Lithium transition metal oxides as rechargeable battery cathode materials
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Lithium Transition Metal Oxides as Battery Cathode
"Although the basics of electricity were established in 600 B.C. By the Greek philosopher
Thales of Miletus and then refined by scientist William Gilbert of England in 1600,
the first battery actually dates back to the 18th century"
(Millard, N.d., p.2).
Modern Miniaturization
Contrary to the contemporary trend to supersize fast food portions, which Jennifer O. Fisher and Tanja V.E. Kral (2007) note in the article, "Super-size me...," manufacturers routinely reduce the size of electronic components. As this practice of downsizing electronic components contributed to improvements in integrated circuit technology and fabrication processes, it simultaneously led to electronic devices and related peripherals becoming miniaturized. According to Burtrand Insung Lee and Sridhar Komarneni (2005) in the book, Chemical Processing of Ceramics, "the consumer market has readily embraced the miniaturization of products and manufacturers have continuously come up with new products and marketing concepts. All… ubiquitous miniaturized devices… need…efficient, lightweight, and rechargeable power sources" (p. 668). The bulk lithium-ion battery depicts one power source that matches each of these particular requirements that the contemporary consumer craves.
The lithium-ion battery, initially introduced as replacement for the heavier, older nickel-metal hydride (NiMH) battery, provided superior energy density and weighed less than the NiMH. As the lithium-ion battery technology has spread through the consumer electronic field, one finds the lithium-ion battery ubiquitous. A traditional lithium battery contains a lithium anode, a cathode made of a transition metal oxide and an organic electrolyte that contains lithium ions. Transition metal oxides, electrode materials, prove useful in various types of batteries, including rechargeable and lithium. In the journal article, "Vanadium-doped manganese oxides as cathode materials for rechargeable lithium batteries," Charles J. Capozzi and Jun John Xu (2002), both with the Department of Ceramic and Materials Engineering, Rutgers University, explain that in the past, researchers believed "the reaction of lithium metal and a transition metal oxide yielded lithium oxide due to reduction of the transition metal oxide. However, emf values were not consistent with thermodynamically expected values" (Introduction section, ¶ 1). Some studies, according to Capozzi and Xu report, conclude that lithium intercalated into the transition metal oxide structure by expanding the volume of the transition metal oxide structure. Through the examination of related literature, the researcher relates a number of advantages, disadvantages, future prospects, fabrication methods and challenges for lithium transition metal oxide, one type ceramic, as a battery cathode and simultaneously introduces the lithium transition metal oxides as the battery cathode.
Time Refines Batteries
Count Alessandro Volta of Italy developed the first battery, according to the article, "Battery power," (2008). In a paper Volta submitted to the Royal Society in 1799, he described his battery, which "comprised alternating discs of zinc and copper with pieces of cardboard soaked in brine between the metals" ("Battery power," ¶ 2). In time, this battery became known as Volta's pile. A number of individuals introduced and manufactured additional various cell chemistries. During 1836, John Frederic Daniell, a British chemist, invented the Daniell cell (Ibid.). In the article "Gassner, Carl," Cutler J. Cleveland and Tom Lawrence (2008) report that Carl Gassner, a German scientist, invented the first commercially successful dry cell battery in1881. Gassner's battery became the contemporary, general-purpose, carbon-zinc battery. Gassner added zinc chloride to the electrolyte. This significantly increased the cell's useful life and reduced the corrosion of zinc when the cell idled. In1899, Waldmar Jungner, a Swede, developed the first nickel-cadmium (NiCd) battery (Ibid.). Figure 1 depicts the chemistry of the Daniell cell.
Figure 1: The Daniell Cell's Chemistry (Battery Power, 2010, Further Reading Section).
When the circuit is complete, electrons flow from the zinc to the copper, owing to the electrical potential. Conventional current flows from the positive (anode) to the negative (cathode): this is the opposite to the direction of electron flow.
The porous separator prevents bulk mixing of the electrolytes but allows aqueous ions to pass through to maintain the ionic balance.
