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Embedded Self-Circulation of Liquid Reactants for Micro
Fuel Cells
Micro direct methanol fuel cells (mDMFCs) are
widely anticipated as the next-generation high energy density micro power
source for portable electronics and MEMS. However, enormous challenges have
been slowing down its commercialization, including methanol crossover, cathode
flooding, MEA dry-out, and the need for complex peripheral components, which
results in a significant packaging penalty. While electrochemists make
tremendous efforts to improve MEA performance, we believe that MEMS and
nanotechnologhies can provide a comprehensive microfluidic management paradigm
to solve the above-mentioned problems of mDMFCs. A key component of
this microfluidic approach is reactant regulation with integrated compact
structures and little or no power consumption. We have developed a bubble-driven micro pumping mechanism that utilizes
gas byproducts to transport liquid reactants in the micro fuel cell without
consuming electrical power. Moreover, this pumping mechanism can be embedded
into the microchannels of mDMFCs without occupying much of the overall volume, greatly reducing
the packaging penalty. |
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| Bubble motion the pumping section |
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| Measurement of the flow rate
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Continuous mDMFC operation w/o embedded
self-circulation of methanol fuel |
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Universal gas bubble removal by hydrophobic venting
Blocking of microchannels by gas
bubbles has been a daunting problem for microfluidics. Our study shows that
this problem can be solved by making small hydrophobic holes in the wall of a
microfluidic reactor. Ours is the first demonstrated approach that can quickly
remove any gas bubbles from a packaged microfluidic device, whether the gas is
soluble in the solvent or not. The leakage prevention pressure of the
hydrophobic holes is determined by its surface properties and size. By using
hydrophobic nanoporous polypropylene with pore size of ~ 100 nm in radius, we
demonstrated leakage prevention pressure as high as 200 kPa for both water and
10 M methanol. |
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| Principle
of the universal gas bubble removal mechanism by hydrophobic venting
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A
degassing plate with bubble traps and distributed hydrophobic venting
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| A gas-venting microchannel is removing
bubbles from 10M methanol
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Comparative Study of Electrolysis and Boiling for
Bubble-Driven Microactuations
Boiling to generate thermal
bubbles has been the most popular way for bubble-driven microactuation, mainly
because no additional structures are needed for bubble removal. With our
hydrophobic venting technology, it is now possible to remove insoluble gas bubbles
quickly with a very simple structure. Therefore, electrochemically-generated gas bubbles are finally viable
for microactuation, and it is time to reevaluate electrochemical bubbles as
compared to thermal bubbles for bubble-driven microdevices. In this study, we
show that the power consumption of electrolysis microactuation is several
orders of magnitude lower than that of boiling. Analyses of controllability,
bio-compatibility and scaling effects also show the advantages of electrolysis. |

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| Schematic
view of test chips for two kinds of bubble-driven microactuation |
Experimental
results shows lower power consumption and better controllability of
electrolysis actuation
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Bubble Capturing Potential FBc: the Quantity to Evaluate The Surface’s
“Affinity” for Bubbles
It has been demonstrated that gas
bubbles can serve as pressure sensors, imaging particles, signal sources for
MRI, drug delivery vessels, and microlenses. Guided by surface free energy, gas
bubbles in a liquid environment can automatically attach to energetically
favorable locations (bubble-traps) and align into a prescribed array pattern to
perform their functionalities in parallel. In this study, bubble capturing
potential Fbc is proposed as the quantity to evaluate the surface’s “affinity”
for bubbles. A bubble-trap can therefore be viewed as an area with local
maximum Fbc. Two types of bubble-traps are proposed and evaluated. Type I bubble-traps are hydrophobic patterns
on a hydrophilic flat surface. Type II bubble-traps are concave pits surrounded
by a hydrophilic flat surface. Simulation of bubble capturing potential Fbc explains the bubble-capturing
behavior for both cases and predicts better performance for type II
bubble-traps. Experiments agree well with the theoretical prediction and
suggest promising applications. |
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| Bubbles in three-phase system a: floating; b,c and d: attached on different surface structures |
Simulation result of bubble capturing potential |

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| Gas bubbles captured on arrayed type I
bubble-traps
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Gas bubbles captured on arrayed type II
bubble-traps
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