SECTION 2: ENERGY STORAGE FUNDAMENTALS. ESE 471 Energy Storage Systems

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Transcription:

SECTION 2: ENERGY STORAGE FUNDAMENTALS ESE 471 Energy Storage Systems

2 Performance Characteristics

Energy Storage Performance Characteristics 3 Defining performance characteristics of energy storage mechanisms Capacity Power Efficiency

Capacity 4 Capacity The amount of energy that a device can store Total energy capacity, EE tt Total energy stored in a device when fully charged Usable energy capacity, EE uu The total energy that can be extracted from a device for use Difference between stored energy at maximum state of charge (SoC) and minimum SoC In general, storage devices are not fully discharged, so typically EE uu < EE tt

Capacity 5 Units of capacity: Watt-hours (Wh) (Ampere-hours, Ah, for batteries) State of charge (SoC) The amount of energy stored in a device as a percentage of its total energy capacity Fully discharged: SoC = 0% Fully charged: SoC = 100% Depth of discharge (DoD) The amount of energy that has been removed from a device as a percentage of the total energy capacity

Capacity 6 We can also characterize storage devices in terms of size or mass required for a given capacity Specific energy Usable energy capacity per unit mass Units: Wh/kg Energy density ee mm = EE uu mm Usable energy capacity per unit volume Units: Wh/m 3 or Wh/L ee vv = EE uu VV These are very often used (incorrectly) interchangeably

Power 7 Power is an important metric for a storage system Rate at which energy can be stored or extracted for use Charge/discharge rate Limited by loss mechanisms Specific power Power available from a storage device per unit mass Units: W/kg Power density pp mm = PP mm Power available from a storage device per unit volume Units: W/m 3 or W/L pp vv = PP VV

Power vs. Energy 8 Capacity and the rate at which energy can be stored or extracted are different characteristics Applications determine which is most important High specific power Low specific energy Low specific power High specific energy www.tecategroup.com

Efficiency 9 Another important performance characteristic is efficiency The percentage of energy put into storage that can later be extracted for use All storage systems suffer from losses Losses as energy flows into storage Losses as energy is extracted from storage

Round-Trip Efficiency 10 Round-trip efficiency Energy extracted from a storage system as a percentage of the energy put into the system ηη rrrr = EE oooooo EE iiii ηη rrrr = EE iiii EE llllllll,iiii EE llllllll,oooooo EE iiii

Round-Trip Efficiency 11 We can define a charging efficiency Amount of energy stored as a percentage of the energy input ηη iiii = EE ss EE iiii = EE iiii EE llllllll,iiii EE iiii And a discharging efficiency Amount of energy output as a percentage of the energy stored ηη oooooo = EE oooooo EE ss = EE ss EE llllllll,oooooo EE ss ηη oooooo = EE iiii EE llllllll,iiii EE llllllll,oooooo EE iiii EE llllllll,iiii

Round-Trip Efficiency 12 The round trip for energy in a storage system is a cascade of the charge and discharge processes Round trip efficiency given by: ηη rrrr = ηη iiii ηη oooooo In general, efficiency is a function of: Charging/discharging power, PP iiii and PP oooooo State of charge

Charging Time 13 Typically, what is needed is a certain power for a certain time Charging time The time it takes to go from minimum SoC to maximum SoC at a given power input The time it takes to store the usable energy, EE uu tt cc = EE uu PP cc where PP cc is the rate of energy storage Note that, due to losses, the rate of energy storage, PP cc, is less than the input power, PP iiii

Charging Time 14 The power we have direct control over is the input power, PP iiii The charging time in terms of input power is tt cc = EE uu PP iiii PP llllllll,iiii = EE uu PP iiii ηη iiii

Discharge Time 15 Discharge time The time required to go from maximum SoC to minimum SoC at a given output power Due to losses, the rate of discharge, PP dd, is greater than the output power, PP oooooo tt dd = EE uu PP dd Again, the power of interest is the power we have direct control over, the output power, PP oooooo, so tt dd = EE uu PP oooooo + PP llllllll,oooooo = EE uu PP oooooo /ηη oooooo = EE uu PP oooooo ηη oooooo

16 Ragone Plots

Ragone Plots 17 Two primary figures of merit for energy storage systems: Specific energy Specific power Often a tradeoff between the two Different storage technologies best suited to different applications depending on power/energy requirements Storage technologies can be compared graphically on a Ragone plot Specific energy vs. specific power Specific storage devices plotted as points on the plot, or Categories of devices plotted as regions in the Ragone plane