Anode: Zn(s) Zn2+(aq) + 2e-
Cathode: Cu2+(aq) + 2e- Cu(s)
For a copper-zinc cell under standard conditions (25°C, 1 mol dm-3, 1 atmosphere) the cell voltage may be calculated from the oxidation and reduction half reactions.
Zn(s) 1/2 Zn2+ | Cu2+(aq) 1/2 Cu(s)
E Zn2++ 2e- Zn E = -0.76V
E Cu2+ + 2e- Cu E = +0.34V
E for the cell = +0.34 - (-0.76) = 1.10V. (Battery Power, 2010, Further Reading Section)
Batteries consist of three separate parts, an anode (-) which comprises that negative side, a cathode (+) positive side, and the electrolyte. In a traditional battery, the cathode and anode connect to an electrical circuit. The Northwestern State University article, "How do batteries work?"(2010), explains that "the chemical reactions in the battery causes a buildup of electrons at the anode. This results in an electrical difference between the anode and the cathode. & #8230;[One may] think of this difference as an unstable build-up of the electrons" (¶ 3). As a result the electrons rearrange themselves by repelling each other and finding a place with fewer electrons.
In batteries, these electrons can only travel to the cathode, as the electrolyte stops the electrons from reaching the anode and end up at the cathode. "When the circuit closes (a wire connects the cathode and the anode) the electrons will be able to get to the cathode. In the picture above, the electrons go through the wire, lighting the light bulb along the way" (How do batteries…, 2010, ¶ 4). Electrochemical processes changes the chemicals in the cathode and anode to ensure they do not supply electrons, this explains why there is limited power available from batteries. When recharging a battery, the flow of electrons is reversed by using a different power source, perhaps solar panels, allowing the anode and cathode to be restored to their full power. Figure 2 depicts this process.
Figure 2: Depicts Currency of a Battery (How do batteries…, 2010).
A myriad of items, including, but not limited to, cars; cell phones; computers; microchips; etc. may use energy batteries provide. M. Armand and J.-M. Tarascon (2008), with the Universite de Picardie Jules Verne, Amiens, France, assert in the journal article, "Building better batteries," that variations of the combustion reaction fueled the past few centuries' technological revolution. During the majority of the 20th century, several generations of disposable dry cell batteries as well as Jungner's rechargeable nickel-cadmium served as the primary power sources for portable electric and electronic equipment. A number of inherent problems challenged the dry cell batteries and the nickel cadmium batteries as they not only contained lead, mercury and cadmium, they proved to have high toxicity when individuals disposed them. The nickel-cadmium batteries also became known for "memory effect." When one charged one of these batteries prior to it being completely expended, the battery would only hold the charge from the point the individual charged it. In regard to the lithium ion battery,
Metallic lithium, which is used in lithium primary cells, is unsuitable for rechargeable cells owing to dendritic crystal growth of the metal in the recharge phase which can damage the cell. Instead lithiated graphite is used as the anode.
Anode: Lithiated graphite (LiC6)
Cathode: LiCoO2
Electrolyte: LiPF6 in aprotic solvent
Overall reaction: Li 1-x CoO2 + CLix LiCoO2 + CE = 3.7V
Lithium atoms in the lithiated graphite are intercalated between the hexagonal layer molecular structure of the graphite and are free to move around. On discharge these atoms migrate from the graphite to the lithium cobalt oxide. This technology was developed by the British company AEA Technology and commercialised by Sony under licence from AEA. Currently Quallion in the U.S. uses this technology in microbatteries (the size of a grain of rice) in medical implants for neurological disorders. The batteries have a 10-year life. (Battery Power, 2010, Secondary Cells Section, ¶ 12).
