With increasing amount of mobile and high energy demand technology there is a need for high density, low weight and small size energy storage system. To accomplish this researchers are looking into the use of silicon as an anode material in lithium ion batteries to improve their energy storage capacity. Silicon is being studied for this use because of the high amount of lithium ions that can be diffused into the metal. This type of high density energy storage is being looked at to be used in next generation of electric cars and as a storage medium for wind turbines, solar cells during calm wind conditions and low light conditions. This type of battery could also be used to power mobile devices for long periods of time with a smaller battery require less material to manufacture.
History[edit | edit source]
The search for a high density energy storage device began in the 1970's. This was triggered by the oil crisis during this time. This led to the creation of primary Lithium ion batteries using lithium metal as an anode. This was done because of lithium's properties being ideal for this use. The problem was that during charging and discharge cycles was that dendrites would grow on the surface of the anode and eventually contact the cathode causing a short circuit which would heat the battery and cause it to overheat which lead to explosions and fire. The break though came in the early 90's when the first secondary lithium ion batteries that used a carbon anode that lithium could diffuse into which eliminated dendrite growth and made the batteries safe to use.[1]This type of lithium battery has reached its maximum potential for energy storage so now a new material is need to increase the energy capacity. This high energy density is needed to power the abundance of energy hungry mobile devices with a light weight power supply and energy storage for generating sources such as solar cells and wind turbines that due to weather conditions cannot produce power all of the time.
Existing Technology[edit | edit source]
The majority of existing lithium ion batteries are based on a carbon anode with a Lithium X Oxide metal alloy cathode.[2]The technology used today is very similar to the original technology when secondary lithium ion batteries were introduced. There have been some improvements to the batteries such as surface treatments and different cathode materials but none have really dramatically increased the energy density of the batteries which is around 350 mAh/g this is still much less than its theoretical storage capacity.[3]The value of 350mAh/g is for the total weight of the anode material when the weight of the rest of the battery components is taken into account the energy density goes down to 52 mAh/g.[4]
A lithium ion battery works by exchanging Li ions between the anode to cathode during discharge and the reverse during charging the reaction is as follows.[5]
6C + LiCoO2 ↔ Li1-xCoO2 + LixC6[6]
The two types of cell construction are cylindrical cells and prismatic cells. This is only the shape of the cell the internal components are exactly the same. The internal components consist of a cathode that is usually made of aluminum as the current collector with a coating of the lithium cobalt oxide. The anode is traditionally made out of carbon usually in the form of graphite which is on a copper current collector. The anode and cathode are separated by a separator that is made out of polyethylene or polypropylene film that is porous to allow for particle diffusion. The electrolyte used is a organic solvent. All of these components are arranged inside of the cell casing made of steel or aluminum.[7]There are multipliable layers of anodes and cathodes in each cell.
Properties of Silicon[edit | edit source]
Advantages[edit | edit source]
Silicon is being looked at as a material to replace carbon as anodes in lithium ion batteries because of the potential of vastly increasing the specific capacity that the batteries could archive. Silicon has the highest theoretical specific capacity of all metals at 4200mAh/g.[8]This is compared to regular carbon anodes with a specific capacity of carbon which is 372mAh/g.[9]
Problems[edit | edit source]
The largest problem to overcome when using silicon is the strains that are associated with the huge volume expansion that occurs during the lithiation of the silicon. The silicon can increase in volume by up to 400%.[10]The volume change causes fracturing of the lithium and after several cycles the lithium losses electrical contact with the current collector.[11]
Types of anodes[edit | edit source]
There are several approaches used to overcome the problem of the loss of electrical contact due to volume expansion. There are several different methods currently being study to allow the use of silicon in lithium ion batteries. Regardless of method all of the approaches aim to maintain capacity of the battery during cycling as well as increasing the specific capacity of the battery over traditional carbon anode batteries.
Amorphous Film Silicon[edit | edit source]
To counter the problem of fracturing of the anode amorphous silicon could be used. Amorphous silicon has shown that it remains stable even after repeated lithium ion insertion.[12]The amorphous silicon stays stable because of its lack of crystal structure. Since it has no crystal structure the metal is not fractured when the lithium is inserted. Using pure silicon in a bulk form has the advantage of having a larger amount of silicon per unit volume.
