ELEC 344, F-16 ELEC 344 - UBC ECEhamida/elec344/ELEC 344_M1.pdf · 2016-09-07 · • Magnetic...
Transcript of ELEC 344, F-16 ELEC 344 - UBC ECEhamida/elec344/ELEC 344_M1.pdf · 2016-09-07 · • Magnetic...
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ELEC 344Applied Electronics and
ElectromechanicsFall 2016
Instructor: Dr. Hamid Atighechi
My Webpage: www.ece.ubc.ca/~hamida
Class Webpage:
TBD
NOTE: Class notes are originally prepared by Dr. Juri
Jatskevich
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Major Topics Covered
• Principles of electromagnetics, inductance and reluctance
• Magnetic circuits & magnetically coupled systems
• Linear and rotating electromechanical devices
• Electromechanical energy conversion, developed forces and
torques
• AC power, three-phase system, connections and applications
• Rotating magnetic field, poly-phase systems
• Induction motor, operation, equivalent circuit
• Synchronous motor, operation, steady-state equivalent circuit
• Brushless dc motors, operation, steady-state characteristics
• Stepper motors, principle of operation, full-step, micro-
stepping, driver circuits
• Single phase AC motors
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Module 1, Part 1Introduction & Magnetic Circuits
(Read Chapter 1)
Most Important Topics
• Applications of Electromechanics
• Fundamentals of Electromagnetics, Maxwell’s Equations
• Sign & direction conventions
• Basic magnetic circuits, concepts, analogies, calculations
• Flux, flux linkage, inductance
• Magnetic materials, saturation, hysteresis loop
• Coil under ac excitation, type of core losses
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Applications of ElectromechanicsProduction of Electric Energy & Modern Electric Grid
Industrial Loads
Motor Drives
Fuel Cells
Battery
Storage
HydroPV Solar
Wind
Energy
HVDC
Transmission
System
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Mining Industry
Applications of Electromechanics
AC and DC
Electric Drives
Electric Cable Shovel Electric Dragline
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Heating and Melting
Applications of Electromechanics
Induction Furnace Induction Heater
No Flame Heater for
Dental Instrument
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Applications of ElectromechanicsModern Transportation
Diesel-Electric Hybrid
All-Electric
Toyota Hybrid,
operates at 288V,
reaches 30kW
Tesla Roadster,
Induction Motor,
reaches 200 kW
Liebherr T282B earth-
hauling truck 2.7MW
AC Propulsion
Canada Line
(Richmond-Airport-Vancouver Line)
SNC-Lavalin & Rotem Company
All-Electric => Zero Emission Transportation
Vancouver TransLink
Trolley Bus
New Flyer Industries
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Applications of ElectromechanicsModern Ships
Hybrid
High-Phase Count Motor Drives
Future Canadian Ship:
Joint Support Ship (JSS)
30.4MW Electric Propulsion
Carnival Liberty
Cruise Ship
2 x 20MW
Electric
Propulsion
HMCS Windsor Diesel-
Electric, 2x5MW motor-
generators
20MW, 15-Phase
Induction Motor
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High-Speed, Low-Weight, High-Phase-Count
Motors, Generators and Converters
Antares 20E
42kW BLDC Propulsion Airbus A380
Electric Toys
BLDC Propulsion
Applications of ElectromechanicsModern Aircraft
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High & Low
Applications of ElectromechanicsELEC 344, F-16
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Electromechanical DevicesIndustrial
Manufacturing
Automotive
Aircraft
Ships
Computers
Office
Household
…
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Electromechanical Energy Conversion
Input
Electrical
EnergyConversion
Device
Output
Mechanical
EnergyElectrical
System
(generator,
source, etc.)
Mechanical
System
(machine tool,
plant, etc.)
Input
Mechanical
EnergyConversion
Device
Output
Electrical
EnergyMechanical
System
(Prime Mover,
Turbine, etc.)
Electrical
System
(transmission,
distribution,
load, etc.)
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Electromechanical Energy Conversion
• Transformation of Electrical Energy
Input
Level X
Conversion
Device
Output
Level Y
Electrical
System
(generator,
source, etc.)
