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Energy Systems Research Laboratory, FIU
Renewable Energy Utilization
Professor Osama A. Mohammed
Department of Electrical and Computer Engineering
EEL5285 & EEL 4930All Sections (Spring 2018)
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
What is Covered
Part I: Renewable Energy Systems
• Introduction
• Electric Systems in Energy Context
• Basic Review of Electric Quantifies and Impact of Power Conditioning
• Energy Efficiency and operational issues
• Energy Generation and operation and control
• Alternate and Renewable Energy Sources and its Economics– Alternate and Renewable Energy Sources
o Wind Energy
o Distributed generation technologies
o Hydro Power
o Wave/ Tidal Power
o Cooling and Heat Pumps
o The Solar Resource
Part II: Renewable Energy Utilization
• Renewable Energy Utilization
• Energy Storage including Electric/Pluggable Hybrid Cars
• Smart Grid Integration Issues
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Background on the Electric Utility
Industry
• First real practical uses of electricity began with the
telegraph (around the civil war) and then arc lighting in the
1870’s (Broadway, the “Great White Way”).
• Central stations for lighting began with Edison in 1882,
using a dc system (safety was key), but transitioned to ac
within several years. Chicago World’s fair in 1893 was key
demonstration of electricity
• High voltage ac started being used in the 1890’s with the
Niagara power plant transferring electricity to Buffalo; also
30kV line in Germany
• Frequency standardized in the 1930’s
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Regulation and Large Utilities
• Electric usage spread rapidly, particularly in urban areas. Samuel
Insull (originally Edison’s secretary, but later from Chicago)
played a major role in the development of large electric utilities
and their holding companies
– Insull was also instrumental in start of state regulation in 1890’s
• Public Utilities Holding Company Act (PUHCA) of 1935
essentially broke up inter-state holding companies
– This gave rise to electric utilities that only operated in one state
– PUHCA was repealed in 2005
• For most of the last century electric utilities operated as vertical
monopolies
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Vertical Monopolies
• Within a particular geographic market, the
electric utility had an exclusive franchise
Generation
Transmission
Distribution
Customer Service
In return for this exclusive
franchise, the utility had the
obligation to serve all
existing and future customers
at rates determined jointly
by utility and regulators
It was a “cost plus” business
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Vertical Monopolies
• Within its service territory each utility was the only
game in town
• Neighboring utilities functioned more as colleagues
than competitors
• Utilities gradually interconnected their systems so
by 1970 transmission lines crisscrossed North
America, with voltages up to 765 kV
• Economies of scale keep resulted in decreasing
rates, so most every one was happy
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
History, cont’d -- 1970’s
• 1970’s brought inflation, increased fossil-fuel
prices, calls for conservation and growing
environmental concerns
• Increasing rates replaced decreasing ones
• As a result, U.S. Congress passed Public Utilities
Regulator Policies Act (PURPA) in 1978, which
mandated utilities must purchase power from
independent generators located in their service
territory (modified 2005)
• PURPA introduced some competition, but its
implementation varied greatly by state
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power System Structure
• All power systems have three major components:
Load, Generation, and Transmission/Distribution.
• Load: Consumes electric power
• Generation: Creates electric power.
• Transmission/Distribution: Transmits electric
power from generation to load.
• A key constraint is since electricity can’t be
effectively stored, at any moment in time the net
generation must equal the net load plus losses
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
LOADS
• Can range in size from less than one watt to 10’s of
MW
• Loads are usually aggregated for system analysis
• The aggregate load changes with time, with strong
daily, weekly and seasonal cycles
– Load variation is very location dependent
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Loads- Household Consumption
Source: EIA 2008
Annual Energy
Review
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Example: Daily Variation for CA
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Example: Weekly Variation
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
GENERATION
• Large plants predominate, with sizes up to
about 1500 MW.
• Coal is most common source (56%), followed
by nuclear (21%), hydro (10%) and gas
(10%).
