# Stop Flow Lithography Synthesis and Characterization of Structured Microparticles

Authors: David Baah; Tobias Donnell; Sesha Srinivasan; Tamara Floyd-Smith
Journal: Journal of Nanomaterials
 (2014)

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## Abstract

In this study, the synthesis of nonspherical composite particles of poly(ethylene glycol) diacrylate (PEG-DA)/SiO2 and PEG-DA/Al2O3 with single or multiple vias and the corresponding inorganic particles of SiO2 and Al2O3 synthesized using the Stop Flow Lithography (SFL) method is reported.  Precursor suspensions of PEG-DA, 2-hydroxy-2-methylpropiophenone, and SiO2 or Al2O3 nanoparticles were prepared.  The precursor suspension flows through a microfluidic device mounted on an upright microscope and is polymerized in an automated process. A patterned photomask with transparent geometric features masks UV light to synthesize the particles. Composite particles with vias were synthesized and corresponding inorganic SiO2 and Al2O3 particles were obtained through polymer burn-off and sintering of the composites.  The synthesis of porous inorganic particles of SiO2 and Al2O3 with vias and overall dimensions in the range of ~35–90 µm was achieved.  BET specific surface area measurements for single via inorganic particles were 56–69 m2/g for SiO2 particles and 73–81 m2/g for Al2O3 particles.  Surface areas as high as 114 m2/g were measured for multivia cubic SiO2 particles. The findings suggest that, with optimization, the particles should have applications in areas where high surface area is important such as catalysis and sieving.


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## Body

## 1. Introduction

Organic and inorganic micro- and nanoparticles and their composites with tailored morphologies exhibit unique structural or shape dependent phenomena. For these particles, control of shape and morphology are desirable for improved application performance. For example, nonspherical particles are promising as drug delivery vehicles due to the dramatic increase in surface area-to-volume ratio (as a result of departure from spherical shape to nonspherical shape) and improved surface interaction (due to larger surface area) leading to increased cellular uptake into target organs [1, 2]. Consequently, efforts to develop new methods (both “bottom-up” and “top-down”) to synthesize particles with unique structural features have intensified. Recent reviews of the literature highlight developments toward shape control of micro- and nanoparticles with focus on scientifically and technologically important particles [3, 4]. Burda et al. (2005) explained that, with the bottom-up approach, particle formation begins with nucleation and homogenous nucleation is governed by the driving forces of thermodynamics [5]. For spherical particles, this driving force is expressed by the free energy change (Δ
G) of particle formation expressed in
(1)
Δ
G
r
=
-
4
V
π
r
3
k
B
T
In
⁡
S
+
4
π
r
2
γ
,
where V is the molecular volume of the precipitated species, r is the radius of the nuclei, k
B is the Boltzmann constant, S is the saturation ratio, and γ is the surface energy per unit surface area [5]. Even though it is the contention of the authors that particle growth follows the path of minimum energy which largely favors the formation of spherical particles, they posited that particle formation is kinetically driven and that any metastable shape can be arrested by changing the reaction conditions. Consequently, surfactant molecules and different concentrations of monomers as capping agents, as well as varying temperatures and pH of precursor solutions, are used as shape, size, and morphological control parameters following nucleation and during particle growth [5–9]. Conditions, such as slowing down the rate of polycondensation reaction in the sol gel synthesis of SiO2 nanoparticles, yield smaller sized particles whereas larger sized particles are obtained by increasing the ammonia concentration [10]. Other authors have discussed the use of emulsion droplets, hard and soft templates, sacrificial templates, and template free approaches for the synthesis of particles with unconventional structures and their applications in batteries, biomedicine, catalysis, and sensing [11–13]. Additionally, the independent or combined applications of the principles of Oswald ripening and Kirkendall effects have been used to achieve the synthesis of generally spherical and pseudospherical particles with hollow cavities for applications in gas adsorption and energy storage [14–22]. Like hollow particles, the introduction of small vias or ordered macropores is a novel means of creating structures with increased surface area [23].Given the potential of nonspherical particles, new approaches have been developed to provide additional methods to fill the need to synthesize them. While microfluidics technology is diverse in its usage including evaluation of nanobiomaterials and controlled release [24, 25], its application in particle design and synthesis is unparalleled. Recent articles have catalogued specific microfluidic platforms, particle formation precursors, and conditions which produce myriad particles with unique morphological features and production rates [26–28]. For example, the stop flow lithography (SFL) technique, used in this study, produces particles at a rate of 0.2 g/hr and depends on the free radical polymerization of the precursor onto which UV light is projected using a microscope. SFL is limited to extrusion of two-dimensional particles and, therefore, is an excellent method for synthesis of nonspherical particles for the current and potential applications that benefit from nonspherical particle shapes. SFL controls the particle axial dimension and the cross-sectional area using the microchannel depth and objective lens magnification, respectively. The versatility of this method extends to the ability to synthesize encoded particles for microRNA detection [29] with dimensions as small as 800 nm realized [30]. In previous work by the author and others, the SFL technique has been used to demonstrate the synthesis of nonspherical organic particles and their composites [31–33] as well as metal and metal oxide particles [34–36]. However, niche application requirements of metal oxide particles demand particles with ordered porosity which possess important physical properties, such as high surface area, favorable to heterogeneous catalysis, supports, sieves, and adsorbents [37, 38].In this paper, we report the synthesis of two-dimensionally extruded microparticles with single and multiple vias and different cross-sectional shapes using the SFL method. The particles reported in this paper consist of high fidelity and solvent free PEG-DA/SiO2 and PEG-DA/Al2O3 composite particles and their corresponding inorganic particles obtained through binder burn-out. In this work, microstructured particles are those in which vias are introduced with the aim of imparting additional surface area. The corresponding particle nanostructure results from the inorganic nanoparticles used to synthesize the microparticles. This paper is significant because it extends our work on the synthesis of solid metal oxide particles using SFL to microstructured particles with potential applications in the areas of catalysis, supports, sieves, and adsorbents. Also, to our knowledge, it provides the first detailed characterization of the nanostructure of these types of particles. SiO2 and Al2O3 are common catalyst support materials and were chosen because SiO2 has a low melting point and Al2O3 was simultaneously being investigated for abrasives applications. However, in theory, this method is applicable to any metal oxide or other material that can be acquired in nanoparticle form and has a melting point higher than 600°C, the temperature above which all polymer binder is removed.


