NSF Workshop:
Emerging Opportunities of Nanoscience to Energy Conversion and Storage
Section 4: Nanotechnology for Fuel Cells and
Batteries
by Katsuyo Thornton, John Harb, and Liwei Lin
Introduction
In this section, technologies for
energy conversion and storage based on electrochemistry are considered. As electrochemical systems, fuel cells
and batteries share much in common.
They convert chemical energies into electricity and vice versa. They consist of an anode and a cathode,
separated by an electrolyte (see Figure X-1). A pair of reduction and oxidation reactions results in
electric current generation.
Interfaces are important in their performance since the interfacial
regions are where heterogeneous chemical reactions can take place. Many of the governing physics of
their basic cell components, such as thermodynamics and charge conservation are
identical. Therefore, many of the
issues impeding improvements of fuel cells and batteries are also in
common. Nanoscience can make an
impact in several aspects:
o New
materials with unique properties resulting from nanoscale effects
o Nanofeatures
and structures to enhance performance
o Improved
fundamental understanding of physical mechanisms at the nanoscale
o Nano-derived
methods for manufacturing and assembly
o Multifunctional
materials that include energy storage and generation
Novel materials such as carbon
nanotubes can be useful in electrochemical systems. For example, electrodes
using single-walled carbon nanotubes have been shown to improve performance in
both batteries (Terrones, 2003) and fuel cells (Girishkumar et al., 2005). While this example has a cost
disadvantage, such solutions may be appropriate in specialized applications. Furthermore, interfaces of traditional
materials can exhibit behaviors fundamentally different from those of the bulk
due to the change in the local atomic structure. In nanostructured materials,
the interfacial regions become dominant and closely spaced. As a result, such materials possess
unique properties not observed in the bulk materials. Maier (2005) recently
reviewed the area of nanoionics and its significance to electrochemical systems
in Nature Materials. Indeed, it has already been
demonstrated that nanoscale effects can be exploited to improve electrochemical
systems, as discussed later.
While the issues addressed by
these strategies are shared between the battery and fuel cell systems, there
are fundamental differences between the two in other areas. Since a fuel cell requires the
transport of the fuel through the anode, fluid or gas dynamics are additional
physics governing the system.
Understanding of nanofluidics and gas dynamics at the nanoscale thus
becomes essential in optimizing the design. There is significantly more freedom in designing the 3D
architecture of batteries since, unlike fuel cells, no fuel or waste products
need to be transported into/out of the cell. For example, a battery can be designed with particles or
rods of cathodic material coated with electrolyte material, embedded in a matrix
of anodic material (Long, 2004).
Since battery technologies are relatively mature, especially compared to
that of fuel cells, the breakthrough improvement must consider highly designed
novel architectures, with precisely controlled domain sizes and patterns.
Furthermore, challenges facing conventional fuel cells and non-conventional
fuel cells, such as those based on biosystems or microscale devices, are also
very distinct. Therefore, we will
examine the three aspects, conventional fuel cells, non-conventional fuel
cells, and batteries, in turn, describing the current state-of-the-art,
technological barriers, and possible nanoscience-based approaches to overcome
the barriers.
Conventional Fuel Cells
Fuel cells have the potential to
offer significant efficiency and environmental benefits over todayÕs
traditional energy technologies, but significant cost reductions and efficiency
improvements are necessary for fuel cells to emerge as a practical energy
alternative. The recent National
Research Council/National Academy of Engineering report (2003) on the hydrogen
economy lists the primary barriers to full fuel cell adoption as: (1) cost,
efficiencies, and lifetime of current systems, and (2) the lack of H2
infrastructure and production. In
order for an alternative energy technology to be competitive with conventional
power sources, a target goal of $500/kW and twice the current efficiency must
be achieved. Nanotechnology could
make a dramatic impact by improving the performance and by fulfilling materials
requirements.
The basic principles behind fuel
cells have been known for quite a long time, and the first demonstration of
fuel cell was performed in the late 1830s by Sir William Robert Grove. Since
then, there have been significant developments and demonstrations of various
types of fuel cells. Commercialized units have been realized in some types of
fuel cells (e.g., phosphoric acid fuel cells and molten carbonate fuel cells),
but wider market penetration has not been achieved due to their high cost.
Thus, the fate of conventional fuel cells depends not on the feasibility, but
rather on cost effectiveness of the systems and their operation. While the total cost per unit of
electricity generated is the ultimate metric of the issue, there are several
metrics that directly influence it.
These are:
Which of these sources hinder the success of fuel
cells depend on the type of the fuel cell. There are many conventional fuel cell approaches, and not
all of them are discussed here. Of
those, the solid oxide fuel cells (SOFCs) for large-scale power generation and
the proton exchange membrane fuel cells (PEMFCs, also known as the polymer
electrolyte fuel cells) for smaller scale applications are considered to be
promising approaches. The sources of high cost of these two types of fuel cells
are quite different. For example,
a SOFC has a disadvantage of very high operation temperature, requiring
expensive components especially in interconnects. A PEMFC, on the other hand, must rely on highly efficient,
expensive catalysts. The issues
associated with the SOFCs are reviewed first, followed by those of the PEMFCs.
