GA A26949 SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS FOR INERTIAL CONFINEMENT FUSION EXPERIMENTS

Similar documents
GA A26323 MODIFYING THE POR SIZE OF RESORCINOL FORMALDEHYYDE AEROGELS FOR FABRICATION OF HOLLOW SPHERES FOR DIRECT DRIVE ICF EXPERIMENTS

GA A25658 PRECISION X-RAY OPTICAL DEPTH MEASUREMENTS IN ICF SHELLS

Preparation of Organic Aerogels

FUSION TECHNOLOGY INSTITUTE

GA A26474 SYNERGY IN TWO-FREQUENCY FAST WAVE CYCLOTRON HARMONIC ABSORPTION IN DIII-D

GA A22689 SLOW LINER FUSION

Inside Wall Temperature Measurements of DSTs Using an Infrared Temperature Sensor

Preparation of DielectAcs HR Mirrors from Colloidal Oxide Suspensions Containing Organic Polymer Binders

Three-Dimensional Silicon Photonic Crystals

Influence of Nonionic Surfactant Concentration on Physical Characteristics of Resorcinol-Formaldehyde Carbon Cryogel Microspheres

GA A22722 CENTRAL THOMSON SCATTERING UPGRADE ON DIII D

GA A27806 TURBULENCE BEHAVIOR AND TRANSPORT RESPONSE APPROACHING BURNING PLASMA RELEVANT PARAMETERS

Determine the Inside Wall Temperature of DSTs using an Infrared Temperature Sensor

THE DISCOVERY OF FULLERENES IN THE 1.85 BILLION-YEAR-OLD

GA A27805 EXPANDING THE PHYSICS BASIS OF THE BASELINE Q=10 SCENRAIO TOWARD ITER CONDITIONS

A Distributed Radiator, Heavy Ion Driven Inertial Confinement Fusion Target with Realistic, Multibeam Illumination Geometry

GA A23736 EFFECTS OF CROSS-SECTION SHAPE ON L MODE AND H MODE ENERGY TRANSPORT

Solid Phase Microextraction Analysis of B83 SLTs and Core B Compatibility Test Units

Plasma Response Control Using Advanced Feedback Techniques

Capabilities for Testing the Electronic Configuration in Pu

Supplementary Information

Response to Comment on "The National Ignition Facility Laser Performance Status"

PROJECT PROGRESS REPORT (03/lfi?lfibr-~/15/1998):

GA A26057 DEMONSTRATION OF ITER OPERATIONAL SCENARIOS ON DIII-D

Abstract of paper proposed for the American Nuclear Society 1997 Winter Meeting Albuquerque, New Mexico November 16-20, 1997

STABILIZATION OF m=2/n=1 TEARING MODES BY ELECTRON CYCLOTRON CURRENT DRIVE IN THE DIII D TOKAMAK

GA A24166 SUPER-INTENSE QUASI-NEUTRAL PROTON BEAMS INTERACTING WITH PLASMA: A NUMERICAL INVESTIGATION

Encapsulation. Battelle Technology. Introduction

INTERMOLECULAR POTENTIAL FUNCTIONS AND HIGH RESOLUTION MOLECULAR SPECTROSCOPY OF WEAKLY BOUND COMPLEXES. Final Progress Report

(4) How do you develop an optimal signal detection technique from the knowledge of

PROGRESS REPORT JULY TO SEPTEMBER

ADSORPTION ON NANOSURFACES: A DETAILED LOOK AT METAL CLUSTERS USING INFRARED SPECTROSCOPY

Determine the Inside Wall Temperature of DSTs using an Infrared Temperature Sensor

GA A22677 THERMAL ANALYSIS AND TESTING FOR DIII D OHMIC HEATING COIL

Analysis of Shane Telescope Aberration and After Collimation

Fission-Fusion Neutron Source

GA A27235 EULERIAN SIMULATIONS OF NEOCLASSICAL FLOWS AND TRANSPORT IN THE TOKAMAK PLASMA EDGE AND OUTER CORE

UNDERSTANDING TRANSPORT THROUGH DIMENSIONLESS PARAMETER SCALING EXPERIMENTS

2 Preparation of hollow spheres, microcapsules and microballoons by surfactant free emulsion templating

Simulation of Double-Null Divertor Plasmas with the UEDGE Code

Development of a High Intensity EBIT for Basic and Applied Science

DE '! N0V ?