## 2. Experimental

### 2.1. Materials

Precursor suspensions are prepared using a commercial SiO2 dispersion in water (Ludox AS-40 or Ludox CL-X colloidal silica), poly(ethylene glycol) diacrylate, 2-hydroxy-2-methylpropiophenone, hydrogen peroxide, and ascorbic acid all supplied by Sigma Aldrich, as well as an aluminum oxide nanodispersion (Al2O3, 20 wt%, 30 nm) supplied by US Research Nanomaterials Inc. The particle synthesis was conducted using geometrically patterned photomasks and in microfluidic devices whose fabrication methods were described in a preceding work [31, 39].


### 2.2. Particle Synthesis and Collection

Figure1 is a schematic illustration of the particle synthesis workstation. Patterned photomasks mask the UV light from a source. This photomask is inserted in the field stop of an upright microscope (Olympus BX51WF Microscope) and changed, when necessary, to change the imposed cross-sectional shapes of the particles. The UV light is focused onto the precursor flow stream using a 10x or 20x microscope objective lens. In addition to light focusing, the objective controls the particle cross-sectional size with the particle size decreasing as the objective magnification increases. The axial dimension of the particles is controlled by the microfluidic channel depth. In a typical operation, a three-way solenoid valve regulates the air-pressure-driven precursor solution supply to the microfluidic device mounted on the stage of a microscope. The precursor is prepared by mixing aliquots of the commercial suspensions of the inorganic nanoparticles with PEG-DA to constitute suspensions containing 10 wt% Al2O3 and 20 wt% SiO2 in 30 wt% PEG-DA. The goal was to use the highest possible concentration of nanoparticles in the suspension, but the concentration was limited by excessive fluid resistance to flow (high viscosity) caused by the particle loading as well as light scattering and consequent inadequate binder crosslinking in spite of index matching. The source of precursor supply is a 10 mL syringe, with the tip connected to the microfluidic device through ethyl vinyl acetate microbore tubing of 0.04′′ ID (WU-06492-04 Cole Parmer). The light source is a Lumen 200 (Prior Scientific) equipped with a 200 watt metal arc bulb connected to a Shutter Driver (VCM-D1, Uniblitz) whose opening and closure are synchronized with those of the solenoid valve to control the introduction of fresh precursor solution as well as expelling synthesized particles. A 365 nm bright-line filter (Max Lamp Mercury Line Filter-Hg01-365-25; Semrock) is positioned in the light path to select the appropriate wavelength of 365 nm for the photoactivation. Once the shutter is opened, the light comes through to the sample and a free radical polymerization is triggered which lasts for the period the light is on. Typically with this method, particles are synthesized in 75–350 ms exposure times in a fully automated process [36, 39, 40].Figure 1
Schematic of the stop flow lithography (SFL) setup consisting of a UV light source, a microfluidic device mounted on an upright microscope, and a prepolymer supply reservoir mounted on a clamp stand and connected to a solenoid valve to regulate sample flow to the device and particle ejection from the device.Particle separation is by gravity settling. The process is described in an earlier report [31]. Further, wash reagents (10 vol% hydrogen peroxide and 15 wt/vol % ascorbic acid) are used for final washing to maintain particle fidelity. Once the composite particles are collected, washed free from unreacted precursor, and stabilized, they are sintered using a 1500°C Compact Muffle Furnace (KSL-1500X-S) equipped with a programmable controller. For the composite SiO2 particles, the furnace is ramped from room temperature to 600°C at 5°C/min to first remove moisture and then burn off the polymer binder. The temperature is held at 600°C for 30 min to ensure complete removal of binder and then ramped again at ~4.5°C/min to 1150°C and held for 8 hours. Finally, controlled cooling is conducted at ~3°C/min to 100°C and the furnace shuts off while the particles continue to cool to room temperature. The process described produces consolidated ceramic particles. Sintering of PEG-DA/Al2O3 composite particles follows a similar profile except that the maximum temperature is 1450°C, near the limit of the equipment, with at least a two-hour hold time.


### 2.3. Characterization

The zeta potential of the particles in suspension was measured using a Zeta Potential Analyzer (ZetaPlus, BIC). First, aliquots of the mother liquor are centrifuged at 5000 rpm for 10 mins and the supernatant was collected. A few drops of the mother liquor are added to the supernatant, mixed thoroughly, and used as sample. Prior to sample measurement, a zeta potential reference material (BI-ZR3) is analyzed to check the instrument performance and reliability.Scanning electron microscopic (SEM) images of the samples were collected to show their microstructural features. First, approximately 5 mg of the dried aliquot sample is placed on a conductive carbon tape attached to the top of a 13 mm radius aluminum stub and placed in an EMS 550X Sputter Coating machine to coat the sample surface in a thin film of gold. Subsequently, the sample is imaged using a JOEL JSM 5800 or ZEISS EVO 50VP scanning electron microscope.The surface area and pore size distribution analyses are carried out using Quantachrome Instruments’ Autosorb-iQ BET surface area analysis. Approximately 0.5 g of sample is loaded in a 6 mm tube with a filler rod and outgassed for at least 3 hrs at 300°C, after which a 7-point nitrogen physisorption isotherm is performed at the liquid nitrogen temperature of 77 K. The BET (Brunauer-Emmett-Teller) surface area of the samples is determined using ASiQwin II data analysis software.


## 2.1. Materials

Precursor suspensions are prepared using a commercial SiO2 dispersion in water (Ludox AS-40 or Ludox CL-X colloidal silica), poly(ethylene glycol) diacrylate, 2-hydroxy-2-methylpropiophenone, hydrogen peroxide, and ascorbic acid all supplied by Sigma Aldrich, as well as an aluminum oxide nanodispersion (Al2O3, 20 wt%, 30 nm) supplied by US Research Nanomaterials Inc. The particle synthesis was conducted using geometrically patterned photomasks and in microfluidic devices whose fabrication methods were described in a preceding work [31, 39].