• New construction is mostly natural gas, with
economics highly dependent upon the gas
price
• Generated at about 20 kV for large plants
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Basic Gas Turbine Efficiency
Brayton Cycle: Working fluid is
always a gas
Most common fuel is natural gas
Maximum Efficiency
550 2731 42%
1150 273
Typical efficiency is around 30 to 35%
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Gas Turbine
Source: Masters
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Combined Heat and Power
Overall Thermal Efficiency = 33% (Electricity) + 53% (Heat) = 86%
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Combined Cycle Power Plants
Efficiencies of up to 60% can be achieved, with even higher values when the steam is used for heating
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Determining operating costs
• In determining whether to build a plant, both the fixed
costs and the operating (variable) costs need to be
considered.
• Once a plant is build, then the decision of whether or not
to operate the plant depends only upon the variable costs
• Variable costs are often broken down into the fuel costs
and the O&M costs (operations and maintenance)
• Fuel costs are usually specified as a fuel cost, in $/Mbtu,
times the heat rate, in MBtu/MWh
– Heat rate = 3.412 MBtu/MWh/efficiency
– Example, a 33% efficient plant has a heat rate of 10.24
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Heat Rate
• Fuel costs are usually specified as a fuel cost, in
$/Mbtu, times the heat rate, in MBtu/MWh
– Heat rate = 3.412 MBtu/MWh/efficiency
(1 KWh=3.412KBtu)
– Example, a 33% efficient plant has a heat rate of
10.24 Mbtu/MWh
– About 1055 Joules = 1 Btu
– 3600 kJ in a kWh
• The heat rate is an average value that can change as
the output of a power plant varies.
• Do Example 3.5, material balanceProfessor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Historical and Forecasted Heat Rates
http://www.npc.org/Study_Topic_Papers/4-DTG-ElectricEfficiency.pdf
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Fixed Charge Rate (FCR)
• The capital costs for a power plant can be annualized by
multiplying the total amount by a value known as the
fixed charge rate (FCR)
• The FCR accounts for fixed costs such as interest on
loans, returns to investors, fixed operation and
maintenance costs, and taxes.
• The FCR varies with interest rates, and is now below
10%.
• For comparison this value is often expressed as
$/yr-kW
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Annualized Operating Costs
• The operating costs can also be annualized by
including the number of hours a plant is actually
operated
• Assuming full output the value is
Variable ($/yr-kW) =
[Fuel($/Btu) * Heat rate (Btu/kWh) +
O&M($/Kwh)]*(operating hours/hours in year)
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Coal Plant Example
• Assume capital costs of $4 billion for a 1600 MW coal
plant with a FCR of 10% and operation time of 8000 hours
per year. Assume a heat rate of 10 Mbtu/MWh, fuel costs
of 1.5 $/Mbtu, and variable O&M of $4.3/MWh. What is
annualized cost per kWh?
Fixed Cost($/kW) = $4 billion/1.6 million kW=2500 $/kW
Annualized capital cost = $250/kW-yr
Annualized operating cost = (1.5*10+4.3)*8000/1000
= $154.4/kW-yr
Cost = $(250 + 154.4)/kW-yr/(8000h/yr) = $0.051/kWh
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Capacity Factor (CF)
• The term capacity factor (CF) is used to provide a
measure of how much energy a plant actually produces
compared to the amount assuming it ran at rated
capacity for the entire year
CF = Actual yearly energy output/(Rated Power * 8760)
• The CF varies widely between generation technologies,
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Generator Capacity Factors
Source: EIA Electric Power Annual, 2007
The capacity factor for solar is usually less than 25% (sometimes
substantially less), while for wind it is usually between 20 to 40%). A
lower capacity factor means a higher cost per kWh
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIUProfessor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Alternate and Renewable Energy Sources
Energy Systems Research Laboratory, FIU
Wind Power Systems
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Historical Development of Wind Power
• In the US - first wind-electric systems built in the late
1890’s
• By 1930s and 1940s, hundreds of thousands were in
use in rural areas not yet served by the grid
• Interest in wind power declined as the utility grid
expanded and as reliable, inexpensive electricity could
be purchased
• Oil crisis in 1970s created a renewed interest in wind
until US government stopped giving tax credits
• Renewed interest again since the 1990s
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
US Wind Resources
http://www.windpower.org/en/pictures/lacour.htmhttp://www.windpoweringamerica.gov/pdfs/wind_maps/us_windmap.pdf
50 meters
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Cape Wind
off-shore wind farm
• For about 10 years Cape Wind Associates has been attempting to
build an off-shore 170 MW wind farm in Nantucket Sound,
Massachusetts. Because the closest turbine would be more than
three miles from shore (4.8 miles) it is subject to federal, as
opposed to state, jurisdiction.