Solid Oxide Fuel Cells
The SOFCs are fuel cells with solid, nonporous
electrolyte of metal oxide such as yttria-stabilized zirconia. They have advantages over other types
of fuel cells, including their solid construction allowing design simplicity,
ability to directly use unreformed fuel, and potential for very high
efficiency. Thus, significant research and development efforts are underway to
bring this technology to commercial reality (see, for example, Kendall (2005)
and Holtappels, Vogt, & Graule (2005) for the overview). DOEÕs Solid State Energy Conversion
Alliance (SACA) Program is aiming to develop a market-ready SOFC with $400/kW
cost by 2010 (Solid State Energy Conversion Alliance, 2005), a factor of ten
reduction during the ten-year program.
Although sub-MW systems are possible (Minh, 2004), the SOFC technology
is most advantageous in large-scale power generation because a very high
efficiency (up to 70%) can be achieved when a gas turbine is combined with the
fuel cell system.
The major disadvantage of the
SOFCs is the high operating temperature, which increases the materials cost and
shortens the cell life, resulting in a high overall cost. The currently demonstrated SOFC systems
typically operate around 1000ûC, barring the use of inexpensive metal-alloy
interconnects. Therefore, the
major effort has been geared toward lowering the operating temperature. The
main reason for this high operating temperature stems from the low ionic
conductivity of the ion-conducting materials and decreased cathodic reaction
rate at low temperatures. To
address the conductivity, nanostructured fuel cell materials have recently been
shown to possess enhanced conductivities of both ions and electrons at much
lower temperatures (Kosacki et al., 2005). Nanostructured electrodes are also advantageous because they
provide larger reactive regions (i.e., three-phase boundaries and surface/interfacial
areas). For example, it has been
demonstrated that nanostructured electrodes have increased transport
efficiencies and decreased energy loss (Liu, Zha, & Liu, 2004; also see
Fig. X-2.). Thus, nanostructured
composites are a promising alternative to standard electrodes. In order to optimize the
electrochemical performance, the relationship between the composite structure
and the electrochemical performance must be identified. To this end, electrochemistry at the
nanoscale and the effects of microstructural characteristics on electrochemical
kinetics must be understood.
Furthermore, fabrication methods must provide sufficient control of the
microstructure such that desired nanoscale structures can be manufactured at a
reasonable cost.
While nanocomposite electrodes
offer significant benefits, these benefits are accompanied by enhanced
diffusivity and reduced characteristic length scale of the composite
structure. This will likely affect
the stability of the nanostructures during operation, and performance
degradation over the expected long lifetime is still a major concern even at
lower temperatures. Therefore,
various diffusion mechanisms occurring in these nanostructured materials (i.e.,
surface diffusion, grain boundary diffusion, etc.) must carefully be
characterized, and their consequences understood. Simulations of microstructural evolution play an important
role in this area due to experimental difficulties associated with long-term
usage. Such simulations must be
accompanied by experiments for validation. Furthermore, either experiments or first principle
calculation may be necessary in order to obtain realistic material properties
needed in the calculation.
Proton Exchange Membrane Fuel Cells
The PEMFCs have proton conductor
membranes made of fluorinated sulfonic acid polymer or another similar polymer
as the electrolyte. This type of
fuel cells is attractive for both transportation and smaller-scale stationary
applications due to its high efficiency, low operation temperature, low pollutant
emission, and relatively compact size.
In particular, for consumers, the PEMFCs with power output in the range
of one to a few hundred kW are ideal alternatives for distributed power for
either industry or residential buildings.
They are also well suited for applications where quick start-up and
quick response to load changes are required (e.g., auxiliary power systems),
and where high power density and low operating temperature (permitting
intermittent operation without significant energy loss) are beneficial.
Despite the apparent benefits
offered by the PEMFC technology, it requires affordable solutions for its key
components. The high capital cost
for PEM fuel cells is by far the largest factor limiting market penetration. Exploration of novel material
alternatives could result for lower-cost components (cost reduction), higher
power density output (increased efficiency), as well as increased durability. Nanostructured materials, including
nanoparticle catalysts, have played an important role in advancing the PEMFC
technology. However, achieving the
goal of a practical PEMFC system will require further investigations of
nanoscale materials for producing the membrane-electrode assembly unit,
including nanocomposite-based proton-exchange membranes, low cost nanoscale low/non-Pt alloy catalysts, and nanostructured electrodes optimized for high performance, cost-effective PEMFC
systems. A variety of recently
engineered nanostructured materials useful in these areas are reviewed by
Malinauskas, Malinauskiene, & Ramanavicius (2005). Fundamental understanding of nanoscale
physics, especially in the area of electrochemistry and catalysis, is essential
in these investigations. First
principle calculations and other types of simulations are often useful in
research for catalytic materials.
For example, Kandoi et al. (2004) applied the periodic density
functional theory combined with a microkinetic model to explain the selectivity
of various catalysts for CO oxidation.