## 2.2. Particle Synthesis and Collection

Figure1 is a schematic illustration of the particle synthesis workstation. Patterned photomasks mask the UV light from a source. This photomask is inserted in the field stop of an upright microscope (Olympus BX51WF Microscope) and changed, when necessary, to change the imposed cross-sectional shapes of the particles. The UV light is focused onto the precursor flow stream using a 10x or 20x microscope objective lens. In addition to light focusing, the objective controls the particle cross-sectional size with the particle size decreasing as the objective magnification increases. The axial dimension of the particles is controlled by the microfluidic channel depth. In a typical operation, a three-way solenoid valve regulates the air-pressure-driven precursor solution supply to the microfluidic device mounted on the stage of a microscope. The precursor is prepared by mixing aliquots of the commercial suspensions of the inorganic nanoparticles with PEG-DA to constitute suspensions containing 10 wt% Al2O3 and 20 wt% SiO2 in 30 wt% PEG-DA. The goal was to use the highest possible concentration of nanoparticles in the suspension, but the concentration was limited by excessive fluid resistance to flow (high viscosity) caused by the particle loading as well as light scattering and consequent inadequate binder crosslinking in spite of index matching. The source of precursor supply is a 10 mL syringe, with the tip connected to the microfluidic device through ethyl vinyl acetate microbore tubing of 0.04′′ ID (WU-06492-04 Cole Parmer). The light source is a Lumen 200 (Prior Scientific) equipped with a 200 watt metal arc bulb connected to a Shutter Driver (VCM-D1, Uniblitz) whose opening and closure are synchronized with those of the solenoid valve to control the introduction of fresh precursor solution as well as expelling synthesized particles. A 365 nm bright-line filter (Max Lamp Mercury Line Filter-Hg01-365-25; Semrock) is positioned in the light path to select the appropriate wavelength of 365 nm for the photoactivation. Once the shutter is opened, the light comes through to the sample and a free radical polymerization is triggered which lasts for the period the light is on. Typically with this method, particles are synthesized in 75–350 ms exposure times in a fully automated process [36, 39, 40].Figure 1
Schematic of the stop flow lithography (SFL) setup consisting of a UV light source, a microfluidic device mounted on an upright microscope, and a prepolymer supply reservoir mounted on a clamp stand and connected to a solenoid valve to regulate sample flow to the device and particle ejection from the device.Particle separation is by gravity settling. The process is described in an earlier report [31]. Further, wash reagents (10 vol% hydrogen peroxide and 15 wt/vol % ascorbic acid) are used for final washing to maintain particle fidelity. Once the composite particles are collected, washed free from unreacted precursor, and stabilized, they are sintered using a 1500°C Compact Muffle Furnace (KSL-1500X-S) equipped with a programmable controller. For the composite SiO2 particles, the furnace is ramped from room temperature to 600°C at 5°C/min to first remove moisture and then burn off the polymer binder. The temperature is held at 600°C for 30 min to ensure complete removal of binder and then ramped again at ~4.5°C/min to 1150°C and held for 8 hours. Finally, controlled cooling is conducted at ~3°C/min to 100°C and the furnace shuts off while the particles continue to cool to room temperature. The process described produces consolidated ceramic particles. Sintering of PEG-DA/Al2O3 composite particles follows a similar profile except that the maximum temperature is 1450°C, near the limit of the equipment, with at least a two-hour hold time.


