Handbook of Energy Storage for Transmission or ... - W2agz.com
Handbook of Energy Storage for Transmission or ... - W2agz.com Handbook of Energy Storage for Transmission or ... - W2agz.com
EPRI Proprietary Licensed Material Appendix – Electrochemical Capacitor Technology Traditional Capacitor Types There are three distinct types of capacitors: electrostatic, electrolytic, and electrochemical. The electrostatic capacitor was invented first. It is referred to historically as a Leyden jar capacitor and is very similar to the simple parallel-plate capacitor. An electrostatic capacitor is created by two conductors (metals) separated by an insulator (air or paper, for instance). Modern electrostatic capacitors use materials other than paper between the plates, for instance, different types of polymeric films, like Mylar or polypropylene. These films can be made quite thin so the metal plates can be spaced very close together. In fact, instead of metal plates, modern electrostatic capacitors consist of a polymeric film that has been vacuum coated with a thin metal coating on each face, forming a very thin structure that can be spiral wound. The thickness of the film dictates the separation between the plates. The dielectric constant of the film establishes the multiplicative factor previously described. High dielectric constants, very thin films, and high breakdown voltages are desired in such devices. Electrostatic capacitors are available in voltage ratings above 10 kV. Electrostatic capacitors are commonly used in high voltage utility applications, such as flexible AC transmission system (FACTS) devices. An electrolytic capacitor is more complicated than an electrostatic capacitor. It is comprised of two electrostatic capacitors in series, a cathode capacitor and an anode capacitor, separated by a liquid electrolyte. This electrolyte is an ion conductor but an electron insulator. The motivation for the development of an electrolytic capacitor was to achieve thinner plate separation thus higher energy than can be achieved by using paper or film dielectrics as with electrostatic capacitors. Electrolytic capacitors store energy across an oxide dielectric layer on a metal surface, an etched aluminum, for instance. A second material sometimes used for electrolytic capacitors is tantalum in the so-called wet-slug capacitor. The tantalum devices are expensive and commonly used only in high reliability applications. The dielectric of an electrolytic capacitor is anodically formed on the surface of a roughened substrate, for instance, aluminum foil. The dielectric thickness is dependent on the voltage used for its formation. Aluminum, for example, forms a dielectric film approximately 14 angstroms thick per volt applied. Thus the dielectric would be ~140 angstroms thick for a 10 V capacitor, clearly much thinner than possible for a polymer film. With such a thin dielectric film, it is not practical to apply the second electrode directly onto it. The approach taken is to use an ion-conducting electrolyte to provide this contact so the second capacitor becomes series-connected with the first. This second capacitor is typically created in a similar manner but with a thinner dielectric layer and, therefore, with much higher capacitance. Thus, an electrolytic capacitor consists of two capacitors in series with one having substantially higher capacitance than the other. This makes the capacitance of the device very close to the smaller of the series-connected capacitors, the one formed at higher (positive) voltage. Electrochemical Capacitors 56
EPRI Proprietary Licensed Material Electrolytic capacitors are generally constructed in a spiral wound configuration. Besides aluminum, these capacitors can be made using tantalum or niobium. Electrolytic capacitor technology today provides devices rated up to 600 V. These capacitors are widely used in filtering applications (dc) because of their relatively low cost, high energy density, and low power dissipation. These are the upright tubular capacitors that are commonly seen in power supplies. The third distinct type of capacitor is designated as electrochemical, and has been referred to as electric double layer ultra capacitors. Electrochemical capacitors store energy by charge separation at the interface between a solid electrode and an electrolyte. Individual capacitor cells operate at low voltage (< 2.7 V) compared to electrostatic or electrolytic capacitors. What makes them interesting is that electrochemical capacitors can have much higher energy densities than other types of capacitors. Thus, they can deliver the energy over longer times than electrostatic and electrolytic capacitors of the same physical size. A common application of small electrochemical capacitors is to provide power for computer memory backup during power outage. The electrochemical capacitor, in its simplest form, is comprised of two double layer charge storage surfaces in series, i.e. two electrostatic capacitors in series. The double layer charge storage surface is formed at the interface between a conductor and an electrolyte when a voltage is imposed across them. Essentially there is an increase in the electrolyte ion concentration, with a change in electrolyte ion orientation, near the surface of the electrode. Charge separation at this interface occurs over a very short distance, ~10 angstroms. Thus, very large capacitance values, on the order of 100 Farads/gram of material, can be obtained with the use of a high surface area conductor like activated carbon. Although the double layer phenomenon has been known for more than 100 years, the first practical device was created in the late 1960’s. Ideal Capacitor and ESR An ideal capacitor is a fundamental circuit element and has no resistive or inductive components. In reality, the first order model of an actual capacitor is a series combination of an inductor, a resistor, and a capacitor. The series resistance and inductance are intrinsic to the construction of the capacitor and are dependent on the design characteristics of the device, such as its geometry and physical size. Note that series resistance is also referred to as the equivalent series resistance, ESR. The