Status and Progress of a Fault Current Limiting HTS Cable To Be Installed In The Consolidated Edison Grid

The Impacts of Carbon Dioxide Storage in the Saline Arbuckle Aquifer on Water Quality in Freshwater Aquifers in Kansas

PLASMA MASS DENSITY, SPECIES MIX AND FLUCTUATION DIAGNOSTICS USING FAST ALFVEN WAVE

Plutonium 239 Equivalency Calculations

BWXT Y-12 Y-12. A BWXT/Bechtel Enterprise SMALL, PORTABLE, LIGHTWEIGHT DT NEUTRON GENERATOR FOR USE WITH NMIS

Scaling of divertor heat flux profile widths in DIII-D

ions which are abundant in waste water. Since zeolites are

Working with Hazardous Chemicals

Parametric Instabilities in Laser/Matter Interaction: From Noise Levels to Relativistic Regimes

EXPLOSIVE PARTICLES PARVLENE ENCAPSUTION. lac0 b Sando v a t. Normal Process Development OCTOBER DEVEZOPMENT D I V I S I O N DEZEMBER 1971

Multicusp Sources for Ion Beam Lithography Applications

Synthesis of Methyl Methacrylate from Coal-derived Syngas

Using the X-FEL to understand X-ray Thomson scattering for partially ionized plasmas

GA A27857 IMPACT OF PLASMA RESPONSE ON RMP ELM SUPPRESSION IN DIII-D

Applications of Pulse Shape Analysis to HPGe Gamma-Ray Detectors

Chromatography. What is Chromatography?

FUSION WITH Z-PINCHES. Don Cook. Sandia National Laboratories Albuquerque, New Mexico 87185

GA A23713 RECENT ECCD EXPERIMENTAL STUDIES ON DIII D

MAGNETIC RESONANCE IMAGING OF SOLVENT TRANSPORT IN POLYMER NETWORKS

Ester Synthesis And Analysis: Aspirin and Oil of Wintergreen. Vanessa Jones November 19, 2015 Thursday 8:30 Lab Section Lab Partner: Melissa Blanco

GA A26785 GIANT SAWTEETH IN DIII-D AND THE QUASI-INTERCHANGE MODE

Novel Ceramic Membrane for High Temperature Carbon Dioxide Separation

PREDICTIVE MODELING OF PLASMA HALO EVOLUTION IN POST-THERMAL QUENCH DISRUPTING PLASMAS

Methodology and Discussion

GA A THERMAL ION ORBIT LOSS AND RADIAL ELECTRIC FIELD IN DIII-D by J.S. degrassie, J.A. BOEDO, B.A. GRIERSON, and R.J.

Alex Dombos Michigan State University Nuclear and Particle Physics

BASAL CAMBRIAN BASELINE GEOLOGICAL CHARACTERIZATION COMPLETED

RWM FEEDBACK STABILIZATION IN DIII D: EXPERIMENT-THEORY COMPARISONS AND IMPLICATIONS FOR ITER

GA A25853 FAST ION REDISTRIBUTION AND IMPLICATIONS FOR THE HYBRID REGIME

Two-Screen Method for Determining Electron Beam Energy and Deflection from Laser Wakefield Acceleration

CQNl_" RESPONSE TO 100% INTERNAL QUANTUM EFFICIENCY SILICON PHOTODIODES TO LOW ENERGY ELECTRONS AND IONS

Hydra Fault Current Limiting HTS Cable to be Installed in the Consolidated Edison Grid

J. R Creighton and C. M. Truong Org. 1126, MS 0601 P.O. Box 5800 Sandia National Laboratories Albuquerque, NM

Exploration of the Feasibility of Polar Drive on the LMJ. Lindsay M. Mitchel. Spencerport High School. Spencerport, New York

