Lithium–air battery


The lithium–air battery is a metal–air electrochemical cell or battery chemistry that uses oxidation of lithium at the anode and reduction of oxygen at the cathode to induce a current flow.
Pairing lithium and ambient oxygen can theoretically lead to electrochemical cells with the highest possible specific energy. Indeed, the theoretical specific energy of a non-aqueous Li–air battery, in the charged state with Li2O2 product and excluding the oxygen mass, is ~40.1 MJ/kg. This is comparable to the theoretical specific energy of gasoline, ~46.8 MJ/kg. In practice, Li–air batteries with a specific energy of ~6.12 MJ/kg at the cell level have been demonstrated. This is about 5 times greater than that of a commercial lithium-ion battery, and is sufficient to run a 2,000 kg EV for ~ on one charge using 60 kg of batteries. However, the practical power and life-cycle of Li–air batteries need significant improvements before they can find a market niche.
Significant electrolyte advances are needed to develop a commercial implementation. Four approaches are active: aprotic, aqueous, solid state and mixed aqueous–aprotic.
Metal–air batteries, specifically zinc–air, have received attention due to potentially high energy densities. The theoretical specific energy densities for metal–air batteries are higher than for ion-based methods. Lithium–air batteries can theoretically achieve 3840 mA·h/g.
A major market driver for batteries is the automotive sector. The energy density of gasoline is approximately 13 kW·h/kg, which corresponds to 1.7 kW·h/kg of energy provided to the wheels after losses. Theoretically, lithium–air can achieve 12 kW·h/kg excluding the oxygen mass. Accounting for the weight of the full battery pack, while lithium alone is very light, the energy density is considerably lower.
A Li–air battery potentially had 5–15 times the specific energy of a Li-ion battery as of 2016.

History

Originally proposed in the 1970s as a possible power source for battery electric vehicles, and hybrid electric vehicles, Li–air batteries recaptured scientific interest late in the first decade of the 2000s due to advances in materials science.
Although the idea of a lithium–air battery was around long before 1996, the risk-to-benefit ratio was perceived as too high to pursue. Indeed, both the negative and the positive electrodes are the reasons why, respectively, rechargeable lithium-metal batteries failed to reach the market in the 1970s. Nevertheless, due to a perceived lack of other alternatives to high specific energy rechargeable batteries, and due to some initially promising results from academic labs, both the number of patents and of free-domain publications related to lithium–oxygen batteries began growing exponentially in 2006. However, the technical difficulties facing such batteries, especially recharging times, nitrogen and water sensitivity, and the intrinsic poor conductivity of the charged Li2O2 species are major challenges.

Design and operation

In general lithium ions move between the anode and the cathode across the electrolyte. Under discharge, electrons follow the external circuit to do electric work and the lithium ions migrate to the cathode. During charge the lithium metal plates onto the anode, freeing at the cathode. Both non-aqueous and aqueous Li-O2 batteries have been considered. The aqueous battery requires a protective layer on the negative electrode to keep the Li metal from reacting with water.