– Federal approval was given on May 17, 2010
– Cape Wind would be the first US off-shore wind farm
• There has been significant opposition to this project, mostly out
of concern that the wind farm would ruin the views from private
property, decreasing property values.
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Massachusetts Wind Resources
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Cape Wind Simulated View,
Nantucket Sound, 6.5 miles Distant
Source: www.capewind.org
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Types of Wind Turbines
• “Windmill”- used to grind grain into flour
• Many different names - “wind-driven generator”,
“wind generator”, “wind turbine”, “wind-turbine
generator (WTG)”, “wind energy conversion system
(WECS)”
• Can have be horizontal axis wind turbines (HAWT)
or vertical axis wind turbines (VAWT)
• Groups of wind turbines are located in what is
called either a “wind farm” or a “wind park”
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Vertical Axis Wind Turbines
• Darrieus rotor - the only vertical axis
machine with any commercial success
• Wind hitting the vertical blades, called
aerofoils, generates lift to create rotation
http://www.reuk.co.uk/Darrieus-Wind-Turbines.htm
• No yaw (rotation about vertical axis)
control needed to keep them facing into
the wind
• Heavy machinery in the nacelle is located
on the ground
• Blades are closer to ground where
windspeeds are lower
http://www.absoluteastronomy.com/topics/Darrieus_wind_turbineProfessor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Horizontal Axis Wind Turbines
• “Downwind” HAWT – a turbine
with the blades behind (downwind
from) the tower
• No yaw control needed- they
naturally orient themselves in line
with the wind
• Shadowing effect – when a blade
swings behind the tower, the wind it
encounters is briefly reduced and
the blade flexes
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Horizontal Axis Wind Turbines
• “Upwind” HAWT – blades are in
front of (upwind of) the tower
• Most modern wind turbines are
this type
• Blades are “upwind” of the tower
• Require somewhat complex yaw
control to keep them facing into
the wind
• Operate more smoothly and
deliver more power
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Number of Rotating Blades
• Windmills have multiple blades
– need to provide high starting torque to overcome weight
of the pumping rod
– must be able to operate at low wind speeds to provide
nearly continuous water pumping
– a larger area of the rotor faces the wind
• Turbines with many blades operate at much lower rotational
speeds - as the speed increases, the turbulence caused by one
blade impacts the other blades
• Most modern wind turbines have two or three blades
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power in the Wind
• Consider the kinetic energy of a “packet” of air with
mass m moving at velocity v
• Divide by time and get power
• The mass flow rate is (r is air density)
21KE (6.1)
2mv
21 passing though APower through area A (6.2)
2
mv
t
passing though A= = A (6.3)
mm v
t
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power in the Wind
Combining (6.2) and (6.3),
21Power through area A A
2v v
31P A (6.4)
2W v Power in the wind
PW (Watts) = power in the wind
ρ (kg/m3)= air density (1.225kg/m3 at 15˚C and 1 atm)
A (m2)= the cross-sectional area that wind passes through
v (m/s)= windspeed normal to A (1 m/s = 2.237 mph)
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power in the Wind (for reference solar is
about 600 w/m2 in summer)
• Power increases like the
cube of wind speed
• Doubling the wind
speed increases the
power by eight
• Energy in 1 hour of 20
mph winds is the same
as energy in 8 hours of
10 mph winds
• Nonlinear, so we cannot
use average wind speedFigure 6.5
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power in the Wind
• Power in the wind is also proportional to A
• For a conventional HAWT, A = (π/4)D2, so wind
power is proportional to the blade diameter squared
• Cost is roughly proportional to blade diameter
• This explains why larger wind turbines are more
cost effective
31P A (6.4)
2W v
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Nikola Tesla: Inventor of Induction
Motor (and many other things)
• Nikola Tesla (1856 to 1943) is one of the key inventors associated with the development of today’s three phase ac system. His contributions include the induction motor and polyphase ac systems.– Unit of flux density is named after him
• Tesla conceived of the induction
motor while walking through a park in
Budapest in 1882.