Electrical
System
(load)
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Electromechanical Energy Conversion
• Electrical Machines– Stationary
• Transformers
– Rotating
• Motors, generators
– Linear Devices
• Solenoids, linear motors, other actuators
• Power Electronics (Switched Mode PSs, Motor & Actuator Drivers, …)– Rectifiers
• AC to DC
– Converters
• DC to DC
– Inverters
• DC to AC
Very broad & interesting area, requires its own course!
Conversion
Device
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Magnetic Circuits: Basic Units
2m
WbT
E – electric field intensity
B – magnetic flux density
H – magnetic field intensity
F – magnetic flux
m
A
m
H
meter
Henry
A
mT
2mTWb
B-H Relation• Current produces the H field (see Ampere’s law)
• H is related to B
HHB r 0
– permeability (characteristic of the medium)
0 – permeability of vacuum
r – relative permeability of material
2meter
WeberTesla
mH7104
000,100100rmagnetic materials
m
V
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Fundamentals
• Maxwell's equations are a set of partial
differential equations that, together with
the Lorentz force law, form the
foundation of classical electrodynamics,
classical optics, and electric circuits
[Wikipedia].
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Fundamentals
Summarized in Maxwell’s Equations (1870s)
1) Gauss’s Law for Electric Field
Electric flux out of any closed surface is proportional to
the total charge enclosed
daEq
d e
s
F
cos0
aE
+
B
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Fundamentals
Summarized in Maxwell’s Equations (1870s)
2) Gauss’s Law for Magnetic Field
Magnetic flux out of any closed surface is zero
There are no magnetic charges
0F m
s
daB
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FundamentalsSummarized in Maxwell’s Equations (1870s)
3) Faraday’s Law
ElectroMotive Force (emf)
The line integral of the electric field around a closed loop/contour C is equal to the
negative of the rate of change of the magnetic flux through that loop/contour
emfdt
dd
dt
dd
SC
F
aBlE
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Fundamentals
20
ms
da FB Wb
dt
demf mF
V
Induced emf:
Lenz’s Law:
The direction of the voltage induced will produce a current that opposes
the original magnetic field. This gives the negative sign, which we do not always
include
Summarized in Maxwell’s Equations (1870s)
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Fundamentals
Summarized in Maxwell’s Equations (1870s)
4) Ampere’s Law (for static electric field)
The line integral of the magnetic field B around a closed loop C
is proportional to the net electric current flowing through that
loop/contour C
net
SC
IdaJd 00 lB
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ConventionsRight hand rule
Right-screw rule
Dot and cross notations
Magnetic field produced
by coil (solenoid)
Flux Lines:
• form a closed loop/path
• Lines do not cut across or merge
• Go from North to South magnetic poles
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Some Definitions
Magnetic Flux
F
SC
dt
dd
dt
dd aBlE
Recall Faraday’s Law - Electromotive Force (emf)
- voltage induced in one turn due to
the changing magnetic flux
For coil with N turns:dt
dNe
F
flux scaled by the number of turns
F N tWb
dt
de
Total induced emf V
Flux is always continuous
c
S
c AB F daB
Flux Linkage
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Some DefinitionsInductance
iLif
Need a function that relates Flux Linkage to the Current
Consider
Then
iL
H
A
tWb
Al
NL
N
Hli
i
AHN
i
ABN
i
N
iL
2
F
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Magnetic Circuits• Basic magnetic circuit
c
cc
A
l
Assume all magnetic field is continuous
and confined inside the core
Consider mmf c
c
ccccc
A
llBlHNiF FF
Define Reluctance (of the given magnetic path)
c
S
c AB F daB Wb
Wb
A
ELEC 344, F-16
What does
it remind
you of?