Anode

Lithium metal is the typical anode choice. At the anode, electrochemical potential forces the lithium metal to release electrons via oxidation. The half-reaction is:
Lithium has high specific capacity compared with other metal–air battery materials. Several issues affect such cells.
The main challenge in anode development is preventing the anode from reacting with the electrolyte. Alternatives include new electrolyte materials or redesigning the interface between electrolyte and anode. Lithium anodes risk dendritic lithium deposits, decreasing energy capacity or triggering a short circuit.
The effects of pore size and pore size distribution remain poorly understood.
Upon charging/discharging in aprotic cells, layers of lithium salts precipitate onto the anode, eventually covering it and creating a barrier between the lithium and electrolyte. This barrier initially prevents corrosion, but eventually inhibits the reaction kinetics between the anode and the electrolyte. This chemical change of the solid–electrolyte interface results in varying chemical composition across the surface, causing the current to vary accordingly. The uneven current distribution furthers branching dendrite growth and typically leads to a short circuit between the anode and cathode.
In aqueous cells problems at the SEI stem from the high reactivity of lithium metal with water.
Several approaches attempt to overcome these problems:
At the cathode during charge, oxygen donates electrons to the lithium via reduction. Mesoporous carbon has been used as a cathode substrate with metal catalysts that enhance reduction kinetics and increase the cathode's specific capacity. Manganese, cobalt, ruthenium, platinum, silver, or a mixture of cobalt and manganese are potential metal catalysts. Under some circumstances manganese-catalyzed cathodes performed best, with a specific capacity of 3137 mA·H/g carbon and cobalt-catalyzed cathodes performed second best, with a specific capacity of 2414 mA·H/g carbon. Based on the first pore-scale modeling of lithium–air batteries, the micro-structure of the cathode significantly affects battery capacity in both non-pore-blocking and pore-blocking regimes.
Most Li–air battery limits are at the cathode, which is also the source of its potential advantages.
Atmospheric oxygen must be present at the cathode, but contaminants such as water vapor can damage it.
Incomplete discharge due to blockage of the porous carbon cathode with discharge products such as lithium peroxide is the most serious.
Catalysts have shown promise in creating preferential nucleation of over, which is irreversible with respect to lithium.
Li–air performance is limited by the efficiency of the reaction at the cathode, because most of the voltage drop occurs there. Multiple chemistries have been assessed, distinguished by their electrolyte. This discussion focuses on aprotic and aqueous electrolytes as solid-state electrochemistry is poorly understood.
In a cell with an [|aprotic electrolyte] lithium oxides are produced through reduction at the cathode:
where "*" denotes a surface site on where growth proceeds, which is essentially a neutral Li vacancy in the surface.
Lithium oxides are insoluble in aprotic electrolytes, which leads to cathode clogging.
A nanowire array cathode augmented by a genetically modified M13 bacteriophage virus offers two to three times the energy density of 2015-era lithium-ion batteries. The virus increased the size of the nanowire array, which is about 80 nm across. The resulting wires had a spiked surface. Spikes create more surface area to host reaction sites. The viral process creates a cross-linked 3D structure, rather than isolated wires, stabilizing the electrode. The viral process is water-based and takes place at room temperature.

Electrolyte

Efforts in Li–air batteries have focused on four electrolytes: aqueous acidic, aqueous alkaline, non-aqueous protic, and aprotic.
In a cell with an [|aqueous electrolyte] the reduction at the cathode can also produce lithium hydroxide:

Aqueous

An aqueous Li–air battery consists of a lithium metal anode, an aqueous electrolyte and a porous carbon cathode. The aqueous electrolyte combines lithium salts dissolved in water. It avoids the issue of cathode clogging because the reaction products are water-soluble. The aqueous design has a higher practical discharge potential than its aprotic counterpart. However, lithium metal reacts violently with water and thus the aqueous design requires a solid electrolyte interface between the lithium and electrolyte. Commonly, a lithium-conducting ceramic or glass is used, but conductivity are generally low.

Acidic electrolyte

A conjugate base is involved in the reaction. The theoretical maximal Li–air cell specific energy and energy density are 1400 W·h/kg and 1680 W·h/l, respectively.