Both
hydrogen and hydrocarbon fuels may be used for PEMFCs. Direct hydrocarbon fuel cells, such as
those using methanol, are a relatively new development and face problems absent
in hydrogen-fueled PEMFCs. For
example, methanol crossover through the electrolyte is a major problem especially
since blocking the methanol transport can also hinder proton conduction. Nanocomposite membranes containing
nanoparticles have been intensively investigated in the recent years (see for
example Choi, et al., 2004 and references therein). While hydrogen-fueled PEMFCs do not suffer from this
problem, they face challenges in hydrogen fuel generation and storage. There are various approaches to
hydrogen production, including those using nuclear energy, coal, and natural
gas. Since producing hydrogen from
hydrocarbons then using the hydrogen as fuel introduces significant
inefficiency, electrolysis using solar energy, and possibly wind energy to a
limited scale, is likely the most environmentally friendly method, eliminating
direct and indirect emission of carbon dioxide from hydrogen-fueled fuel
cells. In the short term, however,
alternative sources must be identified.
The detailed examination of the technologies associated with hydrogen
production is beyond the scope of this report. A few examples of nano-based approaches are catalytic synthesis
of H2 from hydrocarbons, hydrogen production based on biological
systems, and nano-photoelectrochemical systems for solar-energy based
production. The opportunities in
new materials for hydrocarbon processing were reviewed by Farrauto, et al.
(2003). The solar energy
technology is discussed elsewhere in this report. The challenges associated with bio-based hydrogen generation
were discussed by Angenent, et al. (2004). Possible hydrogen storage methods range widely from
pressurized gas or cryogenic liquid cylinders to absorbers using novel
materials such as carbon nanotubes (Terrones, 2003 and references therein),
metal-organic frameworks and metal hydrides (Fichtner, 2005 and references
therein). The development of a
practical system is extremely challenging due to the high diffusivity, low
density, and high flammability of hydrogen. The absorber-based storage technology is still in its
exploratory phase, and its feasibility has yet to be determined. While the success of research in this
area remains to be seen, nanoscience impact on novel storage material can be
the breakthrough required for the success of hydrogen-fueled fuel cells,
especially for transportation applications, where hydrogen safety must meet
higher standards.
Non-Conventional Fuel
Cells
While exploratory, there
has been research toward developing novel types of fuel cells. As examples, two possibilities where
nanoscience may play a significant role are discussed below.
Micro
Fuel Cells
Most
ongoing fuel cell research and development are targeted at the types of fuel
cell technologies discussed above, which are limited to large-scale
applications such as generation of industrial and residential power or
automotive power. At much smaller scales, devices are currently powered by
batteries. The disadvantage of
battery power is the need for electricity for recharging, which may not be
available in some instances, and relatively large weight for both rechargeable
and non-rechargeable batteries.
For micro fuel cells, possible fuels such as methanol or alcohol have
high power per unit mass and per unit volume and may easily be carried. Furthermore, micro fuel cells may offer
significantly higher power densities.
The possible applications may include powering much smaller devices (such
as microelectromechanical devices and Òlabs on chipsÓ), as well as standard
hand-held electronic devices (such as cell phones).
Micro
fuel cells may be based on PEM fuel cell technology or similar, which are
discussed above. However, the
design cannot simply be scaled down since additional challenges will result
from much smaller construction (Maynard & Meyers, 2002). Additionally, most of the portable
applications will be for the end-users, and therefore the design requirements
include a light, compact, stand-alone package that is user-friendly. Thus, fuel, waste, and thermal
management (FWTM) transparent to the users is important in this case (Cowey,
Green, Mepsted, & Reeve, 2005).
Similarly, for microscale applications such as those for the lab-on-chip
technology, FWTM devices, including pumps and heat exchangers, must also be
designed, fabricated, and operated at the microscale. Nanoscience will certainly play an important role in such
devices.
As
in the standard PEM fuel cells, fuel cells of this type will likely depend on
highly efficient catalysts that enable the utilization of liquid fuels. Nano-derived materials will likely be
the answer to the quest for such material, as discussed earlier. Furthermore, successful development of
micro fuel cells will require fundamental understanding of fluid flow, as well
as electrochemical transport, at very small scales. For example, small-scale geometries can result in new
phenomena in fluid flow (Stone, Stoock, & Ajdari, 2004 and references therein),
such as the reduction of friction resulting from surface roughness of the flow
boundary (Cottin-Bizonne, et al., 2003).
Consequently, the validity of the standard descriptions of underlying
physics must be examined. Although
electrochemisty at the nanoscale is universally important in predicting the
performance of such novel devices, the knowledge has not been fully
developed. Thus, testing and
modifying the standard continuum equations and boundary conditions against
experiments in micro/nanofluidic devices are essential in this endeavor. Furthermore, understanding of
electro-osmotic flows is important since removing wastewater, which is in
liquid form in the low temperature environment that these systems must operate,
is difficult. As for other nanoscale
devices, fabrication of nanofluidic devices poses a challenge, and both
top-down and bottom-up methods of nanostructural assembly should be given
considerations. A combination of
top-down and bottom-up approaches, where a top-down approach such as
lithography is used to control a bottom-up self-assembly, may be particularly
promising (Mijatovic, Eijkel, & van den Berg, 2005).
