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Week 3- Renewable Energy Fundamentals and System Components

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Renewable Generation and Conversion
B31GC
Renewable Energy Fundamentals
Learning Objectives
This session
• We will review key system components for
renewable energy applications
• We will understand the fundamental working
principle of different generator types
• We will understand the operating principles of
different power converter types
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Principles of electromagnetism
Some basics
Complex impedance
General
Resistor
๐‘ฃาง = ๐‘.าง ๐‘– าง
Sinusoidal form
๐‘  ๐‘ก = ๐ด0 ๐‘๐‘œ๐‘ (2๐œ‹๐‘“๐‘ก + ๐œ‘แˆป
๐‘ฃ ๐‘ก = ๐‘…. ๐‘– ๐‘ก = ๐‘…. ๐ผ๐‘๐‘œ๐‘ (๐œ”๐‘ก + ๐œ‘แˆป
๐‘ฃาง = ๐‘…๐ผ๐‘’ ๐‘—๐œ‘
We choose:
๐‘– ๐‘ก =๐‘—๐œ‘๐ผ๐‘๐‘œ๐‘ (๐œ”๐‘ก + ๐œ‘แˆป
Phasor
๐‘๐‘… = ๐‘…
๐‘– าง = ๐ผ๐‘’
๐‘ าง = ๐ด๐‘Ÿ๐‘š๐‘  ∠๐œ‘
or ๐‘ าง = ๐ด0 ∠๐œ‘
Inductance
Capacitance
1
1
๐œ‹
เถฑ๐‘– ๐‘ก ๐‘‘๐‘ก =
๐ผ๐‘๐‘œ๐‘  ๐œ”๐‘ก + ๐œ‘ −
๐ถ
๐ถ๐œ”
2
1
1
๐‘๐‘ = −๐‘—
๐‘ฃาง = −๐‘—
๐‘–าง
๐ถ๐œ”
๐ถ๐œ”
๐‘ฃ ๐‘ก =
๐‘ฃาง = ๐ฟ๐œ”๐ผ๐‘’
๐ด๐‘Ÿ๐‘š๐‘  =
๐ด0
2
=
1 ๐‘‡
เถฑ ๐‘ (๐‘กแˆป2 ๐‘‘๐‘ก
๐‘‡ 0
๐œ‹
๐‘—(๐œ‘+ แ‰
2
= ๐‘—๐ฟ๐œ”๐‘– าง
๐‘๐ฟ = ๐‘—๐ฟ๐œ”
4
Laws
Electric and
magnetic circuits
Ohm’s law
๐‘ฃ ๐‘ก =๐‘– ๐‘ก ๐‘…
Impedance
๐‘—
๐‘ฃ ๐‘ก = ๐‘– ๐‘ก (๐‘… + ๐‘—๐‘ค๐ฟ −
แˆป
๐‘ค๐ถ
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Laws
Electric and
magnetic circuits
๐‘š๐‘š๐‘“ = ๐œ™. ๐‘†๐‘…
๐‘š๐‘š๐‘“ = ๐œ™. ℜ
= ๐œ™ ℜ1 + ℜ2 + 2ℜ3
๐‘™1
๐‘™2
๐‘™3
= ๐œ™(
+
+2โˆ™
แˆป
๐ด๐œ‡๐น๐‘’ ๐ด๐œ‡๐น๐‘’
๐ด๐œ‡๐ด๐‘–๐‘Ÿ
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Laws
Electric and
magnetic circuits
Ni = mmf = ๐œ™ โˆ™ ℜ
๐‘™1
๐‘™2
๐‘™3
= ๐œ™(
+
+2โˆ™
แˆป
๐ด๐œ‡๐น๐‘’ ๐ด๐œ‡๐น๐‘’
๐ด๐œ‡๐ด๐‘–๐‘Ÿ
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Michael
Faraday was
born in
England in
1791
Faraday’s law
Electric and
magnetic circuits
Faraday’s Law:“When the magnetic flux linking a
circuit is varied, an emf is induced in the
circuit”
emf = −
๐‘‘๐œ™
๐‘‘๐‘ก
Lenz’s law:“The direction of an induced emf is
always such that it tends to set up
current opposing the change of the
flux”
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Emil Lenz was
born in the
Russian
Empire in
1804
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Generator effect
Motor and
generator effect
• Applied magnetic field
• Applied motion
• Resultant electric current
๐น = ๐ต๐‘–๐‘™
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Motor effect
Motor and
generator effect
• Applied magnetic field
• Applied electric current
• Resultant motion
๐น = ๐ต๐‘–๐‘™
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Motor and
generator effect
๐‘‘๐œ™
๐‘’๐‘š๐‘“ = −๐‘
๐‘‘๐‘ก
= −๐‘๐œ”๐œ™๐‘š ๐‘๐‘œ๐‘ ๐œ”๐‘ก
๐‘‘๐‘–
๐‘‰ = −๐ฟ
๐‘‘๐‘ก
๐‘‘๐œ™
๐ฟ=๐‘
๐‘‘๐‘–
For a linear magnetic circuit: −๐ฟ =
๐‘๐œ™
๐‘–
Inductance = number of flux linkage per
unit current
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Power generation and
transmission
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Advantages
AC power generation
DC
Resistive losses
Materials used
AC
Transformer
3 phase AC
Deliver more power per cabling
Constant power
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AC transmission
High voltage transmission
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AC transmission
Equivalent circuit per-phase diagram
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AC transmission
Single line per-phase diagram
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High voltage
transmission
The ideal transformer
(IT) -> operation
Transformer ratio: α=
๐‘‰1
๐‘‰2
๐ผ