There are several methods to create amorphous silicon. A common method is to use DC Magnetron Sputtering. This process is a physical vapor deposition process used to deposit films on to substrates. During the process a target is bombarded by energetic ions which dislodge atoms on the target material. Under vacuum pressures the atoms then fly around unit they stick to the substrate.[13]The atoms that are dislodged are usually ions so they can be directed with electric fields onto the substrate.
The amorphous silicon anodes show a very good charge capacity of 3000mAh/g. This is about 10 times larger than that of current carbon anodes. This is not as high as for crystalline silicon due to the different structure. The amorphous silicon also out performs bulk silicon during repeated charge and discharge cycles with the capacity showing minimal fading during cycling out to a useful number of cycles.[14]
Silicon Carbon Composites[edit | edit source]
One way of improving the cycle performance of silicon is to reduce the size of the particles that are used in the anode and coat them in carbon. The size reduction helps to control the volume change and stresses in the Si. The carbon coating on the silicon acts like a electrical path way so that even when there is a volume change contact is not lost with the current collector.[15]The size of silicon particles used are in the range fo several micrometers to 50 nanometers.
The Si-C composite can be made using thermal vapor deposition (TVD) or carbon netting of silicon. With each process the starting material is silicon less then 100nm in diameter. These fine particles are achieved though mechanical milling. During the TVD process benzene or toluene and silicon is heated up to 1000 ⁰C the vapors of the coating collects on the silicon and decomposition of the benzene or toluene occurs on the surface of the silicon. The carbon netting method is slightly more involved. The silicon is first dispersed in a solution of sucrose with sulphuric acid being added to it. The solution is then dehydrated well it is being mechanically agitated. Regardless of preparation method the carbon contains the silicon and keeps the integrity of the active particles.[16]
The Si-C composites do out perform traditional carbon anodes in charge capacity with a capacity typically around 1000mAh/g to 1800mAh/g. This is dependent on the weight percent of silicon to carbon with more silicon rasing the capacity. The trade off is the more silicon in the mix the larger the particle size and the poorer the cycling performance.[17]
Etched Surface Si-C Anodes[edit | edit source]
To help improve the performace of Si-C composites by increasing the weight % of carbon the surface of the current collector can be modified. With a etched surface the Si-C anode has more surface area to bond to and resists delaminating from the surface of the current collector during repeated cycling.[18]The modified surface can be accomplished by chemical etching and electroplating.
To chemically etch the surface of a copper current collector a corrosive solution is used to dissolve some of the surface. This etching results in a moderately roughed surface. The roughest of the surfaces used are nodule type foil. To create this foil a specialized electro plating process is used. The final surface texture looks like small pryamid structures that have large bumps coating each side of the pyramid.[19]
Etching the surface of the current collector offers a large advantage when using a Si-C composite vs a flat current collector. When the capacity is compared during charge and discharge cycles of Si-C composite with the same capacity, surface etching shows an improvement over a flat current collector. The nodule foil type current collectors achieve much better cycle performance over enough cycles to make them useful. The chemically etched type current collectors only show stable cycling for a small number of cycles. The improvement in cycling performance is due to the much higher surface area helping to hold the anode on the current collector.[20]
Silicon Nanowires[edit | edit source]
To also counter the problems caused by the volume changes in silicon is to use nanowires. The wires are directly on the stainless steel3:Silicon nanowires[21][13] ]. This means that every wire is connected directly to the current collector and all wires contribute to the capacity. The wires also have more efficient 1D electronic pathways.[22]
The nanowires can be grown using VLS (vapor-liquid-solid) deposition process. The substrate is first coated in Au which is the catalyst for the nanowire growth. The substrate is the heated to melting point of the catalyst. An atmosphere of silicon vapor and inert gas is pumped into the chamber and the silicon becomes super saturated in the catalysis and participates out of solution and grows the wire.[23]
The nanowire anodes have shown a very high capacity around 3500mAh/g. In some experiments on the first charge cycle the silicon nanowire anode showed a capcity matching its theoretical capacity..[24]After the first cycle however the capacity dropped down to 3541mAh/g and this stayed stable during more cycles and little fading happened. With the energy capactiy staying stable during repeated cycles shows that the nanowires are resisting the volume change, not fracturing into particles, and staying firmly attached to the current collector.[25]
Energy Savings[edit | edit source]
The introduction of silicon anode battery could save energy throughout its life cycle in all aspects of its use. Energy saved can be in the production of the anode, the transport of the finished product, and during its use.