Alkaline aqueous electrolyte

Water molecules are involved in the redox reactions at the air cathode. The theoretical maximal Li–air cell specific energy and energy density are 1300 W·h/kg and 1520 W·h/l, respectively.
New cathode materials must account for the accommodation of substantial amounts of, and/or LiOH without causing the cathode pores to block and employ suitable catalysts to make the electrochemical reactions energetically practical.
Non-aqueous Li–air batteries were demonstrated first. They usually use mixed ethylene carbonate+ propylene carbonate solvents with LiPF6 or Li bis-sulfonimide salts like conventional Li-ion batteries, however, with a gelled rather than liquid electrolyte. The voltage difference upon constant current charge and discharge is usually between 1.3 and 1.8 V even at such ridiculously low currents as 0.01–0.5 mA/cm² and 50–500 mA/g of C on the positive electrode, However, the carbonate solvents evaporate and get oxidized due to a high overvoltage upon charge. Other solvents, such as end-capped glymes, DMSO, dimethylacetamide, and ionic liquids, have been considered. The carbon cathode gets oxidized above +3.5 V v Li during charge, forming Li2CO3, which leads to an irreversible capacity loss.
Most effort involved aprotic materials, which consist of a lithium metal anode, a liquid organic electrolyte and a porous carbon cathode. The electrolyte can be made of any organic liquid able to solvate lithium salts such as,,, and ), but typically consisted of carbonates, ethers and esters. The carbon cathode is usually made of a high-surface-area carbon material with a nanostructured metal oxide catalyst. A major advantage is the spontaneous formation of a barrier between anode and electrolyte that protects the lithium metal from further reaction with the electrolyte. Although rechargeable, the produced at the cathode is generally insoluble in the organic electrolyte, leading to buildup along the cathode/electrolyte interface. This makes cathodes in aprotic batteries prone to clogging and volume expansion that progressively reduces conductivity and degrades battery performance. Another issue is that organic electrolytes are flammable and can ignite if the cell is damaged.
Although most studies agree that is the final discharge product of non-aqueous Li-O2 batteries, considerable evidence that its formation does not proceed as a direct 2-electron electroreduction to peroxide O but rather via a one–electron reduction to superoxide O, followed by its disproportionation:
Superoxide has traditionally been considered as a dangerous intermediate in aprotic oxygen batteries due to its high nucleophilicity, basicity and redox potential However, reports suggest that LiO2 is both an intermediate during the discharge to peroxide and can be used as the final discharge product, potentially with an improved cycle life albeit with a lower specific energy. Indeed, it was shown that under certain conditions, the superoxide can be stable on the scale of 20–70 h at room temperature. An irreversible capacity loss upon disproportionation of LiO2 in the charged battery was not addressed.
Pt/C seems to be the best electrocatalyst for O2 evolution and Au/C for O2 reduction when is the product. Nevertheless, "the performance of rechargeable lithium–air batteries with non-aqueous electrolytes is limited by the reactions on the oxygen electrode, especially by O2 evolution. Conventional porous carbon air electrodes are unable to provide mAh/g and mAh/cm2 capacities and discharge rates at the magnitudes required for really high energy density batteries for EV applications." The capacity and the cycle life of non-aqueous Li-O2 batteries is limited by the deposition of insoluble and poorly electronically conducting LiOx phases upon discharge.. This makes the practical specific energy of Li-O2 batteries significantly smaller than the reagent-level calculation predicts. It seems that these parameters have reached their limits, and further improvement is expected only from alternative methods.

Mixed aqueous–aprotic

The aqueous–aprotic or mixed Li–air battery design attempts to unite advantages of the aprotic and aqueous battery designs. The common feature of hybrid designs is a two-part electrolyte connected by a lithium-conducting membrane. The anode abuts the aprotic side while the cathode is in contact with the aqueous side. A lithium-conducting ceramic is typically employed as the membrane joining the two electrolytes.
The use of a solid electrolyte is one such alternative approaches that allows for a combination of a lithium metal anode with an aqueous cathode. Ceramic solid electrolytes of the NASICON family has been studied. Compatible with water at alkaline pH and having a large electrochemical window, their low Li+ ion conductivity near room temperature makes them unsuitable for automotive and stationary energy storage applications that demand low cost. Further, both Ti and Ge are reduced by metallic Li, and an intermediate layer between the ceramic electrode and the negative electrode is required. In contrast, solid polymer electrolytes can provide a higher conductivity at the expense of a faster crossover of water and of other small molecules that are reactive toward metallic Li. Among the more exotic membranes considered for Li-O2 batteries is single-crystal silicon.
In 2015 researchers announced a design that used highly porous graphene for the anode, an electrolyte of lithium bis sulfonylimide/dimethoxyethane with added water and lithium iodide for use as a "mediator". The electrolyte produces lithium hydroxide at the cathode instead of lithium peroxide. The result offered energy efficiency of 93 percent and cycled more than 2,000 times with little impact on output. However, the design required pure oxygen, rather than ambient air.