## 2.3. Characterization

The zeta potential of the particles in suspension was measured using a Zeta Potential Analyzer (ZetaPlus, BIC). First, aliquots of the mother liquor are centrifuged at 5000 rpm for 10 mins and the supernatant was collected. A few drops of the mother liquor are added to the supernatant, mixed thoroughly, and used as sample. Prior to sample measurement, a zeta potential reference material (BI-ZR3) is analyzed to check the instrument performance and reliability.Scanning electron microscopic (SEM) images of the samples were collected to show their microstructural features. First, approximately 5 mg of the dried aliquot sample is placed on a conductive carbon tape attached to the top of a 13 mm radius aluminum stub and placed in an EMS 550X Sputter Coating machine to coat the sample surface in a thin film of gold. Subsequently, the sample is imaged using a JOEL JSM 5800 or ZEISS EVO 50VP scanning electron microscope.The surface area and pore size distribution analyses are carried out using Quantachrome Instruments’ Autosorb-iQ BET surface area analysis. Approximately 0.5 g of sample is loaded in a 6 mm tube with a filler rod and outgassed for at least 3 hrs at 300°C, after which a 7-point nitrogen physisorption isotherm is performed at the liquid nitrogen temperature of 77 K. The BET (Brunauer-Emmett-Teller) surface area of the samples is determined using ASiQwin II data analysis software.