series-RLC circuit has a characteristic frequency f o , the self-resonance frequency, at which the magnitude of the impedance is a minimum. This self-resonant frequency occurs when the inductance and the capacitance balance each other to produce an impedance equal to the series resistance value. This frequency occurs at f o = 1/ 2π√(LC). At frequencies below f o , capacitive behavior is dominant; above this frequency inductive behavior is dominant. The series resistance can be measured precisely at frequency f o . The self-resonant frequency of electrostatic capacitors can be in the MHz or higher range, depending on the size and design of the device. The self-resonance frequency for electrolytic capacitors is generally in the range of kHz to tens of kHz because the capacitance is much larger and the inductance is also higher, making the resonance frequency lower. For large electrochemical capacitors, the self-resonant frequency is Electrochemical Capacitors 57
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Electrolytic capacit<strong>or</strong>s are generally constructed in a spiral wound configuration. Besides<br />
aluminum, these capacit<strong>or</strong>s can be made using tantalum <strong>or</strong> niobium. Electrolytic<br />
capacit<strong>or</strong> technology today provides devices rated up to 600 V. These capacit<strong>or</strong>s are<br />
widely used in filtering applications (dc) because <strong>of</strong> their relatively low cost, high energy<br />
density, and low power dissipation. These are the upright tubular capacit<strong>or</strong>s that are<br />
<strong>com</strong>monly seen in power supplies.<br />
The third distinct type <strong>of</strong> capacit<strong>or</strong> is designated as electrochemical, and has been<br />
referred to as electric double layer ultra capacit<strong>or</strong>s. Electrochemical capacit<strong>or</strong>s st<strong>or</strong>e<br />
energy by charge separation at the interface between a solid electrode and an electrolyte.<br />
Individual capacit<strong>or</strong> cells operate at low voltage (< 2.7 V) <strong>com</strong>pared to electrostatic <strong>or</strong><br />
electrolytic capacit<strong>or</strong>s. What makes them interesting is that electrochemical capacit<strong>or</strong>s<br />
can have much higher energy densities than other types <strong>of</strong> capacit<strong>or</strong>s. Thus, they can<br />
deliver the energy over longer times than electrostatic and electrolytic capacit<strong>or</strong>s <strong>of</strong> the<br />
same physical size. A <strong>com</strong>mon application <strong>of</strong> small electrochemical capacit<strong>or</strong>s is to<br />
provide power <strong>f<strong>or</strong></strong> <strong>com</strong>puter mem<strong>or</strong>y backup during power outage.<br />
The electrochemical capacit<strong>or</strong>, in its simplest <strong>f<strong>or</strong></strong>m, is <strong>com</strong>prised <strong>of</strong> two double layer<br />
charge st<strong>or</strong>age surfaces in series, i.e. two electrostatic capacit<strong>or</strong>s in series. The double<br />
layer charge st<strong>or</strong>age surface is <strong>f<strong>or</strong></strong>med at the interface between a conduct<strong>or</strong> and an<br />
electrolyte when a voltage is imposed across them. Essentially there is an increase in the<br />
electrolyte ion concentration, with a change in electrolyte ion <strong>or</strong>ientation, near the surface<br />
<strong>of</strong> the electrode. Charge separation at this interface occurs over a very sh<strong>or</strong>t distance,<br />
~10 angstroms. Thus, very large capacitance values, on the <strong>or</strong>der <strong>of</strong> 100 Farads/gram <strong>of</strong><br />
material, can be obtained with the use <strong>of</strong> a high surface area conduct<strong>or</strong> like activated<br />
carbon. Although the double layer phenomenon has been known <strong>f<strong>or</strong></strong> m<strong>or</strong>e than 100<br />
years, the first practical device was created in the late 1960’s.<br />
Ideal Capacit<strong>or</strong> and ESR<br />
An ideal capacit<strong>or</strong> is a fundamental circuit element and has no resistive <strong>or</strong> inductive<br />
<strong>com</strong>ponents. In reality, the first <strong>or</strong>der model <strong>of</strong> an actual capacit<strong>or</strong> is a series<br />
<strong>com</strong>bination <strong>of</strong> an induct<strong>or</strong>, a resist<strong>or</strong>, and a capacit<strong>or</strong>. The series resistance and<br />
inductance are intrinsic to the construction <strong>of</strong> the capacit<strong>or</strong> and are dependent on the<br />
design characteristics <strong>of</strong> the device, such as its geometry and physical size. Note that<br />
series resistance is also referred to as the equivalent series resistance, ESR.<br />
The series-RLC circuit has a characteristic frequency f o , the self-resonance frequency, at<br />
which the magnitude <strong>of</strong> the impedance is a minimum. This self-resonant frequency<br />
occurs when the inductance and the capacitance balance each other to produce an<br />
impedance equal to the series resistance value. This frequency occurs at f o = 1/ 2π√(LC).<br />
At frequencies below f o , capacitive behavi<strong>or</strong> is dominant; above this frequency inductive<br />
behavi<strong>or</strong> is dominant. The series resistance can be measured precisely at frequency f o .<br />
The self-resonant frequency <strong>of</strong> electrostatic capacit<strong>or</strong>s can be in the MHz <strong>or</strong> higher range,<br />
depending on the size and design <strong>of</strong> the device. The self-resonance frequency <strong>f<strong>or</strong></strong><br />
electrolytic capacit<strong>or</strong>s is generally in the range <strong>of</strong> kHz to tens <strong>of</strong> kHz because the<br />
capacitance is much larger and the inductance is also higher, making the resonance<br />
frequency lower. F<strong>or</strong> large electrochemical capacit<strong>or</strong>s, the self-resonant frequency is<br />
Electrochemical Capacit<strong>or</strong>s 57