In 1980, Mizushima et al. initially examined LiCoO2. At that time, a number of researchers projected LiCoO2 to comprise a potential positive electrode for lithium-ion rechargeable batteries. Sony Corporation commercialized the first lithium-ion battery in 1991. Sony used lithium cobalt oxide for the positive electrode and graphite (carbon) for the negative electrode. Since 1991, manufactures have generally used LiCoO2 as the primary cathode in commercial lithium-ion batteries. LiCoO2 continues to claim a significant stance as a cathode material. Lithium oxide used as a flux in ceramic glaze, also serves as a replacement for lithium cobalt oxide as the cathode in the lithium ion batteries used ... lithium (element, metal -- in chemistry Merriam Webster Dictionary defines "flux' (2010) as a substance used to promote fusion (as of metals or minerals); especially: one (as rosin) applied to surfaces to be joined by soldering, brazing, or welding to clean and free them from oxide and promote their union" (p. 1).
Lee and Komarneni (2005) assert that currently, manufacturers use three intercalation materials as positive electrode materials to produce commercial lithium-ion rechargeable batteries: LiCoO2, LiNiO2, and LiMn2O4. Armand and Tarascon (2008) explain:
The lithium-ion battery, first commercialized by Sony in 1991, owes its name to the exchange of the Li+ ion between the graphite (LixC6) anode and a layered-oxide (Li1?xTMO2) Cathode2, with TM being a transition metal (usually cobalt but sometimes nickel or manganese). The energy it stores (?180 Wh kg?1) at an average voltage of 3.8 V is only a factor of 5 higher than that stored by the much older lead -- acid batteries. This may seem poor in the light of Moore's law in electronics (according to which memory capacity doubles every 18 months), but it still took a revolution in materials science to achieve it. Billions of lithium-ion cells are produced for portable electronics, but this is not sustainable as cobalt must be obtained from natural resources (it makes up 20 parts per million of Earth's crust). (Armand & Tarascon, 2008, p. 653).
Fu investigated the lithium-ion conductivities of glasses and glass-ceramics in the LI2O-AlO3-TiO2P2O5 system. Fu's samples revealed high conductivity, albeit when Abrahams and Hadzifejzovic similarly investigated the LI2O-AlO3-TiO2P2O5 glass and glass-ceramic systems, their findings revealed "a maximum room temperature conductivity of 3.98 x 10-6 S/cm in their crystallized cast-gas pellet sample. When Fu later investigated the incorporation of a number of other M2O3 type constituents where M = Y, Dy, Gd, and LA to extend the research, Fu found that the parent glass' ionic conductivity basically remained consistent with increasing ionic radium of M3+. The ionic conductivities of the glass-ceramics, albeit, significantly decreased while the ionic radius of the M3+. atom increased (Lee & Komarneni, 2005).
Table one depicts characteristics of the primary processes planned for ceramic membranes use.
Table 1: Ceramic Membranes Main Characteristics Processes (Lee & Komarneni, 2005 p. 631).
Process
Nature of Feed/Strip
Pore size
Origin of selectivity
Pressure Gradient
Elemental Operation
Microfiltration
0.1-10µm
Sieving effect
1-3 bars
Clarification, debacterization, separation
Ultrafiltration
Liquid/liquid
1 nm-0.1 µm
Sieving effect
3-10 bars
Clarification, purification, concentration
Nanofiltration
Sieving + specific interactions with the membrane
10-40bars
Purification, water softening, separation, concentration
Pervaporation
Liquid/gas
Sieving + additional specific interaction
1 bar
Separation
Gas filtration Gas separation
Gas/gas
100 µm
50 nm-
Sieving effect
Sieving + additional specific interaction
0.1-5 bars 0.1-50 bars
Separation, dusting
Separation, extraction, Purification
Gas separation
Dense
Ionic conduction of O2- by oxides p (O2)
Air separation, transport of O2
Figure 3 portrays typical representative cathode crystal structures: (a): rhombohedra R3m; (b) monoclinic C2/m; (c) spinel Fd3m; (d) orthorhombic Pmmm. Figure 2 also relates ceramic materials for lithium-ion battery applications.
Figure 3: Typical Representative Cathode Crystal Structures (Lee & Komarneni, 2005, p. 669).
