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Status: [7th Sept] solid draft

ELECTRICITY STORAGE

Introduction

IF mass storage of electrical energy were easy and cheap, then the problem of integrating large-scale renewables into the energy sector would be greatly simplified. The variability of supply could simply be buffered in storage and drawn down as needed to meet demand.

This page has two purposes: the primarily OzEA project -- of modelling electrical supply meeting demand in a system with high renewable penetration -- requires specification of the system storage capabilities, and this page provides the background discussion on this specific point. This page is also a place for exploring more generally the possibilities for large scale and economically feasible storage in electricity systems looking into the medium term.

The short answer is that Hydro Electricity is the only mass electricity storage that we have available. Other possibilities, including thermal storage within concentrated solar thermal plants, may develop but remain speculative at this time.

Storage and Demand Management

Conceptually 'Storage' has two halves; the first half is the sinking of electricity into a storage medium, and the second is 'on demand' availability of electricity from the storage medium. It is usual to think of Electricity Storage as encompassing both of these halves in a single mechanism or process, however, processes that achieve either can be relevant here.

For example, hydro electricity (as distinct from Pumped Storage Hydro) stores energy in the form of water from rain contained in a dam at a height: this is storage of energy that is available as electricity on demand, but does not take electricity to 'charge'. Conversely, the use of plentiful electricity to displace the use of gas (in a furnace or some other heating process) productively uses that electricity, but not in a way that makes it available for future use. Compressed air storage for use with gas turbines (as below) is a similar displacing mechanism. In short, sometimes the need is to 'put' electricity somewhere useful; sometimes the need is to 'get' extra electricity in order to balance supply against demand.

The further one delves into variations on the basic concept of storage, the more the term Demand Management becomes applicable. We make no hard distinction here, but do develop these areas as separate discussions.

Pumped Storage Hydro

Pumped Storage Electricity is when water is pumped from a lower dam into a higher dam to 'charge' a hydro system where the water otherwise runs downhill through turbines to generate electricity. As a rule of thumb this process gives back around 80% of the electricity put in.

Australia currently has around 20 GWh of pumped storage hydro capacity, principally associated with the Tumut 3 System as part of the Snowy Mountains Scheme, and also the Wivenhoe - Splityard Creek system near Brisbane. So far as OzEA is aware there are no serious proposals to build further large PSH capacity in Australia.

Straight Hydro

There are, however, tens of thousands of GWh of straight Hydro power in Australia when the dams are full, and the various Hydro facilities can collectively provide around 7 GW of power supply. The total capacity (perhaps in excess of 30,000 GWh) is not an especially useful number; what matters is the total amount of power that can be reliably drawn from these resources year after year, which in turn would involve an analysis of long-term rainfall patterns. As an expedient we consider the amount of currently used Hydro power that can be displaced by other sources (predominately Wind), and take such displacement as 'storage' for the purposes of OzEA analysis. Work to provide an estimate of this 'storage' is pending, however it is noteworthy that Tasmania uses significant amounts of Hydro power.

Compressed Air Energy Storage (CAES)

Energy can be stored in the form of a compressed gas, however, there are some complexities to appreciate here. Like hydro power, compressed air energy storage can IN PRINCIPLE approach 100% efficiency; however, unlike hydro power it is problematic in practice to achieve high efficiencies. Pumping water (an essentially incompressible fluid) up a hill incurs frictional losses in the pipes, and any losses associated with the engineering realities of the turbines. With a compressible fluid (i.e. a gas) the process is more complex - and we briefly outline the physics in a non-mathematical way.

Physically, the temperature of a gas is related to the (square of the) average velocity of the individual gas molecules. The act of compressing a gas tends to involve hitting the molecules 'up the pipe', and thus the molecules themselves obtain higher velocities resulting in the gas overall obtaining an increased temperature -- in addition to an increased pressure. It is this increase in temperature that is wasteful because the heated gas, like a cup of coffee, tends to return to the temperature of the surrounding environment by dissipating low grade waste heat. In this way the pressure of the gas once it has settled (cooled) in storage is less than the pressure at the time of compression. These losses can be reduced by being as gentle as possible with the gas in the compression process (as slowly as possible, and in a staged manner). Thus, a trade-off exists between efficiency on the one hand, and the engineering complexity and cost on the other.

[fc - Aug 2010] I'm struggling to get the physics of the decompression straight in my head, possibly because I'm thinking in terms of ideal rather than real gases. Am fairly sure that there is "adiabatic cooling" of the gas as pressure is released, thus creating further losses. The point does not bear further time on clarification at this stage, although I'd be grateful if anyone can give a tidy wrap up.

