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

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EPRI Proprietary Licensed Material Description Introduction Discovered by Henrich Helmholtz in the 1800s, electrochemical capacitors were first practically used in 1979 for memory backup in computers and are now manufacturer by many companies. Electrochemical capacitors are distinguished from other types as “double-layer capacitors 1 .” Manufactured products have also been given names including “super,” “ultra,” “gold,” “pseudo,” as well as “electric double-layer” capacitors. Double layer electrochemical capacitors differ from other types by having capacitance and energy density values several orders of magnitude larger than even the largest electrolytic-based capacitor. They are true capacitors in that energy is stored via electrostatic charges on opposing surfaces, and they can withstand a large number of charge/discharge cycles without degradation. They are also similar to batteries in many respects, including the use of liquid electrolytes, and the practice of configuring various size cells into modules to meet power, energy, and voltage requirements of a wide range of applications. The first products were rated at two to five volts and had capacitance values measured in fractions of a Farad to several Farads. Although early applications were primarily computer memory backup, the technology has evolved to larger scale applications. Today’s devices range in size up to hundreds of thousands of Farads at low voltage and, in some applications, systems voltages (multiple series-connected capacitors) are above 600 V. The technology has grown into an industry with an annual sales estimated to be $100 million. It is poised for rapid growth in the near future with higher energy and higher voltage devices suitable for power quality and advanced transportation applications. With the advent of distributed power generation, capacitors are being considered for fuel cell and micro-turbine load inrush support, and for leveling fluctuating energy flow from natural sources like wind turbines or solar. Capacitor Fundamentals A capacitor is a device used for storing electrical charge. There are three distinct types of capacitors: electrostatic, electrolytic, and electrochemical, see appendix for a description of each type. The simplest capacitor is a parallel-plate electrostatic. It has two conductors of area A separated by a distance t. The region between the plates is usually filled with air, paper or other dielectric material, which increases the stored energy in the device. The charge, Q, that is stored in the device, is proportional to the voltage applied to the conductors. This proportionality constant is the capacitance. The capacitance C is equal to the dielectric constant times the area divided by the separation. 1 There is some uncertainty within the industry on the exact name for capacitors with massive storage capability. This is in part due to the many names of products by different manufacturers, but also due to the relative newness of the industry and recent advances. An electrochemical capacitor commonly stores energy through non-faradic processes (electrostatic). However, faradic processes (electron transfer due to chemical or oxidation state changes) can and do occur. Because both processes can occur, the generic term electrochemical is more appropriate than double-layer electrochemical capacitor, which also excludes the mixed-metal-oxide capacitor technology. In general, this report uses the generic term electrochemical capacitor as suggested by A. Burke and endorse by B. Conway and J. Miller. Electrochemical Capacitors 8

EPRI Proprietary Licensed Material The energy E, that is stored in an ideal capacitor at voltage V, is equal to: E = 0.5 CV 2 The energy increases as the square of the applied voltage. When charged at a constant current, the voltage of an ideal capacitor rises linearly with time. When charged at a constant power, the stored energy rises linearly with time. In reality, the first order model of a capacitor is a series combination of an inductor, a resistor, and a capacitor (see Appendix for additional modeling details). The fundamental equations for all types of capacitors are summarized in Table 1. Note that R s , the series resistance, is also referred to as the equivalent series resistance, ESR. Table 1 Fundamental equations for all capacitors including electrochemical capacitors. Stored Charge, Q Q = CV C = capacitance Stored energy, E, ideal case E = ½ CV 2 V = applied voltage ε = dielectric constant Capacitance of parallel C = εA/t A = area of the capacitor plate plate capacitor, C T = separation of the plates Self-resonant frequency, f o , 1 f for RLC circuit o = 2 Π LC L = inductance Maximum power, P max P max = V 2 /4R s R s = series resistance (ESR) Resistive charge or R = 100 discharge efficiency, η RL + RS Constant current charge or 100( Vr − I oRS ) η = discharge efficiency, η ( V + I R ) L η R L = load resistance r o Electrochemical Capacitors 9 S Vr = rated voltage I o = fixed current For most practical applications in the utility industry, the inductance in the series-RLC circuit can be ignored because operation is well below the self-resonant frequency. Thus, a simple series-RC circuit is a good first-order model for the real capacitor. It is important to understand the effect of the capacitor internal resistance (R s ) on the efficiency of discharge. For example, modeling the capacitor as series-RC circuit being discharged into a resistive load R L the efficiency of discharge in percent is equal to 100R L /(R S + R L ). Thus the efficiency is nearly 100% when the load resistance, R L , is much greater than the internal resistance, R S . On the other hand, the efficiency is exactly 50% for the matched load, that is when R L = R S . That is, for a matched load half the delivered energy is dissipated in the capacitor itself and not in the load. Similar efficiency relationships can be calculated for constant current charge or discharge, as listed in Table 1. Electrochemical Capacitor Characteristics What Is a Double-Layer Capacitor Electrochemical capacitors consist of two electrodes, a separator, electrolyte, two current collectors, and packaging. Within the electrochemical capacitor, charge is stored electrostatically, not chemically as in a battery. It has, as a dielectric, an electrolyte solvent, typically potassium hydroxide or sulfuric acid, and is actually two capacitors