Lithium Oxide, Li2O, a highly undissolvable thermally stable Lithium source, is best suited for ceramic, glass and optic applications. The article, "Lithium Oxide," (2010) published by American Elements, a prominent manufacturer of engineered and advanced material products, explains that "Oxide compounds are not conductive to electricity. However, certain perovskite structured oxides are electronically conductive finding application in the cathode of solid oxide fuel cells and oxygen generation systems" (¶ 1). These particular compounds contain one oxygen anion and one metallic cation.
Lithium transition metal oxides, compounds with phenomenal intercalation, exhibit a variety of captivating electronic and phase phenomena. Gholamabbas Nazri and Gianfranco Pistoia (2004) assert in the book, Lithium batteries: Science and technology, that lithium possesses the ability to "undergo large variation in lithium concentration, often without suffering irreversible changes" (p. 42). This makes lithium transition metal oxides, which consist of metal oxide host "with a crystal structure in which lithium ions occupy a relatively open network of interstitial sites" (Ibid.) ideal electrodes for rechargeable lithium batteries. Lithium transition metal oxides prove to be somewhat instrumental as an anode in rechargeable lithium batteries, however, they are more suited as a cathode because they display high voltage. "In a rechargeable lithium battery, lithium ions are shuttled between an anode and a cathode, whereby lithium ions are removed from and inserted into the electrodes" (Nazri & Pistoia, 2004, p. 42). In the deintercalation of a lithium metal oxide, open spaces are made on the lithium portions of the host, during intercalation, lithium refills these portions.
Inserting and removing lithium ions may cause a remarkable phenomena that could increasingly affect the electrochemical properties of a compound. Differences in the concentration of lithium can change the electronic properties of the transition metal oxide host. "The valence electron of each lithium ion is generally donated to the host where it can either the valence state of the transition metal ion and/or alter the nature of the bonds between the transition metal and the oxygen ions" (Nazri & Pistoia, 2004, p. 43). At the same time, removing lithium from the host may cause the structure of the metal oxide to become unstable or stimulate the order-disorder phase transitions between lithium and vacancies following the attainment of a critical vacancy concentration. At times, these phenomena may significantly affect the voltage characteristic or the lattice parameters of the compound.
Typically, lithium transition metal oxides are not water soluble. They are, however, extremely stable which makes them particularly complementary to ceramic structures. "Metal oxide compounds are basic anhydrides and can therefore react with acids and with strong reducing agents in redox reactions. Lithium Oxide is also available in pellets, pieces, sputtering targets, tablets and nanopowder" (Lithium Oxide, 2010, ¶ 1). Lithium, part of the alkali group of metals, has the maximum specific heat of any other material and the highest electrochemical potential.
In ceramic processing, the first step involves preparing the ceramic powder, while the second step comprises molding (forming). In the publication, "Ceramic materials - forming methods and properties of final element, "Magdalena Gizowska (N.d.) purports that a myriad of methods for forming ceramics exists; albeit they primarily depend on the product's ultimate desired shape. Most widespread methods for forming dense ceramics may be characterized into a number of groups. Well-known are also methods of designing porous ceramic materials.
The third step in ceramic processing sintering, depicts a process that heating causes, material consolidation. "The temperature of sintering is between 2/3-4/5 of melting point of the predominant component in the ceramic material. The visible sign of sintering is the shrinkage of the material (Ibid.). Figure 4 portrays the significant structural changes that occur during fabrication of ceramic products in ceramic processing.
Figure 4: Ceramic Processing Structural Changes (Lee & Komarneni, 2005, p. 669).
Lithium Transition Metal Oxides Disadvantages
Air electrodes and metal -- air battery technologies have already been used in primary systems such as fuel cells, but the use of lithium instead of zinc as the metal will increase the energy output eightfold. An oxygen electrode proceeding in tandem with lithium according to the reaction 2Li + O2 ? Li2O2 can deliver a capacity of 1,200 mAh g?1. The first lithium -- air cell was successfully assembled and discharged in 1996, but attractive rechargeability was demonstrated only recently. It could be argued that such a system unites within the same device the two most prominent failures of battery and fuel-cell technologies, namely the inability to master lithium and oxygen electrodes. These perceived issues have prevented the practical use of lithium -- air batteries (Armand & Tarascon, 2008, p. 654).