Process Systems Engineering

Ali Hayek, a Yongan Xu, b Takashi Okada, a Stephen Barlow, a Xuelian Zhu, b Jun Hyuk Moon, b Seth R. Marder, * a and Shu Yang* b

Supplementary Information

Multi-Scale Chemical Process Modeling with Bayesian Nonparametric Regression

Lab #6: CARBOXYLIC ACIDS LAB

Controlling Backstreaming Ions from X-ray Converter Targets with Time Varying Final Focusing Solenoidal Lens and Beam Energy Variation

A NEW TARGET CONCEPT FOR PROTON ACCELERATOR DRIVEN BORON NEUTRON CAPTURE THERAPY APPLICATIONS* Brookhaven National Laboratory. P.O.

ORGANIC SYNTHESIS: MICROWAVE-ASSISTED FISCHER ESTERIFICATION

Curvature of a Cantilever Beam Subjected to an Equi-Biaxial Bending Moment. P. Krulevitch G. C. Johnson

PROCEEDINGS THIRD WORKSHOP GEOTHERMAL RESERVOIR ENGINEERING. December 14-15,1977

GA A22900 STATUS OF THE DESIGN AND TESTING OF THE OMEGA CRYOGENIC TARGET SYSTEM (OCTS)

Novel Nanoparticles for Ultrasensitive Detection and Spectroscopy

GA A24016 PHYSICS OF OFF-AXIS ELECTRON CYCLOTRON CURRENT DRIVE

Modeling Laser and e-beam Generated Plasma-Plume Experiments Using LASNEX

AP Chemistry Lab #5- Synthesis and Analysis of Alum (Big Idea 1 & 2)

Start-up Noise in 3-D Self-AmpMed

ION EXCHANGE SEPARATION OF PLUTONIUM AND GALLIUM (1) Resource and Inventory Requirements, (2) Waste, Emissions, and Effluent, and (3) Facility Size

12/16/95-3/15/96 PERIOD MULTI-PARAMETER ON-LINE COAL BULK ANALYSIS. 2, 1. Thermal Neutron Flux in Coal: New Coal Container Geometry

Nucleophilic displacement - Formation of an ether by an S N 2 reaction The Williamson- Ether Synthesis

Elements and Their Oxides

Half-Cell, Steady-State Flow-Battery Experiments. Robert M. Darling and Mike L. Perry

Synthetic Studies on Norissolide; Enantioselective Synthesis of the Norrisane Side Chain

UPGRADED CALIBRATIONS OF THE THOMSON SYSTEM AT DIII D

ASTER CONF-~W OSTI MAY DISTRIBUTION OF THIS

Transcription:

GA A26949 SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS FOR INERTIAL CONFINEMENT FUSION EXPERIMENTS by K.M. SAITO, R.R. PAGUIO, J.F. HUND, and R.M. JIMENEZ NOVEMBER 2010

DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.

GA A26949 SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS FOR INERTIAL CONFINEMENT FUSION EXPERIMENTS by K.M. SAITO, R.R. PAGUIO, J.F. HUND, and R.M. JIMENEZ This is a preprint of a paper presented at the Materials Research Society Fall Meeting in Boston, Massachusetts, November 29, Through December 3, 2010 and to be published in Proceedings. GENERAL ATOMICS PROJECT 40011 NOVEMBER 2010

SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS K.M. Saito, et al. Synthesis of Resorcinol Formaldehyde Aerogel Using Photo-Acid Generators for Inertial Confinement Fusion Experiments K.M. Saito, R.R. Paguio, J.F. Hund, and R.M. Jimenez General Atomics, PO Box 85608, San Diego, California 92186-5608, U.S.A. ABSTRACT Traditionally, the synthesis of Resorcinol formaldehyde (R/F) aerogels consists of a 2-step (base/acid catalysis) polycondensation reaction. Since the acid catalyst in the reaction controls the gelation time, we are able to replace the acid catalyst with a non-ionic photo-acid generator decreasing the gelation time from hours, down to a few minutes at room temperature using a UV light source. Not only was the reaction rate fast, but the liquid precursor was stable for several hours prior to UV exposure. After drying, the resulting aerogel porosity was not changed significantly from the standard process. Scanning electron microscopy (SEM) confirms the internal structure of the aerogel was similar to the original and modified R/F pore structures. This paper will discuss the modifications made to the traditional R/F formulation, as well as the benefits of a fast gelation time for aerogel casting applications such as thin films, cylinders, and solid and hollow microspheres. The modified R/F formulation process also opens up the possibility of directly patterning aerogels into complex shapes on a surface using a photo-mask. INTRODUCTION Resorcinol formaldehyde aerogels are currently used in a variety of inertial confinement fusion (ICF) experiments in the form of solid and hollow spheres, cylinders, and thin films. These R/F aerogels are currently synthesized using the traditional 2-step polycondensation reaction devised by Pekala [1]. This 2-step polycondensation reaction consists of a base and acid catalysis step to form the R/F aerogel. The first step in the reaction was the base catalysis step which creates the hydroxymethyl aggregates; these aggregates react with one another to form the primary particles of R/F clusters. These particles then go through an acid catalysis step which bonds the particles together with methylene ether bridges to form the hydrogel. During the base catalysis step, small amounts of acid are generated [1] eventually leading to the gelation of the R/F. This reaction by itself would take significantly longer (hours to days) and not optimal for the experimental working time, necessitating additional acid. Heat was also used in both steps of this reaction to help speed up the process, allowing the gel to setup in the time frame for these experiments in a typical working day. One of the main uses and designs for R/F aerogels in ICF experiments was in the form of hollow microspheres (spherical shells) as shown in figure 1, containing hydrogen isotope fuel. This was for future direct and indirect drive targets at the National Ignition Facility (NIF) and eventual use in an inertial fusion energy (IFE) power plant [2,3]. One of the issues with the R/F aerogel shells was meeting the wall uniformity specification. Investigations and process improvements at General Atomics (GA) have been made to the traditional R/F shell fabrication process first developed by Lambert et al. [4] to improve the yields of intact shells to 90% [5] and wall uniformity specification of 50% [6,7]. Though this yield may be acceptable for near term experiments, this yield was not acceptable for the HAPL energy plant design which required approximately a million shells a day. GENERAL ATOMICS REPORT GA-A26949 1

K.M. Saito, et al. SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS Figure 1. R/F capsules fabricated using the droplet generator method. Diameters of capsules: HAPL is 4500 m, Direct-NIF is 3000 m, Indirect-NIF is 1800 m, and OMEGA is 880 m. The wall uniformity issue has led to the investigation of alternative methods such as dielectrophoresis (DEP) [8,9] to center and fabricate these R/F shells. DEP uses electric fields to move and center the shell while it was in its double emulsion form. The DEP process to center these shells was in development at the University of Rochester (U of R). U of R has developed a 20 MHz device and technique using DEP to center a double emulsion of water-oil-water [10,11]. The work done by Bei, et al. provided the parameters and requirements for the aerogel precursor solution to work in the device [10,11]. One of these parameters was the conductivity of the aerogel precursor solution needs to be in the 10-3 S/m range or lower; the other requirement was the precursor solution must gel at room temperature (RT) in 20 minutes or less. The shells must be cured at RT without heat because heating the DEP system will disrupt the electric field as well as damage the circuits used to create the electric field. Heat can also cause convection currents in the DEP centering device which can cause the double emulsion shell to not center. Based on these requirements, the current R/F synthesis technique was not compatible with the DEP device. This led to the investigation of other possibilities to synthesize the R/F aerogel and use a photo-acid generator (PAG) for the acid catalysis step. PAG activates by exposure from UV light, producing an acid. If the acid produced by the PAG was strong enough, the gelation of R/F will occur in a matter of minutes as opposed to hours. The main concept for substituting the PAG into the R/F process was to control the time at which gelation of R/F occurs. Despite being able to successfully substitute the PAG for the acid catalysis step in the polycondensation reaction, problems arise in finding the right PAG to fit into the reaction and making the PAG soluble in the R/F precursor solution. This paper will discuss these issues and how insertion of the right PAG into the current R/F formulation creates an alternative method to synthesize the R/F aerogel. EXPERIMENT Selecting a photo-acid generator The traditional R/F formulation for fabricating shells uses a precursor solution producing an aerogel with a density of 100 mg/cc, the density requirement for ICF experiments. This formulation was used to determine which PAG works the best for replacing benzoic acid in the acid catalysis step of the polycondensation reaction. A precursor solution consisting of resorcinol, formaldehyde, water, and a base catalyst (0.58 M sodium bicarbonate) are combined in a rotary 2 GENERAL ATOMICS REPORT GA-A26949

SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS K.M. Saito, et al. beaker and heated in a water bath at 70 o C for 45 minutes. As the precursor solution heats, the base catalysis of the reaction occurs and R/F clusters begin to form in the solution. At the 45- minute mark, the precursor solution was removed from the water bath and chilled in an ice water bath for 10 minutes, allowing the reaction to slow down and reduce the acid formation in the solution. After removing the precursor solution from the ice water bath, PAG was used as a substitute for benzoic acid. Several different PAGs were selected and tested based on the solubility in the precursor solution, reactivity to the precursor solution, and the wavelength at which the PAG activates. The precursor solution was divided into smaller, equal volumes and the desired PAG was added to the precursor solution. Since the volume of PAG being added to the precursor solution was small compared to the volume of diluted benzoic acid, the remaining volume of PAG was filled with water to match the volume total of benzoic acid and water in the traditional R/F formulation. To test the gelation of the R/F solution with the PAG, a droplet of R/F was suspended in a vial containing mineral oil, sorbitan moonoleate (SPAN-80), and tetrachloroethlyene (TCE). The mixing ratio of mineral oil to TCE suspended the R/F drops based on the density, and SPAN-80 was a surfactant added to prevent the R/F drops from agglomerating. Drops of the R/F solution with PAG were added to the vial and then exposed using a UV light source (Hg lamp, 100W Green Spot Model GS) as shown in figure 2. The PAG fitting the criteria of being soluble, non-reactive in R/F and a fast gelation time was the PAG used in synthesizing R/F for ICF experiments. Figure 2. Droplets of R/F precursor with the PAG are suspended in an oil mixture and exposed to UV light. The suspension test was a quick way to determine the gelation time of R/F. Fabricating R/F capsules with a photo-acid generator The frequency of the field in a DEP device necessary to center a compound droplet depends on the conductivity of the droplet wall; the higher the conductivity, the higher the frequency required. Because of this, the conductivity of the precursor solution was critical for the solution to center using the DEP device. After selecting the PAG for the second step of the polycondensation reaction, the conductivity of the R/F solution was measured with a conductivity meter (VMR) to ensure the R/F was within the working range for the DEP device. If the R/F solution meets the conductivity requirements for the DEP device, it may be a possible candidate for the DEP centering device. Another way to utilize the PAG in the R/F formulation was to apply it to the current R/F capsule fabrication process with the triple orifice droplet generator [4-7]. The droplet generator contains three orifices consisting of an inner oil (O1) line, the R/F precursor solution with PAG (W1) line, and an outer oil (O2) line. The O1 is an oil mixture containing mineral oil and TCE, GENERAL ATOMICS REPORT GA-A26949 3

