32 research outputs found
Determination of Dew Point Conditions for CO<sub>2</sub> with Impurities Using Microfluidics
Impurities can greatly modify the
phase behavior of carbon dioxide
(CO<sub>2</sub>), with significant implications on the safety and
cost of transport in pipelines. In this paper we demonstrate a microfluidic
approach to measure the dew point of such mixtures, specifically the
point at which water in supercritical CO<sub>2</sub> mixtures condenses
to a liquid state. The method enables direct visualization of dew
formation (∼ 1–2 μm diameter droplets) at industrially
relevant concentrations, pressures, and temperatures. Dew point measurements
for the well-studied case of pure CO<sub>2</sub>-water agreed well
with previous theoretical and experimental data over the range of
pressure (up to 13.17 MPa), temperature (up to 50 °C), and water
content (down to 0.00229 mol fraction) studied. The microfluidic approach
showed a nearly 3-fold reduction in error as compared to previous
methods. When applied to a mixture with nitrogen (2.5%) and oxygen
(5.8%) impuritiesî—¸typical of flue gas from natural gas oxy-fuel
combustion processesî—¸the measured dew point pressure increased
on average 17.55 ± 5.4%, indicating a more stringent minimum
pressure for pipeline transport. In addition to increased precision,
the microfluidic method offers a direct measurement of dew formation,
requires very small volumes (∼10 μL), and is applicable
to ultralow water contents (<0.005 mol fractions), circumventing
the limits of previous methods
Determination of Dew Point Conditions for CO<sub>2</sub> with Impurities Using Microfluidics
Impurities can greatly modify the
phase behavior of carbon dioxide
(CO<sub>2</sub>), with significant implications on the safety and
cost of transport in pipelines. In this paper we demonstrate a microfluidic
approach to measure the dew point of such mixtures, specifically the
point at which water in supercritical CO<sub>2</sub> mixtures condenses
to a liquid state. The method enables direct visualization of dew
formation (∼ 1–2 μm diameter droplets) at industrially
relevant concentrations, pressures, and temperatures. Dew point measurements
for the well-studied case of pure CO<sub>2</sub>-water agreed well
with previous theoretical and experimental data over the range of
pressure (up to 13.17 MPa), temperature (up to 50 °C), and water
content (down to 0.00229 mol fraction) studied. The microfluidic approach
showed a nearly 3-fold reduction in error as compared to previous
methods. When applied to a mixture with nitrogen (2.5%) and oxygen
(5.8%) impuritiesî—¸typical of flue gas from natural gas oxy-fuel
combustion processesî—¸the measured dew point pressure increased
on average 17.55 ± 5.4%, indicating a more stringent minimum
pressure for pipeline transport. In addition to increased precision,
the microfluidic method offers a direct measurement of dew formation,
requires very small volumes (∼10 μL), and is applicable
to ultralow water contents (<0.005 mol fractions), circumventing
the limits of previous methods
Rapid Microfluidics-Based Measurement of CO<sub>2</sub> Diffusivity in Bitumen
In this paper, we demonstrate the first application of microfluidics to study diffusive transport in extra heavy oils, such as bitumen. A cross-channel glass microfluidic chip was used to measure the CO<sub>2</sub> diffusion in Athabasca bitumen. The device was initially filled with CO<sub>2</sub> at low pressure (<1.0 bar). A plug of bitumen was injected into the central (50 μm wide and 20 μm deep) channel and, subsequently, exposed to high-pressure CO<sub>2</sub> on both ends. One-dimensional oil swelling in response to CO<sub>2</sub> diffusion was imaged over time. A simple mathematical approach was applied to calculate the diffusion coefficient based on the oil-swelling data. Measurement results are reported here at a range of pressures (1–5 MPa) and room temperature (21 °C). The measured diffusion coefficients in this range are on the order of 10<sup>–10</sup> m<sup>2</sup>/s, in good agreement with the relevant published data using conventional methods. In sharp contrast to conventional methods that require hours or days and ∼0.5 L of sample, the method presented here requires ∼10 min and a 1 nL plug of sample
Bitumen–Toluene Mutual Diffusion Coefficients Using Microfluidics
In this paper, we present a microfluidic
approach to measure liquid
solvent diffusivity in Athabasca bitumen. The method has three distinguishing
features: (a) a sharp initial condition enabled by the high wettability
of the solvent; (b) one-dimensional diffusive transport (in the absence
of convection) ensured by microscale confinement; and (c) visible-light-based
measurement enabled by the partial transparency of the bitumen at
