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Study of Vector Control Algorithm and Inverter design for BLDC Motor, V/f control Algorithm
1. Study of Vector Control Algorithm
and Inverter design for BLDC Motor,
V/f control Algorithm
Project by: Amol Mahurkar, Ayush Modani, Ghanshyam Mali,
Heena Karir, Manoj Autade, Vivek Kumar
2. Objectives
2
Working of BLDC Motor
Different Control Algorithms for BLDC Motor
Vector Control Algorithm (Sensorless)
Inverter Design for BLDC Motor
Parametric Discussion on Inverter Design
Working of Induction Motor
Voltage versus Frequency Control Algorithm
4. Contents
4
Classification of motors
Motor Basics
BLDC motor and its construction
BLDC Control methods – Sensored Control
Clarke/Park Transformation
Sensorless control
Vector Control
5. Actuators
Industrial fans
Blowers and pumps
Machine tools
Household appliances
Power tools
Disk drives.
Actuators
Rotational Linear
Applications
5
6. Classification of motors
DC
Voltage Supply
AC
Voltage Supply
DC Motors Universal Motors
Solenoids Synchronous
Motors
EC Motors
Stepper Motors
Brushed
Brushless
Brushless
Driver
Electronics
6
9. BLDC Motor
Merits
Demerits
Less Maintenance
Longer Life
Flat SpeedVs.Torque Characteristics
High Efficiency
High Output Power/ Frame Size
Low Rotor Inertia
Higher Speed Range
Low Electric Noise Generation
Higher Cost of Building
Complex & Expensive Control
9
10. Brushless DC motor
Rotor is Permanent Magnet.
Stator is Electromagnet.
Windings is on the stator.
Three phase supply is given to windings
of stator
Torque is produced due to interaction
between magnetic field of rotor and
magnetic field produced by current in the
stator.
10
13. Vector control vs 1200 control
Performance→
Variable
Speed
Low Noise,
High Efficiency
Large
Torque
High
Response
COST
120°Drive
System
Vector
Control.
Typically for
Industry Use
Due to cost
for Appliances
1200control vs.Vector Control
Low performance low cost vs. high performance high cost
13
22. Measure current already flowing in the
motor
Measure ia and ib.
Calculate ic, from Kirchoff’s Law.
A, B, and C axes are “fixed”
with respect to the motor
housing.This reference
frame is also called the
“stationary frame” or “stator frame”.
22
23. Compare the measured current(vector) with the
desired current(vector), and generate error signals.
isis
Error
We must regulate the current vector magnitude and angle
by regulating ia, ib, and ic.
Commanded
Rotor axis flux
23
24. Measure the rotor angle to determine if the net current
vector is oriented at 900 with respect to the rotor flux
Θd
Usually accomplished with
a resolver or encoder.
24
25. Commanded
Convert the three phase current vectors into
two orthogonal vectors that will result In the
same net current vector. In other words,
convert 3-phase motor to 2-phase motor.
Then we have only two current values
to regulate
instead of three!
This is often referred to as the
FORWARD CLARKE
TRANFORMATION
i α
i β
25
26. Jump up on the rotating reference
frame, whose x-axis is rotor flux
axis.
This is often referred to as the
FORWARD PARK
TRANFORMATION
Commanded
i q
i d Θd
Total
4 trig calculations
7 multiplications
3 additions
26
27. +
-
id (commanded) error(t)
id (measured)
+
-
iq (commanded) error(t)
iq (measured)
id and iq are handled independently. Since the comparison is
performed in the rotating frame, AC frequency is not seen. Thus,
they are DC quantities!
Under normal conditions, we have all the
d-axis flux we need supplied by the permanent
magnets in the rotor. So commanded id is set to
zero.
This is how much torque we want!
id can however be used to weaken the field of the machine.
iq controls the amount of torque generated by the motor.
27
28. +
-
error(t)
+
-
iq (commanded) error(t)
iq (measured)
id (commanded)
id (measured)
P
ʃ I
+
+
vd
P
ʃ I
+
+
vq
The PI regulator is a good choice for current regulation
Amplify the error signals to generate
correction voltages
28
29. Modulate the correction voltages onto the
motor terminals
Commanded
i q
i d Θd
We now need to “jump
off” of the rotating
reference frame
Transfer the voltage vectors back
on to the stationary rectangular
coordinate system.
Reverse ParkTransformation
29
30. Commanded
Next, we transform the voltage vectors
from the rectangular coordinate
system to three phase vectors.
Reverse ClarkeTransformation
30
31. Over time, under steady-state conditions, the correction voltages va, vb, and vc
will be sine waves phase shifted by 1200
va
vb vc
31
40. POWER SWITCHING
BJT :Ability to handle high currents and
high voltages, Current controlled device.
Both the MOSFET and IGBT devices are
voltage controlled devices.
Control of the MOSFET and IGBT
devices much easier.