Power in = Power out
๐‘
= ๐ผ2 = ๐‘1
1
2
Windings have no resistance
Core of transformer has infinite
permeability:
• It takes zero mmf to create flux
• All flux is confined to the core
Transformer core lacks losses: no
hysteresis or eddy currents
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Open circuit or no-load test
Real transformers
- Core losses (magnetising current
losses) Rc and Xm
• Hysteresis (non-linear magnetic
effects in core)
• Eddy current losses (Joule heating
of the core)
Measured: V1,I1,P1,V2
Calculated: Rc=V12/P1 , Xm=V12/Q1
Short-circuit or full-load test
- Windings’ losses R1, X1 and R2, X2
Measured: V1,I1,P1 Calculated: R1eq= P1 /I12 , Z1eq= V1 /I1 , Z1eq= Q1 / I12
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Synchronous generators
Single-phase
synchronous generators
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Single-phase synchronous generators
60๐‘“ 60๐œ”
๐‘๐‘  =
=
๐‘
๐‘2๐œ‹
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Single-phase synchronous generators
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Single-phase synchronous generators
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Single-phase synchronous generators
I๐‘š๐‘๐‘’๐‘‘๐‘Ž๐‘›๐‘๐‘’ โˆถ ๐‘ = ๐‘… + ๐‘—๐‘‹
Complex number
Not a phasor as it does not change with time
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Phasor notation and diagrams
Single-phase synchronous generators
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Single-phase
synchronous
generator
Find Ea, rms, pf and power
delivered to load
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Single-phase
synchronous
generator
Find Ea, rms, pf and power
delivered to load
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Single-phase synchronous generators
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Three-phase synchronous generators
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Three-phase synchronous generators
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Three-phase synchronous generators
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Three-phase synchronous generators
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Three-phase synchronous generators
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Connecting threephase systems
1.
Y (wye)
2.
D (Delta)
3.
Conversion from D to Y
Y connection
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Connecting threephase systems
1.
Y (wye)
2.
D (Delta)
3.
Conversion from D to Y
Y connection
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Connecting threephase systems
1.
Y (wye)
2.
D (Delta)
3.
Conversion from D to Y
Y with neutral connection
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Connecting threephase systems
1.
Y (wye)
2.
D (Delta)
3.
Conversion from D to Y
Δ connection
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Connecting threephase systems
Za
1.
Y (wye)
2.
D (Delta)
3.
Conversion from D to Y
Zb
Zc
• For balanced wye-connected load:
• For balanced delta-connected load
• Conversion
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Break
Induction generators
The induction machine
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The stator
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The stator
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The stator
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The rotor
Squirrel Cage
Wound rotor
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The rotor
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Synchronous speed
Machine operation
60๐‘“ 60๐œ” 120๐‘“
๐‘๐‘  =
=
=
๐‘
๐‘2๐œ‹