## 3. Results and Discussion

Table1 shows results from the zeta potential characterization of the precursor metal oxide particles. The high absolute values for Al2O3 (36.0 mV) and SiO2 (−20.9 mV), respectively, are indications of repulsive interparticle electrostatic interaction suggesting that particle agglomeration due to electrostatic attraction is unlikely. Consequently, one can expect to achieve uniform, stable nanoparticle dispersions as precursor suspensions and the corresponding high fidelity metal oxide particles.Table 1
Zeta potential of SiO2and Al2O3 nanoparticles.
SiO2
Al2O3
Solvent
Ludox/Water (n = 10)
Isopropanol (n = 10)
Concentration (% wt)
40
20
Particle size (nm)
15
30
Zeta potential (mV)
−20.9 ± 3.9
36.0 ± 2.6Two different microfluidic devices with channel depths in the range of 60–80 and 220–250μm are used to synthesize particles with the aim of creating particles with different axial dimensions. Additionally, objective lenses (10x and 20x) control cross-sectional size. Square, pentagonal, and circular cross-sectional shapes of particles with single vias are synthesized from the corresponding shape patterned in the photomask. Figures 2(a)–2(c) show SEM micrographs of high fidelity, monodisperse, and solvent free SiO2/PEGDA composite particles in three cross-sectional shapes. The micrographs in Figure 2 demonstrate that not only are high fidelity composite particles synthesized, but the cross-sectional shapes and sizes can be manipulated with relative ease. For example, Figure 2(a) is a square cross section of particles measuring 90–120 μm in axial and 100–110 μm in cross-sectional edge dimensions (220–250 μm device, 10x objective lens). The corresponding reduced form (images not shown) which measures 57–64 μm and 53–59 μm in axial and cross-sectional edge dimensions is produced using a 60–80 μm depth microfluidic device and a 20x objective lens with the same size transparent feature in the mask. Similar results for pentagonal and circular cross sections have been achieved. With the SFL approach, myriad two-dimensional shapes can be extruded to yield particles. Although the particles in Figure 2 have vias in the shape of the overall particles, other shapes can be introduced.SEM micrographs of solvent free SiO2/PEGDA composite particles with single vias in square, pentagonal, and circular cross-sectional shapes. Scale bar = 100 μm.
(a)
(b)
(c)The synthesis of Al2O3/PEGDA composite particles is also demonstrated. Figure 3 shows SEMs of cubic and rod-like composite particles with vias. A limitation of the Al2O3/PEGDA composite particle synthesis is the UV light screening due to Al2O3 as the weight fraction of Al2O3 nanoparticles increases. However, in up to 10 wt% fraction of Al2O3, it is possible to crosslink the precursor for which the images are shown in Figure 3. These Al2O3/PEG-DA composite particles, measuring ~100–110 μm in axial dimensions, are synthesized with a lower concentration of PEG-DA (25 wt%) in order to accommodate the viscosity of the stock Al2O3 nanodispersion. The composite particle integrity is illustrated in Figure 4 which shows a uniform wall thickness for the particles with square cross sections. The thickness of the via walls for the square cross sections is estimated to be in the range of 32–35 μm for the 10x objective and 220-250 μm device.Figure 3
SEM micrographs of solvent free Al2O3/PEGDA single via composite particles with square and circular cross-sectional shapes. Scale bar = 100 μm.Figure 4
Estimation of the wall thickness for the square cross section using the Al2O3/PEG-DA particles. Scale bar = 100 μm.The shape of corresponding inorganic particles was derived from the composites through polymer burn-out and sintering. Figures5(a)-5(b) are a collection of SEMs showing sintered SiO2 particles with vias in square and pentagonal cross sections. The particle fidelity is further demonstrated in the preservation of particle walls even on sintering the via composite particles. The axial dimensions of the particles for both cross section shapes were in the range of 75–85 μm for the 10x objective and 220-250 μm device and 35–45 μm for the 20x objective and 60–80 μm device (image not shown).SEM micrographs of SiO2 single via particles in square and pentagonal cross sections. Scale bar = 100 μm.
(a)
(b)These particles may have applications for hollow micro/nanomaterials based on properties which include high specific surface areas and inner voids [22]. In many cases, such characteristics make the particles superior to the same sized particle with simple and solid structures. Therefore, they are candidates in many important application areas such as catalysis, sensors [41], Li-ion batteries [12, 15], and drug delivery [42]. It is worth noting that the PEG-DA serves two purposes, (
1