Bio-Based
Fuel Cells
Continuous
and long-term power supply generated directly from biological organisms will
have great impact for systems of all dimensions, starting from nanotechnology,
to microsystems, and to macro scale devices. Nano and micro systems, such as sensors or actuators,
requires power for operation. In
futuristic applications, for example, diagnosing medical problems and
delivering drugs from inside the body has been a dream of doctors since Isaac
Asimov's 1966 science fiction classic ÒFantastic Voyage,Ó in which a group of
doctors were miniaturized and injected into a patient to remove a blood
clot. Doctors cannot be shrunk,
but any future engineering device that resembles the Òfantastic voyageÓ will
require power supply. On the other
hand, in the macro scale, implantable medical devices such as spinal cord stimulator
and drug delivery devices used in spinal drug infusion therapy for pain relief
applications require battery power.
All of the above current and future systems from nano to macro size will
benefit from the generation of renewable power sources from biological
processes.
Figure X-3. Harness power
from nature. Photosynthesis
process in green plants converts CO2 and H2O into glucose
(C6H12O6) with the assistance of light. The aerobic respiration process in
living things such as the butterfly shown in the figure consume and convert
glucose and oxygen into CO2 and H2O. One possibility is
to learn from nature and apply engineering approaches to generate and extract
energy from the natural processes as the power sources for artificial machinery
or systems.
We can take the
lesson from the energy cycle from ÒnatureÓ as illustrated in Figure X-3. The energy of light coming from the Sun
assists the photosynthetic process in green plants to convert carbon dioxide
(CO2) and water (H2O) into glucose as:
(1)
Glucose is the
common energy source for living things, including human, and can be considered
as the ÒlargeÓ energy storage unit.
Animals take green plant as the food for glucose support and convert
glucose and oxygen into carbon dioxide, water and ATP (adenosine triphospate)
in the aerobic respiration process.
This can be conceptually expressed as:
(2)
ATP is considered
as the ÒsmallÓ energy storage unit and acts as ÒcurrencyÓ in all energy
transformation in cells. Both the
photosynthesis and aerobic respiration processes happen every second and
everywhere on earth from living things as big as a whale to as small as a
single cell. They are not only the
very fundamental processes for energy conversion but also indispensable
processes for the supply of oxygen for living animals. One energy possibility is to extract
energy from these energy translation processes by building up artificial fuel
cells to interact with living bacteria cells for engineering applications, such
as to power nano or micro devices.
Moreover, because these processes actually occur at the cellular level,
they are perfect for potential power sources for nano and micro systems and
even for large systems.
Enzymatic fuel
cells use enzymatic break down of fuels such as glucose rather than the
metabolic activity of live microorganisms but otherwise perform the same
function as microbial fuel cells (Halme, Zhang, & Ranta, 2000). Researchers have used glucose, lactate,
and even sewage as organic fuels, and glucose oxidase and lactate dehydrogenase
as the enzyme biocatalyst (Liu, Ramnarayanan, & Logan, 2004; Wiltner &
Katz, 2000). Although diffusional
redox mediators have been used, more recent research has centered on enzymes
and redox mediators covalently linked to each other and to the anode (Katz,
Shipway, & Wiltner, 2003; Wiltner & Katz, 2000; Chen, et al.,
2001). This Òbioelectrocatalytic
wiringÓ of enzymes and mediators to the electrode (versus diffusional enzymes
and mediators) has produced current densities as high as hundreds of
microamperes per square centimeter (Katz, Shipway, & Wiltner, 2003). A complementary bioelectrocatalytic
enzyme system at the cathode accepts the electrodes from the anode to complete
the circuit.
In
both cell- or enzyme-based bio fuel cells, two principle factors are limiting
output and efficiency: (1) the ÒslowÓ and ÒrandomÓ diffusional transport of
active substances and redox mediator in solution and (2) sensitivity of the
redox mediator to oxidation by O2. Nanotechnology could provide a unique solution to at least
the diffusion-limited process. In
order to reduce the current-limiting effects of using a diffusional electron
mediator in conjunction with the cells or enzymes that are also in a
diffusional state in solution, one concept is to immobilize cells or enzymes
onto a gold electrode functionalized with biological self-assembled monolayers
– nanotechnology by nature.
It is postulated that such Òbio-wiringÓ of cells/enzymes to the
electrode would facilitate direct transfer of electrons from cells/enzymes to
the electrode, which would remedy both the current-limiting issues. The improvement in efficiency has been
demonstrated in the case of enzymatic fuel cells. Figure 2 shows the possible architecture based on
ÒnanotechnologyÓ that could improve the efficiency of cell-based fuel cells. This architecture adopts a surface
technique pioneered by Katz and Willner (Wiltner & Katz, 2000; Wiltner,
2002): covalently linking the electron mediator pyrroloquinoline quinone (PQQ)
to a gold electrode functionalized by a monolayer of cystamine as illustrated
in Fig. 2. The PQQ monolayer is
anchored to the gold electrode by sulfur.
We recognize that this is merely one example that nanotechnology could
be used in fuel cell development; there could be many other possibilities that
should be further explored.