small scales. The method is applied to measure the diffusion of toluene
into bitumen by imaging transmitted light profiles over time, and
relating intensities to the mass fractions. Plotting toluene mass
fraction versus distance/sqrtÂ(time), results in a tight superposition
of all curves (time-dependent mass fractions) demonstrating the diffusion
dominated nature of the system and the robustness of the method. The
diffusion transport equations were solved and fit to a constant diffusion
coefficient as well as a variety of concentration-dependent diffusion
coefficient relations found in the literature. For intermediate toluene
mass fractions (0.2–0.8), a constant diffusion coefficient
of 2.0 × 10<sup>–10</sup> m<sup>2</sup>/s provides an
appropriate representation. However, at low toluene mass fractions
(<0.2), significantly reduced diffusive transport is observed,
and endpoint analysis indicates diffusion coefficients trending toward
4.3 × 10<sup>–11</sup> m<sup>2</sup>/s. At high toluene
mass fractions (>0.8), the values trend toward 1.5 × 10<sup>–10</sup> m<sup>2</sup>/s. This microfluidic method provides
an inexpensive
and rapid mutual diffusion coefficient evaluation, with significantly
improved spatial/composition resolution vis-à-vis competing
measurement methods
Disposable Plasmonics: Rapid and Inexpensive Large Area Patterning of Plasmonic Structures with CO<sub>2</sub> Laser Annealing
We present a method of direct patterning
of plasmonic nanofeatures
on glass that is fast, scalable, tunable, and accessible to a wide
range of usersî—¸a unique combination in the context of current
nanofabrication options for plasmonic devices. These benefits are
made possible by the localized heating and subsequent annealing of
thin metal films using infrared light from a commercial CO<sub>2</sub> laser system. This approach results in patterning times of 30 mm<sup>2</sup>/min with an average cost of $0.10/mm<sup>2</sup>. Colloidal
Au nanoparticles with diameters between 15 and 40 nm can be formed
on glass surfaces with <i>x</i>–<i>y</i> patterning resolutions of ∼180 μm. While the higher
resolution provided by lithography is essential in many applications,
in cases where the spatial patterning resolution threshold is lower,
commercial CO<sub>2</sub> laser processing can be 30-fold faster and
400-fold less expensive
Morphological Control <i>via</i> Chemical and Shear Forces in Block Copolymer Self-Assembly in the Lab-on-Chip
We investigate the effects of variation in chemical conditions (solvent composition, water content, polymer concentration, and added salt) on the morphologies formed by PS-<i>b</i>-PAA in DMF/dioxane/water mixtures in a two-phase gas–liquid segmented microfluidic reactor. The differences in morphologies between off-chip and on-chip self-assembly and on-chip morphological trends for different chemical conditions are explained by the interplay of top-down shear effects (coalescence and breakup) and bottom-up chemical forces. Using off-chip morphology results, we construct a water content-solvent composition phase diagram showing disordered, sphere, cylinder, and vesicle regions. On-chip morphologies are found to deviate from off-chip morphologies by three identified shear-induced paths: 1) sphere-to-cylinder, and 2) sphere-to-vesicle transitions, both <i>via</i> shear-induced coalescence when initial micelle sizes are small, and 3) cylinder-to-sphere transitions <i>via</i> shear-induced breakup when initial micelle sizes are large (high capillary number conditions). These pathways contribute to the generation of large extended bilayer aggregates uniquely on-chip, at either increased polymer or salt concentrations. Collectively these results demonstrate the broad utility of top-down directed molecular self-assembly in conjunction with chemical forces to control morphology and size of polymer colloids at the nanoscale
Full Characterization of CO<sub>2</sub>–Oil Properties On-Chip: Solubility, Diffusivity, Extraction Pressure, Miscibility, and Contact Angle
Carbon
capture, storage, and utilization technologies target a
reduction in net CO<sub>2</sub> emissions to mitigate greenhouse gas
effects. The largest such projects worldwide involve storing CO<sub>2</sub> through enhanced oil recoveryî—¸a technologically and
economically feasible approach that combines both storage and oil
recovery. Successful implementation relies on detailed measurements
of CO<sub>2</sub>–oil properties at relevant reservoir conditions
(<i>P</i> = 2.0–13.0 MPa and <i>T</i> =
23 and 50 °C). In this paper, we demonstrate a microfluidic method
to quantify the comprehensive suite of mutual properties of a CO<sub>2</sub> and crude oil mixture including solubility, diffusivity,
extraction pressure, minimum miscibility pressure (MMP), and contact