Ying Wang and Guozhong Cao (2008), both with the Department of Materials Science and Engineering, University of Washington, assert in the journal article, "Developments in nanostructured cathode materials for high performance lithium-ion batteries," at present, lithium-ion batteries are efficient, light-weight, and rechargeable power sources for consumer electronics such as laptop computers, digital cameras, and cellular phones. Moreover, they have been intensively studied for use as power supplies of electric vehicles (EVs) and hybrid electric vehicles (HEVs), which require high energy and power densities Lithium-ion batteries are attractive power-storage devices owning to their high energy density; however, their power density is relatively low because of a large polarization at high charge -- discharge rates. This polarization is caused by slow lithium diffusion in the active material and increases in the resistance of the electrolyte when the charging -- discharging rate is increased. To overcome these problems, it is important to design and fabricate nanostructured electrode materials that provide high surface area and short diffusion paths for ionic transport and electronic conduction (p. 2252).
Nanomaterials offer unusual mechanical, electrical, and optical properties endowed by confining the dimensions of such materials, and the overall behaviors of nanomaterials exhibit combinations of bulk and surface properties. Thus, nanostructured materials are drawing a tremendous amount of attention because of their novel properties, and because of their potential applications in a variety of nanodevices, such as field-effect transistors (FETs), chemical and biological sensors, nanoprobes, and nanocables. Reports on the processing, properties, and applications of nanomaterials are appear rapidly, on a daily basis. Many synthesis methods have been reported for the synthesis of nanostructured electrode materials. Among them, solution-based methods are well-known for their advantages in tailoring the size and morphology of the nanostructures. It is the uncomplicated sol -- gel processing (soft chemistry) method in combination with template synthesis or hydrothermal treatment that produces the most desirable nanostructures with remarkable reliability, efficiency, selectivity, and variety (Wang & Cao, 2008, p. 2252).
It should be noted that the nanoparticulate forms of lithium transition metal oxides such as LiCoO2, LiNiO2, or their solid solutions can react with the electrolyte and lead to safety problems. In the case of LiMn2O4, the use of nanoparticles causes undesirable dissolution of Mn. Significant efforts have been made to increase the stability of these nanocrystalline lithium metal oxides. Better stability can be achieved by coating the electrode materials with a nanosized stabilizing surface layer that alleviates these problems. As for LiCoO2, coatings of various phosphates and oxides have been studied and significant improvements in capacity retention have been demonstrated. Kim et al. made an extensive study on the effect of the MPO4 (M1/4Al, Fe, SrH, and Ce) nanoparticle coatings on LiCoO2 cathode materials. They found that the extent of the coating coverage is affected by the nanoparticle size and morphology despite the same coating concentration and annealing temperature (Wang & Cao, 2008, p. 2260).
Lei Wang, Thomas Maxisch, and Gerbrand Ceder (2006), all with the Department of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts, assert in the journal article, "Oxidation energies of transition metal oxides within the GGA+U framework," Oxidation and reduction reactions play a key role in many technological and environmental processes, such as corrosion, combustion, metal refining, electrochemical energy generation and storage, photosynthesis, and metabolism. The ability to correctly predict the reaction energy and electrochemical potentials of such reactions with first-principles methods is therefore important. Although the local density approximation _LDA_ and generalized gradient approximation _GGA_, two standard approximations to density functional theory _DFT_, are rather crude approximations to the many-body electron problems, their successes in accurately predicting materials properties are in large part due to the cancellation of errors in energy differences (p. 1).