K.M. Saito, et al. SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS and the O2 is an oil mixture containing mineral oil, TCE, and SPAN-80. The O1 and W1 combine to form a double emulsion droplet, and suspended in the O2 throughout the gelation process. Density matching the R/F precursor solution with the O1 and O2 was necessary to keep the double emulsion suspended. As the double emulsion droplets of R/F and oil travel into a rotary beaker, the droplets are exposed to UV light for gelation as shown in figure 3. Figure 3. (a) Example of the encapsulation process of the double emulsion. W 1 is the R/F solution with PAG, O 1 is the inner oil mixture, and O 2 is the outer oil mixture. (b) The R/F capsules rotate in a rotary beaker while exposed to UV light. After gelation of the double emulsion R/F droplets, the cured capsules undergo a post cure process to increase the cross-linking density of the R/F. The capsules were solvent exchanged into isopropanol to remove any water in the porous gel network and dried using a supercritical CO 2 drier to prevent shrinkage and cracking, preserving the low density structure of the resulting aerogel. After drying, the R/F capsules may then be handled to undergo characterization of the pore structure, surface roughness and wall uniformity. DISCUSSION Selection of PAG by droplet suspension test Selecting the PAG to substitute the current acid catalyst (benzoic acid) in the traditional polycondensation reaction proved to be the most challenging aspect of the selection process. The first group of PAGs tested all contained the same triflate acid being formed when exposed to UV light. To verify if Pekala s 2-step polycondensation would work with the PAGs, trifluoromethanesulfonic acid (triflic acid) was initially used to prove gelation would occur. By substituting the triflic acid for the acid catalyst, the R/F precursor solution gelled instantaneously verifying the R/F will cure when the activated PAG forms triflic acid. The PAG, dimethyl 2,4- dihydroxyphenylsulfonium triflate (Oakwood Chemical), was selected because of its solubility in water. 0.00735M of PAG was dissolved in water to match the same molar concentration of benzoic acid used in traditional R/F formulation. The PAG solution was added to the R/F precursor solution after the base catalysis step. When adding the PAG solution to the R/F precursor solution, a white precipitate formed instantly at the bottom of the test vial. Since no UV light was exposed to activate the PAG, the white precipitate was not a result of R/F gelation. The R/F was exposed to UV light for 20 minutes, but the bulk solution remained liquid. Also, there was no change in ph after exposing to UV light. Glass tubes were placed in the vial to obtain R/F 4 GENERAL ATOMICS REPORT GA-A26949

SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS K.M. Saito, et al. samples for characterization. Even if the PAG did not activate to form an acid to speed up the gelation, the bulk R/F sample eventually gelled overnight (~12 hours) due to the small amount of acid being formed in the base catalysis step of the reaction. The R/F hydrogel in the tubes were removed and taken through the drying process to form the aerogel. After drying the R/F samples, the aerogel was characterized by X-Ray Fluorescence (XRF) to analyze the composition of the white precipitate. Since the white precipitate cured in the R/F sample pieces, the white precipitate was analyzed on the XRF instrument. High XRF peaks corresponding to sulfur (or sulfur compounds) were present in the areas of the R/F where the white precipitate was present. Sulfur compounds in the aerogel are undesirable for use for ICF experiments because they increase the laser absorption of the aerogel wall of the capsule. According to Sigma-Aldrich, the PAG was an ionic compound containing a sulfonium ion. The addition of the PAG with the sulfonium ion created a side reaction with the R/F precursor solution forming the white precipitate. The results from this test suggest the PAG for the acid catalysis step of the polycondensation reaction would be better if it was a non-ionic compound. The non-ionic PAG found to work with the R/F formulation was CGI 1907 (Ciba/BASF) shown in figure 4. Despite being a non-ionic, the PAG was insoluble in water but soluble in propylene glycol monomethyl ether acetate (PGMEA). The wavelength the PAG (200-325nm) activates within the range of the UV light source (300-480nm). When exposed to UV light, the PAG forms nonafluoro-n-butanesulfonic acid (nonaflic acid). A 0.2925 M solution of CGI1907 in PGEMA was prepared to use for PAG testing. A small volume of the PAG solution was exposed to UV light and the ph went from 6 to 3. Since the PAG solution was a strong acid when activated by UV light, 10 drops of the PAG solution were added to 15 ml of water. The water with drops from the PAG solution was added to 21 ml of R/F precursor solution. The volumes were based on the starting volume of R/F precursor solution after the base catalysis step, and the volume of diluted benzoic acid added to the precursor solution according to the traditional R/F formulation. To conduct the droplet suspension test, drops of the R/F solution containing the PAG were added to the oil mixture in a vial and exposed to UV light for 5 minutes. As the UV light shines on the R/F drops, the droplets begin to rise to the top of the oil mixture. When the UV light turns off, the R/F droplets return to the original height of suspension, indicating the relative density of the droplets are changing when the UV light was applied. The R/F droplets gelled after 5 minutes of exposure by UV light. The cured beads of R/F were then taken through the post-cure and drying process. Table 1 summarizes the PAGs used and the results from droplet suspension test. Figure 4. The chemical structure of the PAG, CGI 1907 (Ciba/BASF), used in the R/F formulation. GENERAL ATOMICS REPORT GA-A26949 5

