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Energy Systems Research Laboratory, FIU Renewable Energy Utilization Professor Osama A. Mohammed Department of Electrical and Computer Engineering EEL5285 & EEL 4930 All Sections (Spring 2018) Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

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Page 1: All Sections (Spring 2018)

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

Page 2: All Sections (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

Page 3: All Sections (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

Page 4: All Sections (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

Page 5: All Sections (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

Page 6: All Sections (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

Page 7: All Sections (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

Page 8: All Sections (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

Page 9: All Sections (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

Page 10: All Sections (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

Page 11: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Example: Daily Variation for CA

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 12: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Example: Weekly Variation

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 13: All Sections (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

Page 14: All Sections (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

Page 15: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Gas Turbine

Source: Masters

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 16: All Sections (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

Page 17: All Sections (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

Page 18: All Sections (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

Page 19: All Sections (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

Page 20: All Sections (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

Page 21: All Sections (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

Page 22: All Sections (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

Page 23: All Sections (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

Page 24: All Sections (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

Page 25: All Sections (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

Page 26: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIUProfessor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Alternate and Renewable Energy Sources

Page 27: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Wind Power Systems

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 28: All Sections (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

Page 29: All Sections (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

Page 30: All Sections (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

Page 31: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Massachusetts Wind Resources

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 32: All Sections (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

Page 33: All Sections (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

Page 34: All Sections (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

Page 35: All Sections (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

Page 36: All Sections (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

Page 37: All Sections (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

Page 38: All Sections (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

Page 39: All Sections (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

Page 40: All Sections (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

Page 41: All Sections (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

Page 42: All Sections (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

Page 43: All Sections (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

Page 44: All Sections (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

Page 45: All Sections (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

Page 46: All Sections (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

Page 47: All Sections (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

Page 48: All Sections (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

Page 49: All Sections (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

Page 50: All Sections (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

Page 51: All Sections (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

Page 52: All Sections (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

Page 53: All Sections (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

Page 54: All Sections (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

Page 55: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Vestas

V80 1.8 MW

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018

Page 56: All Sections (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

Page 57: All Sections (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

Page 58: All Sections (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

Page 59: All Sections (Spring 2018)

Energy Systems Research Laboratory, FIU

Example: GE 2.5 MW Turbines

Professor O. A. Mohammed, EEL5285 Lecture Notes, Spring 2018