EPRI Proprietary Licensed Material<br />

The energy E, that is st<strong>or</strong>ed in an ideal capacit<strong>or</strong> at voltage V, is equal to:<br />

E = 0.5 CV 2<br />

The energy increases as the square <strong>of</strong> the applied voltage. When charged at a constant<br />

current, the voltage <strong>of</strong> an ideal capacit<strong>or</strong> rises linearly with time. When charged at a<br />

constant power, the st<strong>or</strong>ed energy rises linearly with time. In reality, the first <strong>or</strong>der model<br />

<strong>of</strong> a capacit<strong>or</strong> is a series <strong>com</strong>bination <strong>of</strong> an induct<strong>or</strong>, a resist<strong>or</strong>, and a capacit<strong>or</strong> (see<br />

Appendix <strong>f<strong>or</strong></strong> additional modeling details). The fundamental equations <strong>f<strong>or</strong></strong> all types <strong>of</strong><br />

capacit<strong>or</strong>s are summarized in Table 1. Note that R s<br />

, the series resistance, is also referred<br />

to as the equivalent series resistance, ESR.<br />

Table 1 Fundamental equations <strong>f<strong>or</strong></strong> all capacit<strong>or</strong>s including electrochemical capacit<strong>or</strong>s.<br />

St<strong>or</strong>ed Charge, Q Q = CV C = capacitance<br />

St<strong>or</strong>ed energy, E, ideal case E = ½ CV 2 V = applied voltage<br />

ε = dielectric constant<br />

Capacitance <strong>of</strong> parallel<br />

C = εA/t A = area <strong>of</strong> the capacit<strong>or</strong> plate<br />

plate capacit<strong>or</strong>, C<br />

T = separation <strong>of</strong> the plates<br />

Self-resonant frequency, f o ,<br />

1<br />

f<br />

<strong>f<strong>or</strong></strong> RLC circuit<br />

o<br />

=<br />

2 Π LC<br />

L = inductance<br />

Maximum power, P max P max = V 2 /4R s R s = series resistance (ESR)<br />

Resistive charge <strong>or</strong><br />

R<br />

= 100<br />

discharge efficiency, η<br />

RL<br />

+ RS<br />

Constant current charge <strong>or</strong> 100( Vr<br />

− I<br />

oRS<br />

)<br />

η =<br />

discharge efficiency, η ( V + I R )<br />

L<br />

η R L = load resistance<br />

r<br />

o<br />

Electrochemical Capacit<strong>or</strong>s 9<br />

S<br />

Vr = rated voltage<br />

I o = fixed current<br />

F<strong>or</strong> most practical applications in the utility industry, the inductance in the series-RLC<br />

circuit can be ign<strong>or</strong>ed because operation is well below the self-resonant frequency. Thus,<br />

a simple series-RC circuit is a good first-<strong>or</strong>der model <strong>f<strong>or</strong></strong> the real capacit<strong>or</strong>.<br />

It is imp<strong>or</strong>tant to understand the effect <strong>of</strong> the capacit<strong>or</strong> internal resistance (R s ) on the<br />

efficiency <strong>of</strong> discharge. F<strong>or</strong> example, modeling the capacit<strong>or</strong> as series-RC circuit being<br />

discharged into a resistive load R L the efficiency <strong>of</strong> discharge in percent is equal to<br />

100R L /(R S + R L ). Thus the efficiency is nearly 100% when the load resistance, R L , is<br />

much greater than the internal resistance, R S . On the other hand, the efficiency is exactly<br />

50% <strong>f<strong>or</strong></strong> the matched load, that is when R L = R S . That is, <strong>f<strong>or</strong></strong> a matched load half the<br />

delivered energy is dissipated in the capacit<strong>or</strong> itself and not in the load. Similar<br />

efficiency relationships can be calculated <strong>f<strong>or</strong></strong> constant current charge <strong>or</strong> discharge, as<br />

listed in Table 1.<br />

Electrochemical Capacit<strong>or</strong> Characteristics<br />

What Is a Double-Layer Capacit<strong>or</strong><br />

Electrochemical capacit<strong>or</strong>s consist <strong>of</strong> two electrodes, a separat<strong>or</strong>, electrolyte, two current<br />

collect<strong>or</strong>s, and packaging. Within the electrochemical capacit<strong>or</strong>, charge is st<strong>or</strong>ed<br />

electrostatically, not chemically as in a battery. It has, as a dielectric, an electrolyte<br />

solvent, typically potassium hydroxide <strong>or</strong> sulfuric acid, and is actually two capacit<strong>or</strong>s

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