K.M. Saito, et al. SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS Table I. Summary of PAGs used in the droplet suspension test. Photo-Acid Generator Solvent Acid Formation 4-Phenylthiophenyl Water Trifluoromethanesulfonic Diphenylsufonium Trifate Acid (Triflic Acid) Dimethyl2,4- Water Trifluoromethanesulfonic Dihydroxyphenylsulfonium Acid (Triflic Acid) Triflate IRGACURE121 CGI1907 PropyleneGlycol MonomethylEther Acetate (PGMEA) PropyleneGlycol Monomethyl Ether Acetate (PGMEA) Gelation Time N/A Comments PAG does not dissolve in water ~12 hrs Forms white precipitate in side reaction with R/F, no change in ph with UV light exposure p-toluenesulfonic Acid 15 min PAG re-crystallizes in R/F precursor solution; PAG particles on surface of R/F after drying Nonafluoro-nbutanesulfonic Acid (Nonaflic Acid) 5 min Fast gelation of R/F with the PAG When removing the R/F beads from the drier, there appears to be a noticeable skin on the surface of the bead and an oily residue surrounding the bead as shown in figure 5. The skin surrounds the surface of the bead, and more apparent when examining the cross-section of the bead. It was possible the PAG in the R/F solution was only activated on the surface of the bead when exposed to UV light. Observing the R/F beads under the microscope, the skin on the beads appear to vary from bead to bead. While curing the R/F beads in the vial with the UV light, only certain areas of the bead were highly exposed to the UV light. Those areas were apparent when removing the R/F beads from the critical point drier. The skin on the beads was more noticeable on one side than the other due to overexposure of UV light. Even though the R/F beads have a skin on the surface, the process proves the PAG in the R/F solution will gel when exposed to UV light. Figure 5. Image of 2 mm R/F bead taken after the drying process. The pore structures were compared using the SEM images shown in figure 6. At 50,000X magnification, the SEM captures the pore structures of the traditional R/F formulation and the PAG R/F. According to the SEM images, the pore structures of the two R/F samples were visually similar. The pore structure for the PAG R/F looks slightly different because of the PAG molar solution made to conduct the droplet suspension test had a higher molar concentration than the benzoic acid used in the traditional R/F formulation. Using a strong acid for the acid catalysis step in the polycondensation reaction can change the pore structure of the foam. The higher 6 GENERAL ATOMICS REPORT GA-A26949

SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS K.M. Saito, et al. PAG molar solution was made to ensure gelation of R/F occurs as fast as possible when exposed to UV light. Figure 6. Side-by-side pore structure comparison of standard R/F and the PAG R/F via SEM. Applying R/F with PAG to DEP In order for the DEP device to be effective, the R/F solution containing the PAG must have a conductivity of 10-3 S/m or lower [10,11]. When testing the R/F solution, the conductivity was 4x10-2 S/m which was well out of the range the DEP device can be used. If the conductivity of the R/F was too high, the DEP was unable to center the double emulsion droplet. Despite the R/F with PAG having a high conductivity, it s not necessarily due to the addition of the PAG. The conductivity of the water, formaldehyde, and base catalyst (sodium bicarbonate) are measured individually before making the precursor solution. As it turned out, the high conductivity was a result of the base catalyst being added in the first step of the poly-condensation reaction [12]. Although the following R/F solution with PAG cannot be used in the DEP device due to the high conductivity, it may still be effective applying the solution to fabricating R/F capsules with the triple orifice droplet generator method. The droplet generator method with PAG in R/F Before using the droplet generator to fabricate R/F capsules, the R/F solution containing the PAG needs to be density matched [6,7]. A hurdle to overcome during density matching the solution was the change in density as the UV light was exposed to the R/F. During the droplet suspension test, it was found the drops of R/F with PAG would rise as the UV light shines on the drops. Since the drops rise with exposure to UV light, the R/F solution and oil mixture were density matched with the density of the oil being lighter than the density of the R/F. After density matching, the R/F solution with PAG, outer oil mixture, and inner oil mixture were hooked up to the triple orifice droplet generator to create shells [4]. The uncured R/F shells rotate in the beaker and are exposed by UV light for 25 minutes. After exposing to UV light, the capsules were taken through the post-cure and drying process. When the capsules come out of the drier, there appears to be a skin on the surface of the shell, but not as severe as the skin surrounding the entire surface of the beads fabricated during the droplet suspension test. Figure 7(a) and 7(b) were examples of a bead and capsule respectively, after the drying process. Since the R/F capsules were in constant motion in the GENERAL ATOMICS REPORT GA-A26949 7