) as a binder in the composite particles and (2) as a porogenic source in the inorganic particles. Generally, sintering reduces particle porosity. However, the presence of the binder (porogen) is expected to reduce the extent of porosity loss. The high magnification SEM (Figure 6(b)) of the SiO2 particle (inset: Figure 6(a)) surface reveals an agglomerated and tightly packed as well as an uneven particle surface. It appears that the compaction of the composite particles by interparticle electrostatic attractive forces of the constituent inorganic particles is enhanced by the sintering temperature in spite of the departing porogen (polymer binder). It is obvious, from this observation, that the final application of the particles must be considered when choosing the amount of binder, the sintering temperature, the duration of sintering, and other synthesis conditions. The TEM image of the precursor suspension (Figure 6(c)) confirms monodisperse constituent SiO2 nanoparticles which are spherically shaped and approximately 25 nm in diameter. Our goal is to produce inorganic particles of unique morphologies indirectly by first synthesizing the composites and burning out the binder. Particle size reduction is anticipated as the binder leaves and the inorganic component densifies on heat treatment. For the SiO2 particles, the percent change in the particle volume was calculated and found to range from 58 to 68% and 47 to 59% for the 220–250 μm and 60–80 μm channels, respectively. Assuming that it is applicable to use the bulk density for cristobalite, a volume reduction of ~90% for a 20 wt% loading of SiO2 is expected to correspond to a ~50% reduction in edge length. The difference between the experimental measurements and theoretical predictions is attributed to the porosity of the microparticles and the potential deviation of the nanoparticle density from that of the bulk material. It is also observed from Figure 6(b) that the inorganic component consists of spherically shaped SiO2 particles of approximately 25 nm diameter which are shown in Figure 6(c).Figure 6
(a) Low mag. SEM micrograph of SiO2 particles. (b) Higher mag. SEM of the SiO2 particle surface. Scale bar = 200 nm. (c) TEM of the as received Ludox particles. Scale bar = 50 nm.Figure7 shows SEM images of Al2O3 microparticles in circular cross sections imaged in progression of magnification (Figures 7(a)–7(c)) to reveal the microstructural characteristics of the particle surface. The micrographs suggest that the microparticles consist of rod-like Al2O3 nanoparticles aligned in a pattern. The structural features of Al2O3 nanoparticles are further revealed in the TEM image of the precursor suspension in Figure 7(d). Also, unlike the SiO2 nanoparticles, the Al2O3 nanoparticles formed an array with visible interparticle voids (Figure 7(c)). Considering that (
1
) the weight percent loading of the Al2O3 composite particles is low and (2) the sintering of Al2O3 usually requires temperatures in excess of 1600°C, one would expect highly porous Al2O3 microparticles. It might also explain why the theoretical prediction of volume reduction is over 95%, when only approximately ~60% reduction is measured experimentally.Figure 7
SEM micrographs of single via Al2O3 microparticles with a circular cross section (a). (b) and (c) are successively higher magnification images to reveal the microstructural features of (a). (d) TEM of the Al2O3 nanoparticles in suspension as received. Scale bars: (a) = 50 μm, (b) = 10 μm, (c) = 100 nm, and (d) = 100 nm.Figure8 shows multivia PEG-DA/SiO2 composite particles. The multiplicity of vias in the particles is a means to create particles with ordered porosity as well as providing additional surface area.Figure 8
SEM micrograph of multivia PEG-DA/SiO2 composite microparticles. Scale bars: 100 μm.The data for BET surface area, pore volume, and pore size collected by nitrogen physisorption are shown in Table2. Prior to data collection, standard microporous and mesoporous reference materials were evaluated to confirm the accuracy of the instrument. The inorganic, single via, SiO2 microparticles in square, circular, and pentagonal cross sections recorded BET surface area values in the range of 56–69 m2/g with pore volume and pore sizes of 0.08-0.09 cm3/g and 1.9–2.8 nm, respectively. Additionally, the SiO2 particle with four vias yielded a BET surface area, pore volume, and pore size of 114 m2/g, 0.15 cm3/g, and 2.1 nm, respectively. Similarly, the Al2O3 via particles recorded specific surface area values ranging from 73 to 81 m2/g.Table 2
BET surface area of single via SiO2 and Al2O3 particles of different cross sections and multi-via cubic SiO2 particles.
(a)
SiO2
Particle Cross Section Shape
Specific Surface Area(m2/g)
Pore Volume(cm3/g)
Pore Size(nm)
Square
56 and 114∗
0.09 and 0.15∗
1.9 and 2.1∗
Pentagonal
69
0.08
1.2
Circular
64
0.08
2.8
Range of particle dimension (µm)
40–47
(b)
Al2O3
Particle Cross Section  Shape
Specific Surface Area(m2/g)
Pore Volume(cm3/g)
Pore Size(nm)
Square
73
0.45
3.5
Circular
81
0.73
2.9
Range of particle dimension (µm)
75–90
∗4 via particle.The BET data collected for the single and multivia particles has several implications. First, the presence of the vias in these particles makes them superior with respect to surface area for physisorption compared with analogous solid particles. Second, based on the data obtained thus far, it is not obvious that the particle cross-sectional shapes influenced the BET values. Finally, for fully densified solid microparticles, one would expect surface area measurements less than 0.1 m2/g. Thus, obtaining surface areas from 50 to 80 m2/g, prior to optimization, suggests that the particles have potential for applications where structure and high surface area are important. In order to optimize the particles for future applications, removal of templates and volatile fractions by washing and calcination could increase the particle BET surface area by more than one order of magnitude [43, 44]. Also, control of the binder concentration could be another method to improve the porosity.