The energy of a large number of oxidation reactions of 3d transition metal oxides is computed using the generalized gradient approach _GGA_ and GGA+U methods. Two substantial contributions to the error in GGA oxidation energies are identified. The first contribution originates from the overbinding of GGA in the O2 molecule and only occurs when the oxidant is O2. The second error occurs in all oxidation reactions and is related to the correlation error in 3d orbitals in GGA. Strong self-interaction in GGA systematically penalizes a reduced state _with more d electrons_ over an oxidized state, resulting in an overestimation of oxidation energies (Wang, Maxisch & Ceder, 2006, p. 1).
The constant error in the oxidation energy from the O2 binding error can be corrected by fitting the formation enthalpy of simple nontransition metal oxides. Removal of the O2 binding error makes it possible to address the correlation effects in 3d transition metal oxides with the GGA+U method. Calculated oxidation energies agree well with experimental data for reasonable and consistent values of U (Wang, Maxisch & Ceder, 2006, p. 1).
Future Prospects of Lithium transition metal oxides
M. Stanley Whittingham, Oxford University, United Kingdom, Yanning Song, Shanghai Jiaotong University, Shanghai, China, Samuel Lutta, State University of New York at Binghamton, Peter Zavalij, L'viv National University, Ukraine and Natasha A. Chernova (2005), M.V. Lomonosov Moscow State University, assert in the journal article, "Some transition metal (oxy)phosphates and vanadium oxides for lithium batteries," iron and vanadium oxides have a rich structural chemistry when combined with phosphate groups; the transition metal most commonly in an octahedral coordination. The inductive effect increases the potential difference between Fe3+/Fe2+ and Li/Li + couples in phosphate lattices relative to the pure iron oxides; a similar behavior is found for the corresponding vanadium compounds. Of the iron phosphates, the olivine phase LiFePO4 has high thermal and chemical stability, even when lithium-free; the challenges of low electronic conductivity are being overcome, but data is lacking on the true lithium diffusion behavior. The all-ferric lipscombite-type phase, Fe1.33PO4OH, shows the highest capacity of the iron phosphates for lithium intercalation (p. 3362).
The e-VOPO4 material, formed by the oxidative de-intercalation of protons from H2VOPO4, can reversibly react with two lithium atoms in two steps. The face- and edge-sharing transition metal octahedra lead to a range of interesting and structurally revealing magnetic interactions. A number of vanadium oxide phases are known, with those containing VO6 octahedra showing the greatest stability when undergoing redox reactions. Such structures have been synthesized using xerogel, hydrothermal and electrochemical methods. The double-sheet delta structures show reversible lithium intercalation of up to one lithium ion per vanadium, leading to the highest storage capacities. However, the large potential width of discharge and the apparent low reaction rates will minimize their use unless improved (Whittingham, Song, Lutta, Zavalij & Chernova, 2005, p. 3362).
It is difficult to measure the diffusion coefficient by standard cathode methods because there is no compositional variation so what is measured is the movement of the LiFePO 4/FePO4 interface. One experimental study suggests a diffusion coefficient of 2-6 10214 cm2 s21 for LiFePO4,23 and another 24 on LiCoPO4 found values varying from 10211 to 10212 cm2 s21 depending on the electrolyte suggesting that these are "system" diffusion coefficients rather than the true bulk value for the phosphate. Franger et al. have reported 15 a value of around 10213 -- 10214 cm2 sec21 over the whole range of composition for LiFePO4. These values are consistent with conductivity values of less than 1029 S. cm21 for pure compounds. A measurement of the intrinsic ionic conductivity would be desirable, probably using the methods appropriate for a solid electrolyte (Whittingham, Song, Lutta, Zavalij & Chernova, 2005, p. 3366).