CR
N
Al
NL
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Ferromagnetism
• Magnetic moment:
Orbital motion of electrons
Spin of an electron
• In most of the materials,
the net magnetic moment
of one atom if exists is
cancelled out by the other
atom
• The five ferromagnetic
elements are:
Iron, Nicle, Cobalt,
Dysprosum, and Gadolinium
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Classes of Magnetic Materials
Diamagnetism
Paramagnetism
Ferromagnetism
Ferrimagnetism
Antiferromagnetism
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Magnetization Curve
• The magnetic material
shows the effect of
saturation
• The reluctance is
dependent on the flux
density
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Nonlinear
relationship
Linear
relationship
HHB r 0
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Magnetization Curve
• Depending on the
applications, material with
specific magnetization curve
is selected
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Magnetic Circuits• Magnetic circuit with air gap
Assuming all magnetic flux is
confined inside the coreand
Consider mmf
C
NiF dlH
ggcc lHlH
0
ggcclBlB
c
cA
BF
g
gA
BF
totaligc
g
g
c
c
A
l
A
lF FFF
F
0
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Magnetic and Electric Circuits Analogy
21 F
F
Electric Circuit
21 RR
vi
Magnetic Circuit
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Magnetic Circuit
- mmf,
- Flux
- Reluctance,
- Permeance,
- Permeability,
Electric Circuit
- Voltage (emf),
- Current,
- Resistance,
- Conductance,
- Conductivity,
Magnetic and Electric Circuits Analogy
,A
lR
AmpsI ,
VoltV ,
nniRv
SiemensR
G ,1
m
Siemens,
tAF ,
Wb,F
Wb
A
A
l,
A
Wb,
1
nnlHF
0N
ni 0FN
n
m
H,
For node
For loop For loop
For node
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Inductance: ExampleConsider the following electromagnetic system (device)
Equivalent Electric Circuit
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Inductance: ExampleConsider the following electromagnetic system
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Magnetic Materials
Magnetic moment
of an atom
Magnetic Domain Structure
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Magnetic Material Domain Model
demagnetized magnetized
B External field
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Hysteresis LoopELEC 344, F-16
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Hysteresis Loop
Hysteresis loops for
different excitation levelsBr – residual magnetism
Hc – coercivity force,
external field required to
demagnetize the
material
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Magnetic Materials
mA /1001.0~ cH
Soft mag. materials
Hard mag. materials
100cH mA /
Permanent magnets (PM)64 1010~ cH mA /
Types of PMs• Neodymium Iron Boron (NdFeB or NIB)
• Samarium Cobalt (SmCo)
• Aluminum Nickel Cobalt (Alnico)
• Ceramic or Ferrite, very popular
Iron-oxide, barium, etc. compressed powder
Classes of Magnetic Materials
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Magnetic MaterialsSecond quadrant hysteresis curve for some common PM materials
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Energy Stored in InductorConsider the following electromagnetic system
Instantaneous Power – rate of doing work
flossin PPeiritvtitP 2
Power going into the field eiPf dt
de
Recall mmf cclHNiF
and ccBNAN Fwhere
dt
dBHAlBNA
dt
d
N
lHeitP c
ccccccc
f dtPW ff
Change of Energy 2
1
2
1
B
B
cccc
t
t
ccccff dBHAldt
dt
dBHAldtPW
Energy
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Energy Stored in InductorEnergy per-unit-volume
Magnetically Linear (Approximate) System
2
1
B
B
ccf dBHw
Magnetically Nonlinear System
2
1
B
B
ccccf dBHAlW
constHB ;
2
1
2
22
2
1
BBAl
dBBAl
W cc
B
B
cccc
f
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Energy Stored in InductorEnergy in terms of flux linkage
2
1
2
1
iddtPW
t
t
ff
constLL
i ;
2
1
2
2
2
12
11
Ld
LW f
01 22
1 22 Li
LW If =>
Magnetically Linear (Approximate) SystemMagnetically Nonlinear System
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Core Losses
cccccc
cccycleh dBHAldBNA
N
lHidW ,
Consider
AC
excitation
Hysteresis Losses
Power loss can be approximated as
nchh BfKP max,
hK nWhere the constants and
determined experimentally
5.25.1~ n
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Where the constant depends
on lamination thickness and is
determined experimentally
Core Losses
2max,
2
cee BfKP
Consider
AC
excitation
Eddy Current Losses
Power loss can be approximated as
eK
SC
daBdt
ddlE
Faraday’s law
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EECE 365: Module 1, Part 2Basic Electromechanical devices and
Energy Conversion
Most Important Topics and Concepts (Read Chap. 3)• Basic linear devices with position-dependent reluctance &
inductance
• Basic rotating devices with position-dependent reluctance &
inductance
• Concept of coupling field
• Energy & Co-Energy