Solid state

A solid-state battery design is attractive for its safety, eliminating the chance of ignition from rupture. Current solid-state Li–air batteries use a lithium anode, a ceramic, glass, or glass-ceramic electrolyte, and a porous carbon cathode. The anode and cathode are typically separated from the electrolyte by polymer–ceramic composites that enhance charge transfer at the anode and electrochemically couple the cathode to the electrolyte. The polymer–ceramic composites reduce overall impedance. The main drawback of the solid-state battery design is the low conductivity of most glass-ceramic electrolytes. The ionic conductivity of current lithium fast ion conductors is lower than liquid electrolyte alternatives.

Challenges

As of 2013, many challenges confronted designers.

Cathode

Most Li–air battery limits are at the cathode, which is also the source of its potential advantages. Incomplete discharge due to blockage of the porous carbon cathode with discharge products such as lithium peroxide is the most serious. Several modes of precipitates were modeled. A parameter, Da, was defined to measure the variations of temperature, species concentration and potentials.
The effects of pore size and pore size distribution remain poorly understood.
Catalysts have shown promise in creating preferential nucleation of over, which is irreversible with respect to lithium.
Atmospheric oxygen must be present at the cathode, but contaminants such as water vapor can damage it.

Electrochemistry

In 2017 cell designs, the charge overpotential is much higher than the discharge overpotential. Significant charge overpotential indicates the presence of secondary reactions. Thus, electric efficiency is only around 65%.
Catalysts such, Co, Pt and Au can potentially reduce the overpotentials, but the effect is poorly understood. Several catalysts improve cathode performance, notably, and the mechanism of improvement is known as surface oxygen redox providing abundant initial growth sites for lithium peroxide. It is also reported that catalysts may alter the structure of oxide deposits.
Significant drops in cell capacity with increasing discharge rates are another issue. The decrease in cell capacity is attributed to kinetic charge transfer limits. Since the anodic reaction occurs very quickly, the charge transfer limits are thought to occur at the cathode.

Stability

Long-term battery operation requires chemical stability of all cell components. Current cell designs show poor resistance to oxidation by reaction products and intermediates. Many aqueous electrolytes are volatile and can evaporate over time. Stability is hampered in general by parasitic chemical reactions, for instance those involving reactive oxygen.

Applications

Vehicles

Li–air cells are of interest for electric vehicles, because of their high theoretical specific and volumetric energy density, comparable to petrol. Electric motors provide high efficiency. Li–air cells could offer range equivalent to today's vehicles with a battery pack one-third the size of standard fuel tanks assuming the balance of plant required to maintain the battery was of negligible mass or volume.

Grid backup

In 2014, researchers announced a hybrid solar cell-battery. Up to 20% of the energy produced by conventional solar cells is lost as it travels to and charges a battery. The hybrid stores nearly 100% of the energy produced. One version of the hybrid used a potassium-ion battery using potassium–air. It offered higher energy density than conventional Li-ion batteries, cost less and avoided toxic byproducts. The latest device essentially substituted lithium for potassium.
The solar cell used a mesh made from microscopic rods of titanium dioxide to allow the needed oxygen to pass through. Captured sunlight produced electrons that decompose lithium peroxide into lithium ions, thereby charging the battery. During discharge, oxygen from air replenished the lithium peroxide.