Figure
X-4. Bioelectronic wiring of cystamine/PQQ/NADP+ and
cystamine/thylakoids the gold electrode; thylakoids are not shown to scale
relative to PQQ, NADP+, and cystamine. Interpreted and adapted from (Wiltner, 2000; Wiltner, 2002)
for use with PFC.
Batteries
Batteries represent a critical component of almost any
advanced energy strategy, whether for transportation or baseline energy from
non fossil fuel sources (e.g. solar).
In addition, batteries enable mobile applications such as cell phones,
lap top computers, and a host of others.
We also look to batteries to enable a new generation of technologies
that include autonomous microsensing systems and micro implants for biomedical
applications. In
applications for which they are the enabling factor, batteries are often the
limiting factor, and frequently represent the largest and/or heaviest component
of the system. This report
explores ways in which nanoscience and technology can be used to enhance
battery performance.
In order to understand the
potential contributions of nanoscience to battery technology, it is important
to understand the physical processes that determine battery performance. Figure harb1 is a schematic diagram that
illustrates a Li-ion battery.
Lithium batteries represent the largest segment of the portable battery
industry and dominant battery in the computer, cell phone, and camera markets
(Whittingham, 2004). In the
charged state, the amount of lithium is low in the cathode and high in the
anode. Upon discharge, lithium
ions are released from the active material in the anode (typically carbon) and
move through the electrode and separator to the cathode where they are
incorporated into the cathode material.
The release of lithium ions at the anode during discharge is accompanied
by the concurrent release of electrons, which travel through the conductive
network to the anode current collector and from there to the external
circuit. Similarly at the cathode,
electrons travel from the current collector through the conductive network to
the active material where they are ÒconsumedÓ in the reduction reaction as
lithium ions are incorporated into the cathode active material (e.g. CoO2). Some of the physical phenomena
important to this process as well as to the opposite (charging) process
include:
Although their relative importance varies from system to
system, the same general physics are operative for all battery systems. As we examine ways in which nanoscience
can influence battery behavior, we will look for nanoscale behavior that
influences the physical processes listed above.
Battery performance metrics include the specific energy
(Wh/kg), energy density (Wh/l), specific power (W/kg) and power density
(W/l). Values of these metrics for
common primary (single use) and secondary (rechargeable) battery systems are
shown in Figs harb2 and harb3, respectively (Winter, 2004). As a rule of thumb, the practical
energy density of a battery is approximately 25-50% of its theoretical value
owing to the mass/volume of the inert components in a practical system,
irreversible losses and incomplete utilization of the active material in the
battery (Winter, 2004).
Other relevant performance characteristics include cycle life, shelf
life and cost.
The balance of this section will examine ways in which
nanoscience/technology can be used to enhance battery performance. Strategies include: 1) the development
of new materials whose properties are derived from unique nanoscale physics, 2)
the use of nanofeatures and structures to improve the performance of existing
materials, 3) enhancement of our fundamental understanding of nanoscale
processes to enable optimization of existing energy storage devices and the
development of new devices, 4) the development of new nano-derived methods for
manufacturing and assembly of energy storage materials and devices, and 5) the
development of multifunctional engineering materials designed for specific
applications that involve electrochemical energy storage (see Section xx.xx).
Materials
One opportunity for the
improvement of batteries through nanoscience/technology is the exploitation of
unique nanoscale physics to yield materials with improved performance and/or
reduced cost. For example,
Xu et al. demonstrated qualitatively different behavior of electrode materials
at the nanoscale (Xu, 2005). In
one case they demonstrated markedly improved electrochemical behavior for
nanostructured a-Fe2O3 relative to microscale samples of
the same material, where the amount of intercalated lithium increased from 0.03
Li per formula (micro) to 0.47 Li per formula (nano). In another example, electrochemically inactive Li2MnO3
was made active by creating a nanostructured material. These examples illustrate how
phenomena at the nanoscale can lead to a wider selection of suitable materials,
including materials that are less expensive and more environmentally friendly.
The unique characteristics of
nanomaterials have been used in other ways to improve battery performance. Lin and Harb used carbon nanotubes as
the conductive filler in the cathodes of lithium ion batteries (Lin,
2004). They found that the
resistance of electrodes fabricated with single-walled nanotubes was
significantly lower, even without compression, than that of electrodes made
with a traditional carbon black filler, (Fig. harb4). The
performance enhancement due to nanotubes was attributed to the high aspect
ratio of the conductive tubes which facilitated the formation of a conductive
network, and the small size of the nanotubes that allowed them to surround and
make multiple contacts to the larger microsized active material. Unfortunately, the cost of nanotubes
prohibits their use in large commercial batteries. However, they may be useful for microbatteries where the
materials cost is not the driving issue, and where the enhanced performance
without compression is of particular benefit. Because of the very high cost of nanotubes, the opportunity
exists for the development of a low cost, highly conductive, high aspect ratio,
nanosized material for use in batteries of all sizes.
The above materials examples were
focused on improvement of todayÕs best technology. In addition, it may be possible to use
nanoscience/technology to develop completely new types of battery materials or
even new types of battery systems.