• Graphical interpretation of energy conversion
• Electromechanical force and torque
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Basic Electromagnet
lmNN FFF
Voltage equation
(Faraday’s law + KVL)
ll Ni F
Flux linkage
Flux leakage
Magnetizing flux mm Ni F
iLLiNN
ml
ml
22
Flux linkage & inductances
lL - Leakage inductance
(assume constant)
- Magnetizing inductance
(depends of position x)mL
dt
driv
Consider Magnetizing Pathgcm 2
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49
Basic ElectromagnetConsider Magnetizing Path gcm 2
Assume
x
l
Ax
c
cm 2
1)(
0 we getAAA gc
Magnetizing inductance
xk
k
xlAN
NL
ccmm
2
10
22
2
1
cr
cc
A
l
0 - Reluctance of the
stationary + movable core
g
gA
xx
0
)(
- Reluctance of the air-gap
where2
02
1AN
k
andc
clk2
2
Total inductance
llm Lxk
kLLL
2
1
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Practical Reluctance Devices
The basic electromagnet is very
similar to a plunger solenoid (Lab-1)
Open-frame solenoid
Closed-frame
tubular solenoid
Plunger solenoid (Lab-1)
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Other Reluctance DevicesSolenoids with linear motion
Rotating reluctance devices
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Rotating Reluctance Devices
0m
rm
rmm
NLL
2
- Maximum reluctance
iLLiNN
ml
ml
22
Flux linkage & inductances
2m - Minimum reluctance
Magnetizing inductance
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Electromechanical Energy ConversionELEC 344, F-16
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Basic Electromechanical System
mL - Magnetizing inductance
mf
r - Coil resistance
fe - EMF due to magnetizing inductance
(voltage drop due to coupling field)
v - Source voltage
i - Source current
- Movable mass
- Spring constant
- Electromagnetic force
- Energy supplied from electrical system
(going into coupling field)eW
- Energy going into mechanical system
(from coupling field)mW
- Energy in coupling fieldfW
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Electromechanical Energy Conversion
Energy Balance
Coupling
FieldeW mW
dxfWidteWWW mffmfe
0dx
ididtdt
didteW ff
First, lets consider fixed position, and assume
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Energy in Coupling Field
a Energy going in coupling field
aii
idWf
Consider a state of the system
Co-Energy associated with this state
Energy and Co-Energy Balance
diWc
cf WWi
Coupling Field is Conservative – The
stored energy does not depend on the
history of electromechanical variables, it
depends only on their final state/values
0dx, assuming
Non-linear magnetic system
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Energy in Coupling Field
57
The characteristic becomes linear by
increasing the air gap
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Energy in Coupling Field
a Energy going in coupling field
aii
idWf
Consider a state of the system
Co-Energy associated with this state
For magnetically linear systems
Energy and Co-Energy Balance
diWc
iWW cf 2
1
Coupling Field is Conservative – The
stored energy does not depend on the
history of electromechanical variables, it
depends only on their final state/values
0dx, assuming
Linear (Approximate) magnetic system
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Graphical interpretation
bx
Consider relationship
ax
Electromechanical Energy Conversion
i
Assume move from to
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Change in Energy
axState
bxState
OADOBCW f Coupling Field Energy
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ABCDiddtieWb
a
fe
Change in electrical input
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Change in Energy OADOBCABCDWWW fem Change in Mechanical Energy
mW
Change in mechanical work
under constant current
Remember Co-Energy
diWc
xfWW mcm
Developed
Electromagnetic Force
consti
cm
x
xiWxif
,,
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Change in EnergyOABWWW fem Change in Mechanical Energy at constant flux
Change in mechanical work
under constant current
fmm WxfW
Developed
Electromagnetic Force
const
fm
x
iWif
,,
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Electromagnetic Forces & TorquesLinear Devices Rotating Devices
dxfW mm
dxfdW mm
Mechanical Energy/Work
Electromagnetic Force
dTW mm
dTdW mm
Mechanical Energy/Work
Electromagnetic Torquemf mT
x
Wxif c
e
,
x
Wxf
fe
,
c
eW
iT ,
fe
WT ,
For magnetically linear systems
Energy and Co-Energy are the same 2
2
1
2
1ixLiWW cf
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ExampleLinear Devices
ix
kLixLLLixi lml
,
Given that
Calculate xifm ,
2,, alcf ix
kLxiWxiW
2
22
2
1
2
1,
x
ki
x
Li
x
Wxif aa
cm
at given current aii
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Typical Push-Pull Solenoids
Naturally, solenoid coil pulls in the plunger. To get a push action, a thrust pin is added.
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Typical Industrial Push-Pull SolenoidsELEC 344, F-16