One particular implementation of CAES is to use it in combination with Generating Gas Turbines (and this combination is sometimes what is meant by "CAES"). Gas turbines pre-compress the air-fuel mixture (and use perhaps 40% of the energy generated to do this), but with a source of compressed air at a suitable pressure this parasitic load on the turbines can be removed. In this way electricity can be usefully stored; however, and so far as we understand, there is no extra power from the gas turbine - just a reduction in the gas needed to power it.

Vessels for storing usefully large amounts of compressed air present a particular difficulty, usually requiring a convenient underground cavern such as an abandoned mine. It could also be possible to use 'large underwater balloons' for compressed air storage, where at a depth of around 600m the necessary pressure is provided by the water column rather than the strength of the container. Such proposals are very much at the research end of the development spectrum.

High Temperature Thermal Storage

The concentrated rays from a Solar Thermal plant are converted into heat when they are absorbed by the medium at the focal point, and this heat drives a steam turbine or similar heat engine to produce electricity. These two steps can be separated by storing the heat in a suitable medium (e.g. molten salts, large graphite blocks) that is suitably stored / insulated. In this way solar thermal plants can generate electricity into the evening. The length of time that heat can be usefully stored in this way is an economic as much as an engineering problem.

Note that it would be a particularly inefficient storage mechanism to use electricity to generate heat for later use to generate electricity. The reason is that extracting useful work from heat is a fundamentally inefficient process (as per the Carnot Limit), depending strongly on how high the temperature is.

Hydrogen and other Chemical Transformations

It is not difficult to 'make' hydrogen from water and electricity. It is somewhat more complicated to capture and store large amounts of hydrogen. Using hydrogen in a Fuel Cell to generate electricity is efficient but requires expensive platinum catalyst. Burning hydrogen is an easier but much less efficient way of recovering some of the electricity invested. To the best of our knowledge the use of hydrogen for large-scale energy storage remains at a research level.

In addition to Hydrogen there are many ways of storing electrical energy as chemical energy. While this topic is doubtless deserving of more exploration than given here, OzEA is not currently aware of any chemical storage mechanism or proposal that is likely to provide significant storage capacity in the Australian electricity market any time soon. Please let us know of any proposals or technologies that might reasonably be part of the medium term development of the energy sector.

Overall

Storage of electrical energy can take many forms, but the provision of inexpensive and large-scale electricity storage appears for now to be limited to hydro-electricity. In particular this includes the currently existing 20 GWh of Pumped Storage Hydro, and the displacement of hydro power that is currently used for Tasmanian baseload (this latter amount being on 'The List' for calculation). The use of these resources in OzEA models of electricity supply will require attention to the locations and capacities of the individual components.

Beyond these Hydro resources, the potential for the development of further storage capacity within the Australian Electricity System remains opaque. We can only give focus to storage mechanisms that have serious potential to be large scale and low cost in the next decade or so. However, this page is open to general discussion and the sharing of details in relation to all sorts of storage technologies or possibilities.


DISCUSSION: (on storage and its place in a grid with a high penetration of renewables)

2

OzEA_TSELE0002

Neil Howes
Subject: storage of hydro
Date: 2010-05-21 (at 12:21:37)


TAS hydro gives a value of 16,000GWh (about 2 years annual production) if dams are all full.
Lake Eucumbene has a storage capacity of 4,200,000ML (>10,0.00GWh) if full. The limitation is the rate of release (2.2GW in TAS and 2.5GW in Snowy), limiting to 100GWh/day.

4

OzEA_TSELE0004

Stephen Gloor (Ender)
Subject: Solar Thermal Storage
Date: 2010-06-03 (at 17:51:09)


CSP plants that are being constructed and are operating now incorporate storage as part of the design.

Solar Reserve (http://www.solar-reserve.com/) for instance uses the molten salts used for storage as a working fluid so there is no real storage overhead other than oversize collectors.

As far as I can see there is no reason why the salts cannot be heated by surplus wind power. That is either by an efficient electric heater being incorporated in the design so the salts can be heated by electricity from surplus wind or an agreement between the wind farm and the CSP plant that when there is surplus wind the solar plant shuts down its electricity output and only stores energy in the salt. The wind farm operator could basically pay the CSP plant operator not to generate power as a way of storing wind. The wind farm operator would then have x amount of megawatts in the store for use when it needs it for balancing its output. Or if the CSP plant really needed it, it could buy if off the wind farm operators.

fc, 7th Sept: good points. Have now included a section on Thermal Storage

5

OzEA_TSELE0005

Neil Howes
Subject: pumped hydro storage rules
Date: 2010-07-14 (at 10:13:44)