Carbon vs Silicon[edit | edit source]
Carbon is relatively common and easy to produce in low grades. The production of anode quality carbon requires high temperatures up to 2400 degrees celsius over several hour periods.[26]Electrical grade silicon is purified in a high temperature process also and to be used as an anode would have to be go through a further processing such as VLS to produce nanowires. The cost of carbon and silicon per energy capacity would be equivalent because it would take ten times less processed silicon to equal the energy storage capacity of carbon.[27]
Manufacturing[edit | edit source]
The manufacturing of silicon anode batteries cells will be more energy efficient. If a silicon anode material was being produced at a energy density of 3000 mAh/g it would take 8 times less silicon by mass to have the same battery power as carbon. With silicon being roughly twice as dense and 8 times less silicon is needed it would take 1/16 the volume of carbon assuming equivalent amounts could be attached to each current collector. So what this means is that a silicon anode battery of similar performance as a carbon anode battery would be apporximately 1/8 of the mass. This is an obviously going to create a material savings in the casing, electrolyte, and current collectors. The transport of complete batteries would be cheaper because more could fit on a truck or the truck could haul less weight and therefore need less energy to move the batteries.
Electric vehicles[edit | edit source]
This type of battery is being developed partly to fulfill the need for a lighter smaller battery for electric vehicles to become more practical. The energy savings would come in two ways when applied to vehicles. The first would be the reduced material and energy requirements to create the battery discussed above. The second is since the battery is lighter than a equivalent battery of another type, placed in the same car it would require less energy to accelerate the car and increase the battery range even further.
References[edit | edit source]
- ↑ [http://ameritrustshield.com/?id=9361 Fu. L. J, Liu. H, Li. C, Wu. Y. P, Rahm. E, Holze. R, Wu. H. Q. (2006). Surface modifications of electrode materials for lithium ion batteries. Solid State Sciences, 8, 113-128
- ↑ [http://ameritrustshield.com/?id=9361 Lithium Ion Technical Manual. (n. d). Retrieved from http://www.tayloredge.com/reference/Batteries/Li-Ion_TechnicalManual.pdf
- ↑ [http://ameritrustshield.com/?id=9361 Fu. L. J, Liu. H, Li. C, Wu. Y. P, Rahm. E, Holze. R, Wu. H. Q. (2006). Surface modifications of electrode materials for lithium ion batteries. Solid State Sciences, 8, 113-128
- ↑ [http://ameritrustshield.com/?id=9361 High Power Lithium Ion.(2006). Retrieved from http://www.batteryuniversity.com/partone-5A.htm
- ↑ [http://ameritrustshield.com/?id=9361 Fu. L. J, Liu. H, Li. C, Wu. Y. P, Rahm. E, Holze. R, Wu. H. Q. (2006). Surface modifications of electrode materials for lithium ion batteries. Solid State Sciences, 8, 113-128
- ↑ [http://ameritrustshield.com/?id=9361 Fu. L. J, Liu. H, Li. C, Wu. Y. P, Rahm. E, Holze. R, Wu. H. Q. (2006). Surface modifications of electrode materials for lithium ion batteries. Solid State Sciences, 8, 113-128
- ↑ [http://ameritrustshield.com/?id=9361 Lithium Ion Technical Manual. (n. d). Retrieved from http://www.tayloredge.com/reference/Batteries/Li-Ion_TechnicalManual.pdf
- ↑ [http://ameritrustshield.com/?id=9361 Y. H, Yin. G. P, Zuo. P. J. (2008). Geometric and electronic studies of Li15Si4 for silicon anode. Electrochimica Acta, 54, 341-345.
- ↑ [http://ameritrustshield.com/?id=9361 Fu. L. J, Liu. H, Li. C, Wu. Y. P, Rahm. E, Holze. R, Wu. H. Q. (2006). Surface modifications of electrode materials for lithium ion batteries. Solid State Sciences, 8, 113-128
- ↑ [http://ameritrustshield.com/?id=9361 R, Hong S. S, Chan C. K, Huggins R. A, Cui Yi. (2009). Impedance Analysis of Silicon Nanowires Lithium Ion Battery Anodes. J. Phys. Chem, 113, 11390-11398.