Nanostructures
While the previous section
examined the use of materials whose unique properties were derived from the
nanoscale, this section examines the use of nanofeatures or nanostructures
where the physics are essentially the same as for the larger material, but the
performance is enhanced due to the structure. An example of the impact of structure on battery
performance is found in the microbattery work by Humble (2001, 2003). Optimization of deposition conditions
for the cathodic material increased the capacity and rate capability of the
cell by well over an order of magnitude.
Sides et al. (2002, 2005)
prepared nanostructured electrodes for lithium-ion batteries with use of a
porous template. The resulting
electrodes were highly porous, had a very high surface area, and showed
dramatically improved performance on a per mass basis over traditional
electrodes (Fig. harb5). In particular, it was
possible to discharge the electrodes at a very high rate relative to the amount
of active material present.
Unfortunately, template synthesis is tedious and likely expensive on the
large scale. In addition, the
capacity per area is small owing to the thin porous layers that are
formed. Efforts to increase the
capacity have resulted in significant improvements (Sides, 2002), but have yet
to reach levels practical for large cells.
A novel 3D nanostructured battery
was recently proposed by Long et al. (2004) where a very thin electrolyte layer
is formed around a random 3D network of electrode material (Fig. harb6) (see also Rhodes, 2004). The other electrode would then fill the space that
surrounds the electrolyte (see Fig. harb6). All battery components-
anode, cathode and electrolyte- are continuous throughout the Òsponge-likeÓ
structure. A key advantage
of the 3D battery is the short transport distance between the anode and
cathode. However, there is
likely a practical limit to how thick such a battery may be fabricated. Effective distribution of current
throughout the 3D structure will also be challenging for some battery
chemistries. In spite of the
challenges, this type of battery structure represents a departure from
traditional battery fabrication and, if enabled by the appropriate
nanostructures, may make a significant impact. Other types of 3D batteries with micro rather than nano
structures have also been proposed (Ryan, 2003; Long, 2004).
The are other examples of
nanostructured battery materials in the literature (e.g., Fey, 2005; Treger,
2005). For example, LiFePO4
is a relatively new active material for Li-ion batteries whose viability
depends on its nanostructure in order to overcome significant transport
limitations in the solid phase (Treger, 2005).
In summary, nanostructures can be
used to significantly enhance battery performance. The cost and limited capacity per area represent
formidable challenges for the application of some structures to large
commercial markets.
Fundamental Understanding at
the Nanoscale
Another way in which
nanoscience/technology can help advance energy storage technologies is through
the development of improved understanding of the nanoscale processes that
impact the behavior of practical systems.
A fundamental understanding of these processes will lead to new
strategies to enhance battery performance.
An example of an area where
additional understanding is needed is the solid electrolyte interface (SEI)
that forms primarily in the anode of lithium ion batteries (Christensen, 2004;
Aurbach, 2005). This layer forms
by reaction with the electrolyte and grows until electrons can no longer
effectively get to the reaction site due to the insulating nature of the
layer. Although electronically
insulating, the layer readily conducts lithium ions. Thus, lithium ions are transferred from the electrolyte,
through the SEI, to the electrode where they are reduced during charging. Failure to form a stable SEI greatly
reduces the cycle life of the battery.
Changes to the SEI during cycling also reduce the battery lifetime. A fundamental understanding of the
processes that control the formation and stability of the SEI will lead to the
formation of improved SEI layers, and perhaps to the development of an
artificial SEI nanolayer.
There are other aspects of
batteries where our fundamental understanding at the nanoscale is lacking. In addition, fundamental understanding
of new types of electrochemical systems that may contribute to energy storage
in niche areas is needed (e.g., see Long, 2004).
Nanofabrication
One of the reasons that nanotechnology
has received so much attention recently is the promise that it holds for
efficient cost-effective manufacturing techniques (Schulte, 2005). The application of such techniques to
battery fabrication has the potential to make a significant impact. For example, it may be possible to utilize nanotechnology to
fabricate active materials for lithium batteries. However, the performance of these active materials not only
depends on the composition of the material, but also on the material structure
(Whittingham, 2004). Thus,
care must be taken to produce a material with a structure suitable for battery
use.
Kawamura et al. (2005) used
nanofabrication to produce nanostructured LiCoO2 particles (Fig. harb7), and were able to produce particles with an active
crystalline phase. As a result,
they observed a two-fold increase in capacity at high rates, and significantly
improved voltage profiles.
It seems possible that nanofabrication can be used to both reduce
fabrication costs and enhance the performance of some battery materials.
Multifunctional Materials
A final area where nanotechnology
may influence energy storage is in the creation of multifunctional
materials. An example of such a
material is an airplane wing that also serves as the battery to store
energy. The vision of this
multifunctional material is that it is more than just a wing that contains a
battery. Rather, the same
materials used to form the battery are also the structural components of the
wing. There are undoubtedly other
multifunctional concepts to be developed, and examples of such materials are
yet to be found.
Summary
An understanding of the processes
that govern battery behavior can be combined with recent advances in
nanoscience/nanotechnology to create new and improved energy storage devices
for the next generation.
Opportunities exist in at least five different areas as described
above.
Figure harb1.
Schematic diagram of lithium-ion battery. Black- conductive carbon filler, Red Outline- anode active
material, Blue Outline- cathode active material (binder not shown).