Francis,
After discussing with you and thinking more about the way to make full use of existing hydro storage the following rules could be applied.
This is assuming only 50GWh storage, 5GW wind capacity, pipe 2GW to storage(but other connections from storage to NEM grid), and natural gas capacity 2GW.
My thinking is that 5GW of hydro is used mainly during daytime peak demand(8h/day)and virtually none during off-peak periods(16h/day). Thus excess wind in SA during the daytime(up to pipe capacity) doesnt have to be stored because hydro is being used during this period. Conversely during off-peak periods excess wind cannot save hydro and must be stored by pumped hydro or load shed.
Looking at the last 10 months of NEM wind/ demand summary, 46/302 days
wind output was >50% capacity but in 25 events was 20-24h, 7events for <48h and only one event 3days and one event4 days. Thus if can store surplus wind (50-70% capacity) for 24h will be capturing most of high wind output(34 days) and only load shed for 12days(out of 10 months). The GWh production at av 60% capacity will be 3GW or 72GWh/24h period. If 16GW is used by NEM to replace some hydro, during the other 16h off-peak would store 32GWh using pumped hydro, thus up to 48GWh is stored( or banked) and 36GWh used by SA demand for a total of 84GWh out of a potential capacity of 120GWh(70%capacity). On the following daytime peak another 16GWh will be used to bank hydro but only 4GWh could be stored overnight by pumped hydro, so together with 36GWh demand, would use 56GWh/120GWh potential (47% capacity) with 16GWh load shed(72GWh-56GWh). High wind events longer than 48h are very rare(5 days total/10months) so can ignore additional load shedding for those events. Thus 36GWh storage is being used, with 14GWh being kept in reserve for daytime peak above 2GW possible from NG back-up.
The rules would be:

(1) Excess wind brings up peak demand storage to 14GWh during peak demand then during peak replaces up to 16GW hydro(used by NEM). If no hydro is being used, fills up storage then load shed excess.
(2) Excess wind during off peak (16h/day) is stored (up to 32GWh/day) until upper storage is full then load shed. Maximum of 1000MW ( off-peak demand) is used.
(3) Any wind deficit uses upper storage during peak periods (8h/day) up to 2GW(16GWh/day) until all upper is used, then draws on 14GWh reserve and balance using NG up to 2GW. Reserve 14GWh topped up overnight by hydro to provide peak reserve.
(4) Any wind deficit during off-peak uses upper storage(36GWh), then hydro until credits(NEM) are used then with NG at 1 GW until restore lower to 14GWh reserve(14h of NG).

6

OzEA_TSELE0006

Peter Seligman
Subject: Seawater pumped storage
Date: 2011-02-03 (at 18:09:59)


I haven't noticed any reference here to electricity storage using pumped seawater. Such a plant has been operating in Yanbaru, Okinawa, Japan for 12 years. I have put together a plan utilising this idea in Sustainable Energy - by the numbers, published by the Melbourne Energy Institute on http://www.energy.unimelb.edu.au/

Independently a detailed plan based on pumped seawater is described on Nation Builder
http://www.nationbuilder.com.au/assets/States/SA/Default.html

Re Stephen Gloor's comment - using salts to store surplus wind power. Hydro is far more efficient than electrically heating salts because going from elec to heat back to elec is at best 30% efficient, unless a heat pump is used.

That idea is being investigated by a company called Isentropic.

7

OzEA_TSELE0007

Philip Wong
Subject: Large scale and efficient energy storage/transmission
Date: 2012-02-09 (at 18:47:09)


[fc: The form is impressive, but the total lack of background physics etc makes it impossible to take this seriously.]



I am not an expert in this area, I merely have a BE (Electrical engineering) and BSc (Mathematics and Computer Science) from the University of NSW. I came across Evacuated Tube Transport in December 2011. It made quite extraordinary claims about its merit. I did some computer modeling for different scenarios to check his claims and found them to be accurate. I thought it would be a hard sell to convince people to travel in such a system. Then I thought what if it is used to store energy instead, after some calculations I realised that it is also good for transmission. Then I realised it is also good for freight transport.

I have modeled an efficient large scale energy storage/transmission system. It is more efficient and lower cost then pumped hydroelectric or compressed air. The calculations are published at http://www.ioserver.com/etes.html . It allows you to perform optimization, sensitivity analysis and shows the results graphically.

One of the barrier to the use of renewable energy (solar and wind) is their intermittency. As more renewable sources of energy comes online, it become more difficult to balance between production and consumption. In Inner Mongolia, wind farm operators have to turn off ("abandon the wind") their turbines during winter nights because of the lack of demand during those times, having to discard 36GWh of electricity every night. Storage will also reduce the necessity to have excess underutilized generation capacity to handle peak loads. Renewable sources of energy are usually located far away from where there are needed.

This kinetic energy system stores energy in slugs maintained at high speed inside a loop of evacuated tube. In the constant mass version, energy is injected by increasing the speed of the slugs and energy is extracted by decreasing the speed of the slugs, energy can be injected and extracted at any point in the tube. This version can also serve as a power transmission network. In the constant speed version, energy is injected by adding slugs and extracted by removing slugs at a central station. Both versions can also be used to transport freight that can withstand high G forces.