• He emigrated to the US in 1884
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
World’s Largest Offshore Wind Farm Opens
• “Thanet” located off British coast in English Channel
• 100 Vestas V90 turbines, 300 MW capacity
http://edition.cnn.com/2010/WORLD/europe/09/23/uk.largest.wind.farm/?hpt=Sbinhttp://www.vattenfall.co.uk/en/thanet-offshore-wind-farm.htm
Turbines
are
located
in water
depth
of
20-25m.
Rows
are
800m
apart; 500m
between
turbines
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Off-shore Wind
• Offshore wind turbines currently need to be in
relatively shallow water, so maximum distance from
shore depends on the seabed
• Capacity
factors tend
to increase
as turbines
move further
off-shore
Image Source: National Renewable Energy Laboratory
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Maximum Rotor Efficiency
Figure 6.10
Rotor efficiency CP vs.
wind speed ratio λ
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Tip-Speed Ratio (TSR)
• Efficiency is a function of how fast the rotor turns
• Tip-Speed Ratio (TSR) is the speed of the outer tip
of the blade divided by wind speed
Rotor tip speed rpm DTip-Speed-Ratio (TSR) = (6.27)
Wind speed 60v
• D = rotor diameter (m)
• v = upwind undisturbed windspeed (m/s)
• rpm = rotor speed, (revolutions/min)
• One meter per second = 2.24 miles per hour
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Tip-Speed Ratio (TSR)
• TSR for various
rotor types
• Rotors with fewer
blades reach their
maximum
efficiency at higher
tip-speed ratios
Figure 6.11
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Synchronous Machines
• Spin at a rotational speed determined by the number
of poles and by the frequency
• The magnetic field is created on their rotors
• Create the magnetic field by running DC through
windings around the core
• A gear box is needed between the blades and the
generator
• 2 complications – need to provide DC, need to have
slip rings on the rotor shaft and brushes
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Asynchronous Induction Machines
• Do not turn at a fixed speed
• Acts as a motor during start up as well as a
generator
• Do not require exciter, brushes, and slip rings
• The magnetic field is created on the stator
instead of the rotor
• Less expensive, require less maintenance
• Most wind turbines are induction machines
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
The Induction Machine as a Generator
• Slip is negative because the rotor spins faster
than synchronous speed
• Slip is normally less than 1% for grid-
connected generator
• Typical rotor speed
(1 ) [1 ( 0.01)] 3600 3636 rpmR SN s N
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Speed Control
• Necessary to be able to shed wind in high-speed
winds
• Rotor efficiency changes for different Tip-Speed
Ratios (TSR), and TSR is a function of windspeed
• To maintain a constant TSR, blade speed should
change as windspeed changes
• A challenge is to design machines that can
accommodate variable rotor speed and fixed
generator speed
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Blade Efficiency vs. Windspeed
Figure 6.19
At lower windspeeds, the best efficiency is achieved at a lower rotational speed
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Power Delivered vs. Windspeed
Figure 6.20
Impact of rotational speed adjustment on delivered power, assuming gear and generator
efficiency is 70%
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Variable Slip Example: Vestas
V80, 1.8 MW
• The Vestas V80, 1.8 MW turbine is
an example in which an induction
generator is operated with variable
rotor resistance (opti-slip).
• Adjusting the rotor resistance
changes the torque-speed curve
• Operates between 9 and 19 rpm
Source: Vestas V80 brochure
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Vestas
V80 1.8 MW
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Doubly-Fed Induction Generators
• Another common approach is to use what is
called a doubly-fed induction generator in which
there is an electrical connection between the
rotor and supply electrical system using an ac-ac
converter
• This allows operation over a wide-range of
speed, for example 30% with the GE 1.5 MW
and 3.6 MW machines
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
GE 1.5 MW and 3.6 MW
DFIG Examples
Source: GE Brochure/manual
GE 1.5 MW turbines are the
best selling wind turbines
in the US with 43% market share in 2008
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Indirect Grid Connection Systems
• Wind turbine is allowed to spin at any speed
• Variable frequency AC from the generator goes
through a rectifier (AC-DC) and an inverter (DC-
AC) to 60 Hz for grid-connection
• Good for handling rapidly changing wind speeds
Figure 6.21
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018
Energy Systems Research Laboratory, FIU
Example: GE 2.5 MW Turbines
Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018