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| Fig. 1. Power and energy densities of various energy-storage systems. |
Renewable energy sources, including wind and solar, can supply a significant amount of electrical energy in the United States and around the world. However, because of their intermittent nature, the potential of these two energy sources can be fully exploited only if efficient, safe, cost-effective, and reliable electrical energy-storage systems are provided. Storage systems will also be critical to improving the robustness and efficiency of the electrical distribution grid by reducing power surges and balancing the load over time. Energy-storage technologies suitable for applications involving various power capacities and storage time (energy capacity) are shown in Figure 1. For very large energy-storage applications, only pumped-hydro and compressed-gas are cost effective at this time. However, these technologies are limited by geography, while electrochemical energy-storage devices such as batteries, flow batteries, fuel cells, and electrochemical capacitors are promising because of their scalability and versatility. The size (weight and volume) of the device is not as critical for large scale energy storage as it is for portable and transportation applications. Capacitors have fast sub-second response times, deep discharge capability, and can deliver high power but for only short times, so these devices are more suitable for power quality management. Most fuel cells cannot be reversed electrically efficiently, as discussed below. Consequently, only batteries, both conventional and flow batteries, have the energy capacities needed for large-scale electrical energy storage.
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| Fig. 2. Schematic of a redox flow-battery system shown in a discharge mode. |
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| Fig. 3. An exploded view of a single redox flow-battery cell. |
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| Fig. 4. Schematics representing the electrochemical reactions in the iron/chrome redox battery. |
Most redox flow batteries consist of two separate electrolytes, one storing the electro-active materials for the negative electrode reactions and the other for the positive electrode reactions. (To prevent confusion, the negative electrode is the anode and the positive electrode is the cathode during discharge. It is to be noted that these names will be reversed during charge, while the polarity of the electrodes, negative/positive, remains unchanged.) Both the fresh and spent electrolytes may be circulated and stored in a single storage tank as shown in Figure 2. An ion selective membrane is often used to prevent mixing or cross-over of the electro-active species which results in chemical short-circuit of electro-active materials. Only the common counter-ion carrier is allowed to cross the membrane. Figure 4 shows a simplified drawing of the electrochemical charging reactions one of the most commonly suggested redox battery for utility scale application, the iron/chrome system. During power generation (discharge of the battery) the chromium ion oxidizes the iron ion in the solution. In this system the separator allows passage of a chloride anion to balance the charge. Details of these reactions, together with the description of a number of other possible flow-battery systems are shown in the Appendix.
A fuel cell might be considered as a type of flow battery in that the power conversion component is independent of the chemical energy capacity of the device. Most fuel cells involve oxygen at the positive electrode, and cannot be reversed electrically efficiently, and consequently cannot be used effectively as an electrical energy-storage device. The exception might be a high temperature solid oxide fuel cell.
The energy-capacity requirement of a flow battery is determined by the size of the external storage components. Consequently, a redox flow-battery system could approach its theoretical energy density as the system is scaled up to a point where the weight or volume of the battery is small relative to that of the stored fuel and oxidant. An analogous, but conventional system is the internal combustion engine system, in which the power is determined by the size of the engine and the energy capacity is determined by the size of the fuel tank.
A flow battery has a safety advantage that comes from storing the active materials separately from the reactive point source. Other advantages are quick response times (common to all battery systems), high electricity-to-electricity conversion efficiency, no cell-to-cell equalization requirement, simple state-of-charge indication (based on electro-active concentrations), low maintenance, tolerance to overcharge and over-discharge, and perhaps most importantly, the tolerance for deep discharges without affecting cycle life. The hybrid systems like those involving zinc plating do not offer all these advantages, but still have many of the desirable features of a true flow battery. The main disadvantage of flow batteries is their more complicated system requirements of pumps, sensors, flow and power management, and secondary containment vessels, making them most suitable for large-scale storage applications.