The capital cost $/kW/km is inversely proportional to the square root of the kW or kWh of energy storage required. Efficiency increases as the size of the storage required is increased. For HVDC the conductor cost $/kW/km is proportional to the distance and the ohmic loss is proportional to the MW carried. This system is suitable for energy and power applications that requires more than 5 GWh of storage. This system have much bigger MW carrying capacity than overhead lines and cheaper than underground lines.

In conjunction with electrification of transport (see http://www.ioserver.com/et3.htm), this technology will allow most the energy requirements of transport, energy and heat to be sourced from renewables.

Please email ioserver@supernerd.com.au if you find any mistakes or have better data.

8

OzEA_TSELE0008

Philip Wong
Subject: backgroung physics
Date: 2012-02-09 (at 21:44:59)


Please use "view source" to see the javascript for all the calculations. I tried to calculate everything from first principle. e.g you see the following code.
var GravityConstant = 6.67384e-11;
var EarthMass = 5.9742e24;
var EarthRadius = 6378.1e3;
var Gravity = GravityConstant * EarthMass / (EarthRadius * EarthRadius);

Is uses high schools physics and maths for calculating the radius, length, diameter, area, volume, mass, velocity, acceleration, jerk, air resistance, rolling resistance, centrifugal force, watts, temperature, air density, air pressure, specific heat of steel, density of steel, sin, cos and etc.,

There are some areas that I am not so certain, eg. calculating the thickness of the steel tube to withstand atmospheric pressure and water pressure for a given diameter. I need a mechanical engineer that understand how to apply the ASME code for pressure piping for more accurate numbers.

Another area that I am not so sure about is how to calculate the combined effect of gravity, centrifugal force due to the loop radius, centrifugal force due to earth radius on the magnetic force required to levitate the slug. Most calculation ignore the centrifugal forces and assume a straight path.

The costing for the magnets and YBCO bulk crystals comes from a chinese supplier.

I know it looks complicated at first, but it is really very simple.

e.g the mass of the tube is calculated as
TubeMass = PI * (TubeDiameter * TubeThickness + TubeThickness * TubeThickness) * 7850 * TubeLength;
Where PI = 3.14159
TubeDiameter is the inner diameter of the tube in meters
TubeThickness is the thickness of the tube in meters
TubeLength is the length of the tube in meters
7850 is the density of steel in kg/m^3

e.g the time it takes for a slug to go around a loop
SlugLoopTime = TubeLength / SlugVelocity;
SlugLoopTime is the time in seconds
TubeLength is the length of the tube in meters
SlugVelocity is the velocity of the slug in m/s

The calculation are done in a certain way to allow sensitivity analyses and optimisation to be performed. e.g What is the effect of tube diameter to energy loss/efficiency? What is the effect of slug loading on the tube on the total cost? What is the effect of inter slug spacing and slug length affects efficiency.

9

OzEA_TSELE0009

Philip Wong
Subject: Background Physics
Date: 2012-02-11 (at 07:48:04)


Slugs = Math.ceil(2 * Math.sqrt(EnergyMWh * 3.6e9 * PI / (SlugCForce * Gravity * SlugMass * (SlugLength + SlugSpacing))));

The above line in the code is non-obvious and needs explanation

Here is the derivation:

V * V = 2 * E / Mass
Radius = Length / (2 * PI)
G = V * V / Radius = 2 * E / (Mass * Radius)
Mass = Slugs * SlugMass
Length = Slugs * (SlugLength * SlugSpacing)
Mass * Radius = 2 * E / G
Mass * Length = 4 * E * PI / G
Slugs * Slugs * SlugMass * (SlugLength + SlugSpacing) = 4 * E * PI / G
Slugs = 2 * sqrt(E * PI / (G * SlugMass * (SlugLength + SlugSpacing))
G = SlugCForce * Gravity

Where
V is the velocity of the slugs in m/s
E is the kinetic energy in joules
Mass is the total mass of all the slugs in kg
Radius is the radius of the loop in meters
Length is the total of the loop in meters
G is the centrifugal force on the slugs in m/s^s
PI is the value of Pi 3.14159
Gravity is earth gravity 9.8 m/s^s
Slugs is the total number of slugs
SlugMass is the weight of each slug in kg
SlugLength is the length of each slug in meters
SlugSpacing is the distance between each slugs in meters
SlugCForce is the maximum allowable centrifugal force on each slug
EnergyMWh is the kinetic energy that is required to be stored in MWh

If you see anything that is non-obvious, please ask. To me it obvious, but it may be the mistake that I am trying to look for. I am seeking help and critique from experts and people much more intelligent than me to check my calculations. Especially from those that can derive the above by themselves.

I apologise for my poor English.

Maybe I have come to wrong forum to seek help, serious debate and analysis on problems in energy.

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fc - August 2010