angle. The time-lapse oil swelling/extraction in response to CO<sub>2</sub> exposure under stepwise increasing pressure was quantified
via fluorescence microscopy, using the inherent fluorescence property
of the oil. The CO<sub>2</sub> solubilities and diffusion coefficients
were determined from the swelling process with measurements in strong
agreement with previous results. The CO<sub>2</sub>–oil MMP
was determined from the subsequent oil extraction process with measurements
within 5% of previous values. In addition, the oil–CO<sub>2</sub>–silicon contact angle was measured throughout the process,
with contact angle increasing with pressure. In contrast with conventional
methods, which require days and ∼500 mL of fluid sample, the
approach here provides a comprehensive suite of measurements, 100-fold
faster with less than 1 μL of sample, and an opportunity to
better inform large-scale CO<sub>2</sub> projects
Measurement of CO<sub>2</sub> Diffusivity for Carbon Sequestration: A Microfluidic Approach for Reservoir-Specific Analysis
Predicting carbon dioxide (CO<sub>2</sub>) security and
capacity
in sequestration requires knowledge of CO<sub>2</sub> diffusion into
reservoir fluids. In this paper we demonstrate a microfluidic based
approach to measuring the mutual diffusion coefficient of carbon dioxide
in water and brine. The approach enables formation of fresh CO<sub>2</sub>–liquid interfaces; the resulting diffusion is quantified
by imaging fluorescence quenching of a pH-dependent dye, and subsequent
analyses. This method was applied to study the effects of site-specific
variablesî—¸CO<sub>2</sub> pressure and salinity levelsî—¸on
the diffusion coefficient. In contrast to established, macro-scale
pressure–volume–temperature cell methods that require
large sample volumes and testing periods of hours/days, this approach
requires only microliters of sample, provides results within minutes,
and isolates diffusive mass transport from convective effects. The
measured diffusion coefficient of CO<sub>2</sub> in water was constant
(1.86 [±0.26] × 10<sup>–9</sup> m<sup>2</sup>/s)
over the range of pressures (5–50 bar) tested at 26 °C,
in agreement with existing models. The effects of salinity were measured
with solutions of 0–5 M NaCl, where the diffusion coefficient
varied up to 3 times. These experimental data support existing theory
and demonstrate the applicability of this method for reservoir-specific
testing
Flow-Directed Assembly of Block Copolymer Vesicles in the Lab-on-a-Chip
We demonstrate a microfluidic approach to the production
of block
copolymer vesicles via flow-directed self-assembly in a segmented
gas–liquid device. Chemical conditions that favor spherical
micelles in the bulk are found to yield a nearly pure population of
vesicles on a chipî—¸a transformation of two full morphological
stepsî—¸because of a coalescence mechanism enabled by high shear.
The production of polymeric vesicles via top-down control in a microfluidic
device enables new processing routes to applications including drug
delivery formulations in the lab-on-a-chip
Flow-Directed Loading of Block Copolymer Micelles with Hydrophobic Probes in a Gas–Liquid Microreactor
We investigate the loading efficiencies
of two chemically distinct
hydrophobic fluorescent probes, pyrene and naphthalene, for self-assembly
and loading of polystyrene-<i>block</i>-polyÂ(acrylic acid)
(PS-<i>b</i>-PAA) micelles in gas–liquid segmented
microfluidic reactors under different chemical and flow conditions.
On-chip loading efficiencies are compared to values obtained via off-chip
dropwise water addition to a solution of copolymer and probe. On-chip,
probe loading efficiencies depend strongly on the chemical probe,
initial solvent, water content, and flow rate. For pyrene and naphthalene
probes, maximum on-chip loading efficiencies of 73 ± 6% and 11
± 3%, respectively, are obtained, in both cases using the more
polar solvent (DMF), an intermediate water content (2 wt % above critical),
and a low flow rate (∼5 μL/min); these values are compared
to 81 ± 6% and 48 ± 2%, respectively, for off-chip loading.
On-chip loading shows a significant improvement over the off-chip
process where shear-induced formation of smaller micelles enables
increased encapsulation of probe. As well, we show that on-chip loading
allows off-chip release kinetics to be controlled via flow rate: compared
to vehicles produced at ∼5 μL/min, pyrene release kinetics
from vehicles produced at ∼50 μL/min showed a longer
initial period of burst release, followed by slow release over a longer
total period. These results demonstrate the necessity to match probes,
solvents, and running conditions to achieve effective loading, which
is essential information for further developing these on-chip platforms
for manufacturing drug delivery formulations