Current Collector
Figure harb2.
Energy storage capability of common commercial primary battery systems
(Winter, 2004).
Figure harb3.
Energy storage capability of common rechargeable battery systems
(Winter, 2004).
Figure harb4.
Influence of carbon nanotubes on internal resistance of a lithium-ion
cathode (Lin, 2004).
Figure harb5.
Scanning electron micrograph of a template-synthesized V2O5
electrode prepared from 50-nm pore diameter polycarbonate template membranes
(Sides, 2002).
Figure harb6.
ÒSpongeÓ architecture for 3D nanobattery (Long, 2004).
Figure harb7.
Nanostructured LiCoO2 powders for lithium ion batteries
(Kawamura, 2005).
References
for this section (Alphabetical; formats not completely consistent):
Aurbach, D. (2005) ÒA review on new
solutions, new measurements procedures and new materials for rechargeable Li
batteries.Ó Journal of Power Sources, 146:71-78.
Angenent, L.T., Karim, K., Al-Dahhan, M.H.,
Wrenn, B.A., Domiguez-Espinosa, R. (2004). Production of bioenergy and
biochemicals from industrial and agricultural wastewater. Trends in
Biotechnology, 22:477-485.
T. Chen, S. C. Barton, G. Binyamin, Z. Gao,
Y. Zhang, H.-H. Kim, and A. Heller, "A Miniature biofuel cell," J.
Am. Chem. Soc., vol. 123, pp. 8630-8631, 2001.
Choi, W.C., Jeon, M.K., Kim, Y.J., Woo, S.I., & Hong, W.H. (2004).
Development of enhanced materials for direct-methanol fuel cell by
combinatorial method and nanoscience. Catalysis Today
93–95:517–522.
Christensen, J., Newman, J. (2004). ÒA Mathematical Model for the
Lithium-Ion Negative Electrode Solid Electrolyte Interphase.Ó Journal of the Electrochemical Society,
151(11):A1977-A1988.
Cottin-Bizonne, C., Barrat, J.L., Bocquet,
L., Charlaix, E. (2003). Low-friction flows of liquid at nanopatterned
interfaces. Nature Materials, 2:237-240.
Energy Information Administration (2003).
ÒCommercial Buildings Energy Consumption Survey.Ó http://www.eia.doe.gov/emeu/cbecs/contents.html.
Farrauto, R., Hwang, S., Shore, L.,
Ruettinger, W., Lampert, J., Giroux, T., Liu, Y., & Ilinich, O. (2003). New
material needs for hydrocarbon fuel processing: Generating hydrogen for the PEM
fuel cell. Ann. Ri. Materi. Res., 33:1-27.
Fey, G.T., Lu, C., Huang, J., Kumar, T.P.,
Chang, Y.C. (2005).
ÒNanoparticulate coatings for enhanced cyclability of LiCoO2 cathodes.Ó
Journal of Power Sources, 146:65-70.
Fichtner (2005). ÒNanotechnological aspects
in materials for hydrogen storage.Ó Advanced Engineering Materials, 7:443-455.
Girishkumar G, Rettker M,
Underhile R,
Binz D, Vinodgopal K,
McGinn P,
Kamat P
(2005). ÒSingle-wall carbon nanotube-based proton exchange membrane
assembly for hydrogen fuel cells.Ó Langmuir,
21: 8487-8494.
A. Halme, X. Zhang, and A. Ranta, "Study of biological fuel
cells," in Proc. 2nd
Annual Advances in R&D: The Commercialization of Small Fuel Cells and
Battery Technologies for Use in Portable Applications, New Orleans, USA, 2000
Hart, R.W., White, H.S., Dunn, B. and Rolison, D.R. (2003), Ò3-D
Microbatteries,Ó Electrochemistry Communications, 5:120-3.
Holtappels, P., Vogt, U., & Graule, T. (2005). Ceramic materials
for advanced solid oxide fuel cells. Advanced Engineering Materials, 7:292-302.
Humble, P.H., Harb, J.N. and LaFollette,
R.M. (2001), "Microscopic Nickel-Zinc Batteries for Use in Autonomous
Microsystems ", J. Electrochem. Soc.,
vol. 148, p. A1357.
Humble, P.H. and Harb, J.N. (2003),
ÒOptimization of Nickel-Zinc Microbatteries for Hybrid Powered Microsensor
Systems,Ó J. Electrochem. Soc.,
150, A1182.
E. Katz, A. N. Shipway, and I. Willner,
"Biochemical fuel cells," in Handbook of Fuel Cells -
Fundamentals, Technology and Applications,
vol. 355-381, W. Vielstich, A. Lamm, and H. A. Gasteiger, Eds. Chichester, West
Sussex: John Wiley & Sons, 2003.
Kandoi S., Gokhale, A.A., Grabow, L.C.,
Dumesic, J.A., & Mavrikakis, M. (2004). Why Au and Cu are more selective
than Pt for preferential oxidation of CO at low temperature . Catal. Lett.
93:93–100.
