) and glass (microscopy slide, Marienfeld) as a cover. The inner thickness of the chamber was 125 µm, according to the choice of the polyamide film (Kapton, DuPont) spacer, which separated between the substrate and the glass cover.…”
The capacity of nanoparticles to self‐arrange to various structures and their unique physical properties has made these building blocks essential in a broad range of applications and scientific disciplines. In this work, the manipulation of particulate structures that appear from binary dispersions is demonstrated, comprising same size particles of two different chemistries, following the evaporation of an electrolyte solution carrier. By varying the ionic strength and pH in the solutions, the balance between attractive and repulsive surface forces is tuned, that is, electrical double layer, Van der Waals, hydrophobic, and hydrophilic forces, in the binary particle mixtures. Hence, the corresponding potential energy barriers are tuned to particle attachments to each other and to the underlying substrate and alter the nanoscopic arrangement of the different types of particles in the microscopic particulate structures, which appear by convective pattern formation. Hence, by realizing the physical mechanisms which govern the potential energy contributions to the pattern formation of particulate structures at the nanometer scale, the 3D morphology of binary mixtures of same size particles is rendered homogeneous, layered, or phases separated. This is a useful approach toward the top‐down fabrication of nonhomogeneous colloidal structures.
“…The confinement is advantageous for rendering physical parameters in the experiment, for example, temperature, rate of water evaporation, linear geometry of the three phase contact line between the liquid, vapor, and solid substrate and its position (where the majority of the deposit is usually found), well defined. [34,[45][46][47][48] In this work, a rectangular micro-chamber is employed, which is composed of silica as a substrate (<100 >, 550 µm thickness, with 1 µm wet thermal oxide layer, Silicon Materials) and glass (microscopy slide, Marienfeld) as a cover. The inner thickness of the chamber was 125 µm, according to the choice of the polyamide film (Kapton, DuPont) spacer, which separated between the substrate and the glass cover.…”
The capacity of nanoparticles to self‐arrange to various structures and their unique physical properties has made these building blocks essential in a broad range of applications and scientific disciplines. In this work, the manipulation of particulate structures that appear from binary dispersions is demonstrated, comprising same size particles of two different chemistries, following the evaporation of an electrolyte solution carrier. By varying the ionic strength and pH in the solutions, the balance between attractive and repulsive surface forces is tuned, that is, electrical double layer, Van der Waals, hydrophobic, and hydrophilic forces, in the binary particle mixtures. Hence, the corresponding potential energy barriers are tuned to particle attachments to each other and to the underlying substrate and alter the nanoscopic arrangement of the different types of particles in the microscopic particulate structures, which appear by convective pattern formation. Hence, by realizing the physical mechanisms which govern the potential energy contributions to the pattern formation of particulate structures at the nanometer scale, the 3D morphology of binary mixtures of same size particles is rendered homogeneous, layered, or phases separated. This is a useful approach toward the top‐down fabrication of nonhomogeneous colloidal structures.
“…A recent detailed analysis of patterns obtained in evaporative dewetting is given in Ref. [17]. In the case of the well studied "passive systems" the contact line velocity is selected by the system and not externally imposed as in "active systems" like slot-die coating and many other coating processes.…”
We experimentally study the occurrence of pattern formation during the slot-die coating of lowviscosity nearly Newtonian liquids onto Polyethylenterephthalat (PET)-substrates. In particular, it is demonstrated that with increase of the coating speed a homogeneous coating becomes unstable with respect to periodic stripe patterns. Thereby, depending on the liquid viscosity, the stripes can be oriented parallel or perpendicular with respect to the coating direction. Mixed states do also occur. The spatial period of perpendicular [parallel] stripes increases [decrease] with the coating speed. The dependence of the effect on various control parameters of slot-die coating is investigated.Finally, a simple theoretical model based on the hydrodynamics of thin films of partially wetting liquids is analysed. Comparing the results to the experiments, conclusions are drawn regarding the acting instability and pattern formation mechanisms.
“…Depending on the properties of the liquid, wetting behaviour of the liquid on the substrate and withdrawal speed (or strength of evaporation), a large variety of homogeneous and patterned coatings can be produced. For instance, well controlled experiments with particle suspensions [10,11,12] or polymer solutions [13,14,15,16] may produce regular line patterns orthogonal or parallel to the withdrawal direction [11,13,16]. Other described patterns include interconnected or wavy stripes [16], ladder structures [13], hierarchical line patterns [17], droplet or hole arrays [13,14,16], and branched structures [18,19].…”
Section: Introductionmentioning
confidence: 99%
“…For instance, well controlled experiments with particle suspensions [10,11,12] or polymer solutions [13,14,15,16] may produce regular line patterns orthogonal or parallel to the withdrawal direction [11,13,16]. Other described patterns include interconnected or wavy stripes [16], ladder structures [13], hierarchical line patterns [17], droplet or hole arrays [13,14,16], and branched structures [18,19]. Overviews are given in [9,6].…”
Section: Introductionmentioning
confidence: 99%
“…Overviews are given in [9,6]. Note that systematic accounts of parameter dependencies of properties of deposition patterns and of the transitions between different patterns are rare [10,16].…”
We present a brief comparative investigation of the bifurcation structure related to the formation of two-dimensional deposition patterns as described by continuum models of Cahn-Hilliard type. These are, on the one hand a driven Cahn-Hilliard model for Langmuir-Blodgett transfer of a surfactant layer from the surface of a bath onto a moving plate and on the other hand a driven thin-film equation modelling the surface acoustic wave-driven coating of a plate by a simple liquid. In both cases, we present selected two-dimensional steady states corresponding to deposition patterns and discuss the main structure of the corresponding bifurcation diagrams.
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