K.M. Saito, et al. SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS rotary beaker, the capsules have a limited amount of exposure to UV light. The UV light was constantly shining on the surface of the outer oil mixture, but only the R/F capsules moving near the top surface of the oil mixture are being exposed. Instead of the capsules being stationary like the beads, the capsules are in constant motion. Thus, the R/F capsules do not have the same type of exposure to UV light as the R/F beads and the skin on the capsule surface was not as extreme as the beads. In figure 8, the SEM image provides a closer look at the skin from a cross-section standpoint. Another hurdle of the R/F capsules being in constant motion was the inner surface of the capsule does not cure. The UV light source uses a light guide to emit UV light as a point source, focusing on a point rather than covering a broad area. By doing this, the UV light only activated the R/F capsules in the limited area the light was focused on. Ideally, the next step is to surround the rotary beaker containing the PAG R/F capsules with UV lamps to have a more uniform exposure of UV light. This may reduce the skin by not overexposing the PAG R/F with UV light and have greater contact with the UV light to gel the inner surface of the capsules. Figure 7. (a) 2mm R/F bead with the PAG CGI 1907. (b) 2mm R/F capsule with PAG CGI 1907. CONCLUSION Figure 8. Cross-section of PAG R/F shell taken by the SEM. The outlined experiments with the substitution of a PAG for benzoic acid as the catalyst in the 2-step polycondensation reaction show an alternative method to synthesizing R/F. Despite 8 GENERAL ATOMICS REPORT GA-A26949

SYNTHESIS OF RESORCINOL FORMALDEHYDE AEROGEL USING PHOTO-ACID GENERATORS K.M. Saito, et al. the presence of skin on the R/F capsules and beads, the pore structure of the PAG R/F was very similar to the traditional R/F formulation. Despite being unable to utilize the DEP device due to the high conductivity from the base catalysis, the PAG R/F still applies to the triple orifice droplet generator method. Future work will include improvement on how the UV light exposes and contacts the R/F capsules during the curing process and optimizing the formulation and droplet generator process to produce usable shells for future ICF experiments using this alternative R/F synthesis. REFERENCES 1. R.W. Pekala, et al., J. Mater. Sci. 24, 3221 (1989). 2. J.D. Sethian, et al., Nucl. Fusion 43, 1693 (2003). 3. J. Perkins, et al., HAPL Program Website: http://aries.ucsd.edu/hapl/docs/hapltargetspecs.doc 4. S.M. Lambert, et al., J. Appl. Polym. Sci. 65, 2111 (1997). 5. A. Nikroo, et al., Fusion Sci. Technol. 45, 84 (2004). 6. R.R. Paguio, et al., Fusion Sci. Technol. 51, 682 (2007). 7. R.R. Paguio, et al., accepted for publication in Fusion Sci. Technol. (2010). 8. H. Pohl, Dielectrophoresis: The Behavior of Neutral Matter in Nonuniform Electric Fields, Cambridge University Press, Cambridge (1978). 9. T. Jones, Electromechanics of Particles, Cambridge University press, New York (1995). 10. Z.-M. Bei, et al., Applied Physics Lett. 93, 184101 (2008). 11. Z.-M. Bei, et al., J. of Electrostatics 67, 173, (2009). 12. R.R. Paguio, et al., this conference. GENERAL ATOMICS REPORT GA-A26949 9