The cost of an energy-storage device is a major impediment to utility adoption. For example, in the vanadium flow-battery system, one of the few redox flow batteries that have been tested at the utility scale, vanadium itself is a significant cost contributor. Analysis suggests that the cost of vanadium chemicals varies widely, but could contribute between $50/kWh to $110/kWh, or from 50-100% of the cost target of $100-$200/kWh for the energy-storage system. From this standpoint, identifying low cost redox couples with high solubility is critical to meeting market requirements.
The other key cost factor is the construction of the electrochemical cell itself. The construction cost of the cell scales with the total power requirement of the application, but these costs are directly related to the specific power of the device itself - how effectively the rates of the materials are utilized. While flow batteries ought to be able to operate at relatively high current densities, as convection can be employed to deliver reactants to the electrode surface, flow batteries have typically been operated at ~50 mA/cm2, a current density consistent with conventional batteries without convection. It is anticipated that electrolyte management and cell design can deliver at least 5- to 10-fold improvement in power density, thereby reducing the stack cost.
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| Fig. 5. Schematics representing the electrochemical reactions in the all vanadium redox battery. |
Both the fresh and spent electrolytes may be circulated and stored in a single storage tank as shown in Figure 2, or in separate tanks to control the concentrations of the electro-active material. An ion selective membrane is often used to prevent mixing or cross-over of the electro-active species which results in chemical short-circuit of electro-active materials. Only the common counter ion carrier is allowed to cross the membrane. For example, in the bromine-polysulfide system, as Na2S2 is converted to Na2S4 at the negative electrode and Br2 is converted to 2Br- at the positive electrode, the excess Na+ ions at the negative electrode are allowed to cross to the positive electrode to maintain electroneutrality. Figure 4 and 5 show a simplified drawing of the electrochemical reactions for two common redox flow-battery couples; the iron/chrome system and the all vanadium system. In the iron/chrome system the separator allows passage of an anion to balance the charge. This system was one of the earlier flow-battery chemistries studied for utility scale application. In the vanadium system, as V+2 is oxidized to V+3 at the negative electrode and V+5 is reduced to V+4 at the positive electrode, hydronium ions are transported across a proton conducting membrane from the negative electrode to the positive electrode. In this case, however sometimes a microporous non-selective membrane separator can be used since most of the current might be carried by high mobility protons in the acid electrolyte and since the cross-over of the common vanadium cation lowers efficiency but does not cause a permanent loss of capacity.
| Table I. Characteristics of some flow-battery systems | |||
| System | Reactions top: negative; bottom: positive electrode charge: <== ; discharge: ==> |
Eocell | Electrolyte -/+ electrode |
| Redox | |||
| All vanadium | V2+ <==> V3+ + e- VO2+ + e- <==> VO2+ |
1.4 V | H2SO4/H2SO4 |
| Vanadium-polyhalide | V2+ <==> V3+ + e- ½Br2 + e- <==> Br- |
1.3 V | VCl3-HCl/NaBr-HCl |
| Bromine-polysulfide | 2S22- <==> S42- + 2e- Br2 + 2e- <==> 2Br- |
1.5 V | NaS2/NaBr |
| Iron-chromium | Fe2+ <==> Fe3+ + e- Cr3+ + e- <==> Cr2+ |
1.2 V | HCl-FeCl2-CrCl3 (both sides) |
| Hydrogen-bromine | H2 <==> 2H+ + 2e- Br2 + 2e- <==> 2Br- |
1.1 V | HBr-PEM* |
| Hybrid | |||
| Zinc-bromine | Zn <==> Zn2+ + 2e- Br2 + 2e- <==> 2Br- |
1.8 V | ZnBr2/ZnBr2 |
| Zinc-cerium | Zn <==> Zn2+ + 2e- 2Ce4+ + 2e- <==> 2Ce3+ |
2.4 V | CH3SO3H (both sides) |
| * Proton exchange membrane | |||
Listings of electrochemistry books, review chapters, proceedings volumes, and full text of some historical publications are also available in the Electrochemistry Science and Technology Information Resource (ESTIR). (http://electrochem.cwru.edu/estir/)
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