๐‘ƒ
๐œ”
๐œ”๐‘  =
๐‘
p = pair poles
P = number of poles
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e.g. 60 ×
50
1
= 3000๐‘Ÿ๐‘๐‘š
50
60 ×
= 1500 ๐‘Ÿ๐‘๐‘š
2
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Induced current
Machine operation
Fleming’s right-hand rule
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Induced motion
Machine operation
Fleming’s left-hand rule
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Slip (fractional
slip
Machine operation
๐‘†=
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๐‘๐‘  − ๐‘๐‘Ÿ ๐œ”๐‘  − ๐œ”๐‘Ÿ
=
๐‘๐‘ 
๐œ”๐‘ 
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Equivalent circuits
52
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Machine operation
Power to stator Pi
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is2Rs loss
Pg = Tωs
ir2Rr loss
Pm = Tωr
Windage loss
P0 = T0ω0
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Core loss
Frictional loss
53
Mechanical power
as a function slip
Machine operation
๐‘ƒ๐‘š = ๐‘ƒ๐‘” − 3๐ผ๐‘Ÿ2 ๐‘…๐‘Ÿ = ๐‘ƒ๐‘” − ๐‘ƒ๐‘Ÿ
๐‘‡๐œ”๐‘Ÿ = ๐‘‡๐œ”๐‘  − ๐‘ƒ๐‘Ÿ
๐‘ƒ๐‘Ÿ = ๐‘‡ ๐œ”๐‘  − ๐œ”๐‘Ÿ = ๐‘‡๐œ”๐‘  ๐‘ 
๐‘ =
๐‘ƒ๐‘Ÿ
๐‘ƒ๐‘Ÿ
=
๐‘‡๐œ”๐‘  ๐‘ƒ๐‘”
3๐ผ๐‘Ÿ2 ๐‘…๐‘Ÿ
๐‘ƒ๐‘š = ๐‘ƒ๐‘” − ๐‘ƒ๐‘Ÿ = ๐‘ƒ๐‘” 1 − ๐‘  =
(1 − ๐‘ แˆป
๐‘ 
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Machine operation
Load
1−๐‘ 
(
แˆป๐‘…๐‘Ÿ
๐‘ 
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Machine operation
1−๐‘ 
๐‘…๐‘Ÿ
๐‘ 
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Machine operation
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๐‘…๐‘Ÿ′
๐‘ = ๐‘…๐‘  +
+ ๐‘—(๐‘‹๐‘  + ๐‘‹๐‘Ÿ′ แˆป
๐‘ 
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Machine operation
๐ผ๐‘Ÿ′2 ๐‘…๐‘Ÿ′ ๐‘
๐‘‡=
๐‘  ๐œ”
๐‘‰
๐‘…๐‘  + ๐‘…๐‘Ÿ′
=๐‘=
+ ๐‘—(๐‘‹๐‘  + ๐‘‹๐‘Ÿ′ แˆป
๐ผ′
๐‘ 
3๐‘
๐‘‰2
๐‘…๐‘Ÿ′
๐‘‡=
(
แˆป
′
๐œ” ๐‘…๐‘  + ๐‘…๐‘Ÿ 2
๐‘ 
(
แˆป + (๐‘‹๐‘  + ๐‘‹๐‘Ÿ′ แˆป2
๐‘ 
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Machine operation
3๐‘
๐‘ฃ2
๐‘‡๐‘š =
(
แˆป
2๐œ” ๐‘…๐‘  + ๐‘…๐‘ 2 + (๐‘‹๐‘  + ๐‘‹๐‘Ÿ′ แˆป2
๐‘†๐‘š =
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๐‘…๐‘Ÿ′
๐‘…๐‘ 2 + ( ๐‘‹๐‘  + ๐‘‹๐‘Ÿ′ แˆป2
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Machine operation
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Power electronics
Converters
Semiconductor devices
1. Rectifiers (AC to DC)
2. Choppers (DC to DC)
3. Inverters (DC to AC)
4. Cyclo-converters (AC to AC)
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Rectifier
Converters
3-phase full-wave rectifier with
diodes
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Rectifier
Converters
For 30o:
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Rectifier
Average output voltage
๐‘‰๐ท๐ถ
+๐œ‹
6
1
= ๐œ‹เถฑ
−๐œ‹
3 6
3 2๐‘‰๐ฟ cos(๐‘ค๐‘กแˆป
+๐œ‹
6
3 6๐‘‰๐ฟ
=
เถฑ cos(๐‘ค๐‘กแˆป
−๐œ‹
๐œ‹
6
3 6
=
๐‘‰ = 2.34๐‘‰๐ฟ
๐œ‹ ๐ฟ
๐‘‰๐‘๐‘’๐‘Ž๐‘˜ = 2๐‘‰๐‘Ÿ๐‘š๐‘ 
๐‘‰๐‘™๐‘–๐‘›๐‘’−๐‘ก๐‘œ−๐‘™๐‘–๐‘›๐‘’ = 3๐‘‰๐‘™๐‘–๐‘›๐‘’−๐‘ก๐‘œ−๐‘›๐‘’๐‘ข๐‘ก๐‘Ÿ๐‘Ž๐‘™
๐‘‰๐ฟ๐ผ๐‘๐ธ = 3๐‘‰๐‘ƒ๐ป๐ด๐‘†๐ธ
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Rectifier
Converters
• Fully-controlled 3-phase bridge
rectifier – replacing diodes with
thyristors
• Control of voltage level
3 3 2
๐‘‰๐ท๐ถ =
๐‘‰๐ฟ cos ๐›ผ
๐œ‹
= 2.34๐‘‰๐ฟ ๐‘๐‘œ๐‘ ๐›ผ
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Inverter
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Inverter
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Inverter (120o mode of operation)
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Inverter (180o mode of operation)
fd
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DC linked converter
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