## 4. Conclusions

The SFL method is used to synthesize two-dimensionally extruded, nonspherical PEG-DA/SiO2 and PEG-DA/Al2O3 composite particles from which the corresponding inorganic particles are obtained by heat treatment. The approach represents an indirect application of the SFL technique to obtain high fidelity, consolidated inorganic particles. Microparticles of SiO2 and Al2O3 with square, circular, and pentagonal cross-sectional shapes with vias have been synthesized. Two objective lens magnifications of 10x and 20x were used to demonstrate the reduction in particle cross-sectional dimensions whereas two different channel depths (60–80 μm and 220–250 μm) controlled the particle axial dimension. High magnification SEM revealed that the SiO2 microparticles are formed from compacted spherical SiO2 nanoparticles. However, the high magnification image for Al2O3 revealed an array of rod-like Al2O3 nanoparticles interspersed with microvoids. BET surface area measurements for the single via inorganic particles were 56–69 m2/g for the SiO2 particles and 73–81 m2/g for the Al2O3 particles. Additionally, multivia cubic SiO2 particles measured 114 m2/g in BET surface area as determined by nitrogen physisorption isotherms at liquid nitrogen temperature (77 K). The surface areas achieved suggest that the particles have great potential for applications in areas like catalysis and sieving where structure and surface area control are important.



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*Source: 142929-2014-12-31.xml*