Ragone Plots 18

Discharge Time 19 Any given storage system will have a specific energy capacity and a specific power rating A point in the Ragone plane, (pp mm,ee mm ) Discharge time at rated power for that point (neglecting losses): tt dd = ee mm pp mm Constant discharge time maps to lines with unity slope on a Ragone plot Storage systems that lie on the same line have equal discharge times at rated power

Ragone Curves 20 Ragone plots we ve seen so far plot a storage device at one operating point Maximum or rated power Can also depict a device s energy capacity over a range of power A Ragone curve Most curves share a similar characteristic shape Available energy decreases at higher power Fraction of energy lost as heat increases

Thévenin Equivalent Model 21 What is the reason for the characteristic shape of Ragone curves? Consider that we could model a storage device with as an electrical Thévenin equivalent Need not be an electrical storage device Open-circuit voltage is some function of SoC Possibly linear May be highly nonlinear Or, could be constant

Thévenin Equivalent Model 22 Three power components associated with discharge PP dd : discharge power The rate at which energy leaves storage: PP dd = VV oooo ii oo PP llllllll : power lost during discharge Modeled as heat dissipation in the Thévenin resistance: PP llllllll = ii 2 oo RR ss PP oooooo : output power flowing to the external system PP oooooo = vv oo ii oo = VV oooo ii oo RR ss ii oo PP oooooo = VV oooo ii oo ii 2 oo RR ss = PP dd PP llllllll

Thévenin Equivalent Model 23 Discharge time: tt dd = EE uu PP dd Amount of energy extracted from the storage system: EE oooooo = PP oooooo tt dd = EE uu PP oooooo PP dd Substituting in expressions for PP oooooo and PP dd, we have EE oooooo = EE uu EE oooooo = EE uu VV oooo ii oo ii oo 2 RR ss VV oooo ii oo 1 ii oo RR ss VV oooo

Available Energy vs. Output Power 24 EE oooooo = EE uu 1 ii oo RR ss VV oooo We can see that the available energy decreases as ii oo increases Available energy decreases as output power increases Illustrated by the characteristic shape of Ragone plots

25 Storage System Configurations

Storage System Configurations 26 Our focus is grid-connected energy storage Energy stored in many different domains Input and output energy is electrical Three-phase AC power Conversion is required between the storage domain and the electrical domain Transformer Power conversion system (PCS)

System Configurations Mechanical 27 Mechanical storage Pumped hydro, flywheels, compressed air PCS includes a motor/generator Possibly driven by a turbine Motor/generator may be connected directly to the grid Synchronous with the grid Runs at fixed speed

System Configurations Mechanical 28 Alternatively, motor/generator can be run at variable speed Maximize efficiency Interface to grid through power electronic converter Two options for variable-speed operation: Singly-fed motor/generator Doubly-fed motor/generator

System Configurations Mechanical 29 Singly-fed motor/generator Synchronous machine Stator driven with variable-frequency AC from power electronic converter Field windings on rotor supplied with DC excitation voltage Same as for fixed-speed synchronous machine Converter must be rated for full motor/generator power Large, expensive

System Configurations Mechanical 30 Doubly-fed motor/generator Doubly-fed asynchronous machine (DFAM) Stator connected to grid-frequency AC Field windings on rotor supplied with variable-frequency excitation voltage Converters need not be sized for rated motor/generator power Only supply lower-power excitation to the rotor

Power Electronic Converters 31 Variable-speed motors/generators require a static frequency converter (SFC) Both for singly- and doubly-fed configurations Power electronic switching converter Convert between grid-frequency to other frequencies Common SFC topologies Cycloconverter (CCV) AC-AC converter Voltage-source converter (VSC) AC-DC-AC converter

Cycloconverter 32 Cycloconverter AC-to-AC frequency converter Direct conversion between grid and variable frequency AC No intermediate DC link Switching thyristor bridge circuits Controllable connections between all input and output phases

Voltage Source Converter 33 Voltage source converter (VSC) Back-to-back AC/DC converters DC link between converters Variable frequency AC on motor/generator side VSC topologies include: Two-level PWM Multi-level PWM Multi-level modular converter (MMC)

System Configurations Electrical/Electrochemical 34 Electrical and electrochemical storage Ultracapacitors, batteries Output from storage device is already in the electrical domain, but it is DC Need AC/DC conversion to interface with the grid AC/DC conversion Charging: AC-to-DC rectification Discharging: DC-to-AC inversion Voltage source converter is a common choice here Independent control of real and reactive power control Allows storage to provide black start capability