Kawamura, T., Makidera, M., Okada, S.,
Koga, K., Miura, N., Yamaki, J. (2005). ÒEffect of nano-size LiCoO2 cathode powders on Li-ion cells.Ó
Journal of Power Sources, 146:27-32.
Kendall, K. (2005). ÒProgress in solid oxide fuel cell materials.Ó
International Materials Reviews, 50:257-264.
Kosacki, I., Rouleau, C.M., Becher, P.F., Bentley, J., & Lowndes,
D.H. (2005). ÒNanoscale effects on the ionic conductivity in highly textured
YSZ thin films.Ò Solid State Ionics, 176:1319-1326.
Lin, Q. and Harb, J.N. (2004),
ÒImplementation of a Thick-Film Composite Li-Ion Microcathode using Carbon
Nanotubes as the Conductive Filler,Ó J. Electrochem. Soc., vol. 151, A1115.
H. Liu, R. Ramnarayanan, and B. E. Logan,
"Production of electricity during wastewater treatment using a single
chamber microbial fuel cell," Environ. Sci. Tech., vol. 38, pp. 2281-2285, 2004.
Liu, Y., Zha, S., & Liu, M. (2005). Novel nanostructured electrodes
for solid oxide fuel cells fabricated by combustion chemical vapor deposition (CVD). Adv. Mater., 16:256-260.
Long J.W., Dunn, B., Rolison, D.R., White, H.S., Three-dimensional
battery architectures. Chemical Reviews, 104:4463-4492.
Maier, J. (2005). ÒNanoionics:
ion transport and electrochemical storage in confined systems.Ó Nature Materials, 4:805-810.
Malinauskas, A., Malinauskiene,
J., & Ramanavicius, A. (2005). ÒTopical Review: Conducting polymer-based
nanostructurized materials: electrochemical aspects.Ó Nanotechnology,
16:R51-62.
Maynard, H.L. & Meyers,
J.P. (2002). Miniature fuel cells for portable power: Design
considerations and challenges. Journal of Vacuum Science
& Technology B, 20:1287-1297.
Mijatovic, D., Eijkel, J.C.T.,
& van den Berg, A. (2005). Technologies for nanofluidic systems: top-down vs.
bottom-up - a review. Lab on a Chip, 5: 492-500.
Minh, NQ. (2004). ÒSolid oxide
fuel cell technology – features and applications.Ó Solid State Ionics,
174:271-277.
National Research Council and National Academy of Engineering (2004).
The Hydrogen Economy: Opportunities, Costs, Barriers, and R&D Needs.
National Academy Press, Washington DC.
Rhodes, C.P., Long, J.W., Doescher, M.S.,
Fontanella, J.J., Rolison, D.R. (2004).
ÒNanoscale Polymer Electrolytes:
Ultrathin Electrodeposited Poly(Phenylene Oxide) with Solid-State Ionic
Conductivity.Ó J. Phys. Chem. B, 108(35):13079 -13087.
Schulte, J. (2005), Nanotechnology,
J. Wiley & Sons, Sussex, England.
Sides, C.R., Li, N., Patrissi, C.J.,
Scrosati, B., Martin, C.R. (2002).
ÒNanoscale Materials for Lithium-Ion Batteries.Ó MRS Bulletin,
27(8):604-607.
Sides, C.R., Martin, C.R. (2005). ÒNanostructured Electrodes and the
Low-Temperature Performance of Li-Ion Batteries.ÓAdv. Mater, 17(1):125-128.
Solid State Energy Conversion Alliance (2005). http://www.seca.doe.gov/
Stone, H.A., Stroock, A.D., & Ajdari, A. (2004). Engineering flows in small devices: Microfluidics toward a
lab-on-a-chip. Annual Review
of Fluid Mechanics 36:381-411.
Terrones, M. (2003). ÒScience and Technology of the Twenty-First
Century: Synthesis, Properties, and Applications of Carbon Nanotubes.Ó Annu.
Rev. Mater. Res., 33:419–501
Treger, J., Thomas-Alyea, K. and Novikov,
D., ÒMorphological Optimization of LiFePO4 for High Rate Applications,Ó
Abstract No. 133, 208th Meeting of the Electrochemical Society, Los
Angeles, CA, October 16-21.
Whittingham, M.S. (2004). ÒLithium
Batteries and Cathode Materials.Ó Chem. Rev., 2004, 104:4271-4301.
I. Willner and E. Katz, "Integration
of layered redox proteins and conductive supports for bioelectronic
applications," Angew Chem. Int. Ed.,
vol. 39, pp. 1180-1218, 2000.
I. Willner, ÒBiomaterials for sensors, fuel
cells, and circuitry,Ó Science, vol.
298, p. 2407, 2002.
Winter, M., Brodd, R. (2004). ÒWhat Are
Batteries, Fuel Cells, and Supercapacitors?Ó Chem. Rev., 2004, 104:4245-4269.
Xu, J.J., Jain, G., Balasubramanian, M.,
and Yang, J. (2005), ÒQualitatively Different Behavior of Electrode Materials
at the Nanoscale- Implications for 3D Battery Nanoarchitectures,Ó Abstract No.
1243, 208th Meeting of the Electrochemical Society, Los Angeles, CA,
October 16-21.