Binod Kumara (2010), Metals and Ceramics Division, University of Dayton Research Institute, et al., assert in the journal article, "A solid-state, rechargeable, long cycle life lithium -- air battery," the lithium ion battery business has grown into a multibillion dollar global industry, and a robust growth is anticipated in the future. The state-of-the-art lithium ion batteries employ many variations in cell components and chemistries. Most of them use a graphitic carbon anode _negative electrode_, a liquid electrolyte comprised of lithium salts dissolved in organic solvents, a microporous polymer separator, and a lithiumintercalated transition-metal oxide cathode _positive electrode_. The small lithium ion cells and battery packs made from them have gained worldwide consumer acceptance. Larger lithium ion batteries for hybrid and electric vehicles are yet to be developed, tested, and accepted. A few safety incidents and recalls of lithium ion cells produced by major manufacturers have also drawn significant attention (p. 157).
A high temperature environment can lead to the rupture, ignition, and even explosion of liquid electrolyte-based lithium batteries. For example, a lithium ion cell exposed to prolonged sunlight may rupture. A short-circuit in a lithium ion battery can cause it to ignite and explode. Some Li-ion cells are built with safety devices, which can prevent these hazards; however, separator defects and contaminants inside the cell can defeat those safety devices. The underlying causes for the safety concerns are the reactions involving liquid electrolytes, polymer separators, and transition-metal oxide cathodes. The societal needs in the present energy scenario require the development of inexpensive, thermally stable, and safe lithium batteries with high energy and power densities (Kumara, et al., 2010, p. 157).
About 12 years ago, Abraham et al. demonstrated the first practical nonaqueous rechargeable Li -- O2 battery cell. Their cell design employed a Li-ion conducting gel polymer electrolyte _membrane_ derived from either a poly_acrylonitrile_ or a poly_vinylidine difluoride _ polymer. The cell exhibited good capacity utilization vs. discharge rates, but its rechargeability was limited, attributed in part to the limited cycle life of the Li anode. Following this early investigation, several studies have been reported to improve the performance of the Li -- O2 battery. Abraham et al. suggested the use of gel electrolytes with nonvolatile liquid plasticizers to increase battery life (Kumara, et al., 2010, p. 157).
Dobley et al. studied the use of catalysts to enhance the rate capability and the capacity utilization of the oxygen electrode. Kuboki et al. investigated ionic liquids in Li -- O2 cells to increase the overall stability and performance of the battery. Beattie et al. investigated high capacity composite carbon cathodes to increase energy density. Ogasawara et al. demonstrated the rechargeability of Li -- O2 cells starting with Li2O2 in the cathode with or without catalysts. Visco et al. reported the electrochemical performance of a working Li -- O2 cell and suggested that practical Li -- O2 cells may lead to an energy density of 1000 Wh/kg or 1000 Wh/L. Despite these recent efforts, a rechargeable Li -- O2 cell with high energy efficiency and long life, in which charge and discharge proceed with low polarizations, has remained elusive. In this context, the attributes including excellent rechargeability of the Li -- O2 cell reported in this paper are believed to be a major contribution as they overcome the previously identified deficiencies (Kumara, et al., 2010, p. 157).
The primary component of the electrolyte and the cathode is a glass -- ceramic _GC_ material, which is very stable when in contact with water. A chemical degradation of either of the two components by the presence of water leading to cell failure is not anticipated. The polymer -- ceramic _PC_ membranes were prepared from dried poly_ethylene oxide_ _PEO_, LiN_SO2CF2C 3_2 _LiBETI_ salt, Li2O, and boron nitride _BN_. In a typical preparation, a dried mixture of the electrolyte components was energy milled and hot-pressed to obtain 200 -- 400 _m thick membranes (Kumara, et al., 2010, p. 157).