41. MOSFET
Voltage controlled device
Fast switching
No thermal runaway
Small on state resistance
Asymmetric blocking capacity
High power dissipation
PLOSS = Irms
2
* RDS-ON
Where: RDS-ON = drain-to-source on-state resistance
Irms = drain-to-source rms current
42. IGBT
Voltage controlled device
Advantages of both Power MOSFET and
BJT
Slower switching device
Asymmetric blocking capacity
Conductivity Modulation
PLOSS = Iave *VCE-SAT
Where:
VCE-SAT = Collector-to-emitter saturation voltage
Iave = collector-to-emitter average current
43. MOSFET vs IGBT
IGBTs are slower than MOSFETs.
IGBT has a very low on-state voltage
drop due to conductivity modulation and
has superior on-state current density.
45. Freewheeling Diode
A Freewheeling diode is a diode used to
eliminate the sudden voltage spike seen
across an inductive load when its supply
voltage is suddenly reduced or removed.
47. Back EMF
When a BLDC motor rotates, each winding generates a
voltage known as back EMF, which opposes the main
voltage supplied to the windings according to Lenz’s
Law.
It depends on,
Angular velocity of the rotor
Magnetic field generated by rotor magnets
The number of turns in the stator windings
Equation is as,
Back EMF = (E) ∝ NlrBω
48. Continued…..
Back-EMF refers to conclude the speed of the
motor's rotation.
Steps:
i. Provide current to the Motor windings
(as a constant voltage or a PWM motor input to
vary the speed).
ii. Remove the current from the windings and
"float" them.
The time required for the motor to flip from a
motor to a generator depends on the stored
charge in the induction of the motor windings.
52. CONTENTS
Introduction the induction motor.
Stator and Rotor construction.
RMF Generation.
Induced EMF and its direction.
Motor speed and Slip.
Torque vs speed and torque vs slip.
Need of V/F.
Block diagram of V/F control.
Comparison of V/F and Vector control.
53. INDUCTION MOTOR
•Motors operate on principle of Induction and hence the
name “Induction Motors” is used
•Motors also known as AC motors because Alternating
Current (AC) is required
•All AC motors are “brushless”
–No mechanical contacts to wear
–Requires AC source
–If used, inverter creates desired freq and magnitude
of AC
•AC induction motors for lower cost applications
–Single speed applications: fan, blower, pump,
compressor
–No control, just start the AC power source
–Relays are used for ON/OFF
54. STATOR CONSTROCTION
•Stator has windings with lamination to–Create
strong magnetic field–Maintain continuous flux
•Three phase motor windings are sinusoidal
around the stator to produce a roughly
sinusoidal distribution in flux
•When three phase AC voltages are applied to the
stator windings, a rotating magnetic field is
produced–The rotating magnetic field of the
stator drags the rotor around.
MORE
55. ROTOR CONSTRUCTION
Squirrel cage construction
–Behaves like shorted 3-
phase windings
–Rotor bars are often
skewed to prevent
cogging
–No magnets or windings
57. INDUCED EMF
Voltage is induced by following the Lenz Law. So
rotor will rotate in same direction as that of RMF,
to minimize the relative flux cutting.
STATOR
ROTOR
58. INDUCTION MOTOR SPEED
So, the IM will always run at a speed lower than the
synchronous speed
The difference between the motor speed and the
synchronous speed is called the Slip
Where nslip= slip speed
nsync= speed of the magnetic field
nm = mechanical shaft speed of the motor
slip sync mn n n= −
59. THE SLIP
sync m
sync
n n
s
n
−
=
Where s is the slip
Notice that : if the rotor runs at synchronous speed
s = 0
if the rotor is stationary
s = 1
Slip may be expressed as a percentage by multiplying the above
eq. by 100, notice that the slip is a ratio and doesn’t have units
60. SLIP CAUSES…..
1) Fr = s*F
2) E2r = s*E2
Where
Fr: Frequency of Induced Voltage
F: Applied Frequency
E2r: Induced EMF in Rotor
E2: Max. induced EMF in Secondary.
61. TORQUE VS SLIP
T α sR(E2) 2
R 2 + (sx)2
For LowSlip: T α s.
For HighSlip: T α 1/s.
Operated in stable region ie.
Region where(T<Tm)
SLIP(s)
Unstable
Stabl
e
torque
Tm
Tfl
S=
0
S=Sm
S=1
Tm
64. Induced Torque is zero at synchronous speed.
‡
The graph is nearly linear between no load and full load (at near
synchronous speeds).
‡
Max torque is known as pull out torque or breakdown torque
‡
Starting torque is very large.
‡
Torque for a given slip value would change to the square of the applied
voltage.
‡
If the rotor were driven faster than synchronous speed, the motor
would then become a generator.
‡
If we reverse the direction of the stator magnetic field, it would act as
a braking action to the rotor
65. WHY V/F
Ns = (120*F)/P
Constant Torque Applications.
T α sR(E2)2
R2 + (sx)2
Avoid core saturation
Φg α (V/f).
Vector control gives high torque at low RPM
Long distance controlling is easier with V/f
In V/f single drive can drive more than 1 motor.