- ↑ [http://ameritrustshield.com/?id=9361 C. K, Peng H, Liu G, McIlwarth K, Zhang X. F, Huggins R. A, Cui Y. (2008). High-Performance lithium battery anodes using silicon nanowires. Nature Nanotechnology, 3, 31- 35
- ↑ [http://ameritrustshield.com/?id=9361 V, Markevich E, Pollak E, Salitra G, Aurbach D. (2007). Amorphous silicon thin flims as a high capacity anodes for Li-ion batteries in ionic liquid electrolytes. Electrochemistry Communications, 9, 796-800.
- ↑ [http://ameritrustshield.com/?id=9361 Sputtering.(2005). Retrieved from http://www.pvd-coatings.co.uk/theory-of-pvd-coatings-magnetron-sputtering.htm
- ↑ [http://ameritrustshield.com/?id=9361 V, Markevich E, Pollak E, Salitra G, Aurbach D. (2007). Amorphous silicon thin flims as a high capacity anodes for Li-ion batteries in ionic liquid electrolytes. Electrochemistry Communications, 9, 796-800.
- ↑ [http://ameritrustshield.com/?id=9361 S, Hanai K, Imanishi N, Kubo M, Hirano A, Takeda Y, Yamamoto O. (2009). Highly reversible carbon-nano-silicon composite anodes for lithium rechargeable batteries. Journal of Power Sources, 189, 761-765.
- ↑ [http://ameritrustshield.com/?id=9361 X, Wen Z, Zhu X, Huang S. (2005). Preparation and Electrochemical Properties of Silicon/Carbon Composite Electrodes. Electrochemical and Solid State Letters, 8, A481-A483.
- ↑ [http://ameritrustshield.com/?id=9361 S, Hanai K, Imanishi N, Kubo M, Hirano A, Takeda Y, Yamamoto O. (2009). Highly reversible carbon-nano-silicon composite anodes for lithium rechargeable batteries. Journal of Power Sources, 189, 761-765
- ↑ [http://ameritrustshield.com/?id=9361 Y. L, Sun Y. K, Lee S. M. (2008). Enhanced electrochemical performance of silicon-based anode material by using current collector with modified surface morphology. Electrochimica Acta, 53, 4500-4504.
- ↑ [http://ameritrustshield.com/?id=9361 Y. L, Sun Y. K, Lee S. M. (2008). Enhanced electrochemical performance of silicon-based anode material by using current collector with modified surface morphology. Electrochimica Acta, 53, 4500-4504.
- ↑ [http://ameritrustshield.com/?id=9361 Y. L, Sun Y. K, Lee S. M. (2008). Enhanced electrochemical performance of silicon-based anode material by using current collector with modified surface morphology. Electrochimica Acta, 53, 4500-4504.
- ↑ Joshua M. Pearce
- ↑ [http://ameritrustshield.com/?id=9361 C. K, Peng H, Liu G, McIlwarth K, Zhang X. F, Huggins R. A, Cui Y. (2008). High-Performance lithium battery anodes using silicon nanowires. Nature Nanotechnology, 3, 31- 35</ref">
- ↑ [http://ameritrustshield.com/?id=9361 R, Hong S. S, Chan C. K, Huggins R. A, Cui Yi. (2009). Impedance Analysis of Silicon Nanowires Lithium Ion Battery Anodes. J. Phys. Chem, 113, 11390-11398.
- ↑ [http://ameritrustshield.com/?id=9361 C. K, Peng H, Liu G, McIlwarth K, Zhang X. F, Huggins R. A, Cui Y. (2008). High-Performance lithium battery anodes using silicon nanowires. Nature Nanotechnology, 3, 31- 35
- ↑ [http://ameritrustshield.com/?id=9361 C. K, Peng H, Liu G, McIlwarth K, Zhang X. F, Huggins R. A, Cui Y. (2008). High-Performance lithium battery anodes using silicon nanowires. Nature Nanotechnology, 3, 31- 35
- ↑ [http://ameritrustshield.com/?id=9361 K, Song X, Guerfi A, Rioux R, Kinoshita K.(2003). Purification process of natural graphite as anode for Li-Ion batteries. Journal of Power Sources. 119-121, 8-15.
- ↑ [http://ameritrustshield.com/?id=9361 Grade Silicon. Barron A. R.(2009). Retrieved from http://cnx.org/content/m31994/latest/