The GC membrane was prepared from a batch of various oxides corresponding to the 18.5Li2O:6.07Al2O3:37.05GeO2:37.05P2O5 _LAGP_ molar composition. The batch was melted at 1350°C in a platinum crucible, cast into solid glass sheets, powdered and pressed into a membrane, and sintered at about 850°C. The sintering parameters _temperature and time_ were optimized to achieve the highest membrane conductivity. The conductivities of both the GC and PC membranes were extensively characterized, and the data have been reported in prior publications. The cathode was prepared using nickel mesh or foam, carbon black _acetylene 50% compressed_, Teflon _TE-3859_, and GC powder. Nickel foam was used with an intent to achieve further enhancement in cell capacity. Carbon black _25 and 50 wt%_, LAGP _50 and 75 wt %_ powders, and Teflon were mixed with deionized water to obtain a soft mass, which was spread on both sides of the nickel mesh or foam and sandwiched between two stainless steel plates. The LAGP material used in the cathode is similar in chemistry and crystal structure to the LAGP material used in the membrane laminate. The assembled sandwich was pressed, dried at 100°C overnight, and sintered at 240°C for 20 min in an argon atmosphere (Kumara, et al., 2010, p. 157).
The setup of the cells consists of metallic lithium as the anode, three membrane laminates _two PC layers and one LAGP layer_, and a cathode. The cell area in all cases was 2.00 cm2. The cells were assembled in a dry box _O2 _ 80 ppm, H2O _ 89 ppm_ contained in the casing with a spacer and an O-ring. The cathode side of the casing was perforated to allow the flow of oxygen to the cathode. The cell components along the casing were pressed to seal using a Hohsen cell maker _Hohsen Corporation, 10-4-601, Minamisenba, 4-Chome, Chuo-ku, Osaka, Japan_ into a working cell (Kumara, et al., 2010, p. 157).
In this paper, the fabrication, characterization, and performance of solid-state, rechargeable, and long cycle life Li -- O2 cells are presented and discussed. The cells consisted of a lithium metal anode, a membrane laminate fabricated from GC and PC materials, and a solid-state composite oxygen/air cathode prepared from carbon and GC powder. The cells demonstrated excellent thermal stability and rechargeability in the 30 -- 105°C temperature range. A cell was subjected to 40 discharge/charge cycles in the 30 -- 105°C temperature range. The cells exhibited excellent reversibility. The cathode formulations and processing, charge and discharge rates, and thickness of cell components were varied. These cells have produced extremely reproducible results, and the effort to improve their electrochemical performance continues. The results have led us to believe that the fabrication of a totally solid-state, safe, rechargeable, and commercially viable lithium -- air battery with high energy and power densities is well within the reach (Kumara, et al., 2010, p. 158).
Conclusions
It is not yet clear whether the next generation of batteries could be successfully integrated into an energy market that is currently linked to global warming. Fame and fortune certainly await anyone who can come up with a viable alternative to fossil fuels. Furthermore, it is difficult to see how the performance gap between the internal-combustion engine and lithiumion batteries will be filled using only new battery technology; other approaches, such as fuel cells, will be needed, but here a complete overhaul of present systems will probably be required (Armand & Tarascon, 2008, p. 657).
The next generation of lithium-ion batteries fully based on nanomaterials will soon be here, followed by lithium -- air batteries and others using organic materials. And there is plenty to inspire us in the living world, as long as we can capture the function of each molecule in a cumulative sequential process, which is not an easy task. Both biofuel cells and high-voltage liquid-electrolyte microbatteries inspired by electric eels have already been demonstrated. One thing is clear, however. Solving the remaining challenges will require researchers from a range of disciplines, and their success will depend on the efficiency of their crossfertilization (Armand & Tarascon, 2008, p. 657).
Lee and Komarneni (2005) purport that as some researchers expect that the forthcoming frontier in ceramics will probably need molecular level or nanoscale control, the role of ceramics in the age of biology depicts an area of interest. With society transitioning from an energy-rich society to an energy-declining society, the question arises: How "can ceramic materials appease the problem? (Lee & Komarneni, Overview Section, ¶ 1). From the literature the researcher examined for the paper, the researcher contends that both the contemporary trend to supersize fast food portions and lithium transition metal oxides as battery cathode will likely one day comprise historical accounts for researchers to explore. Meantime, just as Gilbert refined concepts relating to the basics of electricity that Thales of Miletus established in 600 B.C., contemporary researchers will continue to refine knowledge regarding lithium transition metal oxides as battery cathode.
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