Multilevel inverter topologies with reduced power circuit
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Multilevel inverter topologies with reduced
power circuit complexity for medium voltage
high power induction motor drives by
cascading conventional two-level and three-
level inverters
Sheron Figarado
Centre for Electronics Design
and Technology
Overview of the presentation
Multilevel inverter topologies
Three-level Common mode voltage elimination schemes
Simulation and Experimental results
Four-level scheme with CMV elimination and capacitor balancing
Simulation and Experimental results
Five-level inverter scheme
Simulation and Experimental results
Conclusion
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Advantages of Multilevel inverters
over two-level inverter
Devices of lower rating can be used thereby enabling the
schemes to be used for high voltage applications.
Reduced total harmonic distortion (THD).
Since the dv/dt is low, the EMI from the system is low.
Lower switching frequencies can be used and hence
reduction in switching losses.
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Disadvantages of multilevel inverters
The number of isolated DC-links are more compared to a
two-level inverter.
Neutral point voltage variations.
Power bus structure and hence the control schemes
become complex as the number of levels increases.
Decrease in Reliability
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Conventional two-level inverter
•Two-level inverters switches between + state
(+Vdc/2) and – state(-Vdc/2) with respect to the
O point.
•The Inverter has 8 switching states for 7
phasor locations.
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Three-level inverters- NPC
•A 3-level inverter has 3 levels of
switching namely +Vdc/2 (+state), 0
and –Vdc/2 (- state).
•The NPC inverter has 27 switching
states for 19 locations.
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Three-level inverters- cascaded
•Cascaded 3-level inverter has a
simpler power bus structure and
reduced device count.
• It has switching states same as
NPC 3-level inverter.
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Three-level inverters- open end
winding configuration
•The voltage rating of the DC bus is half that of 2-level inverter.
•Two isolated DC-links are required to avoid zero sequence currents.
•In this configuration we get 64 switching states for 19 vector locations,
whereas the conventional 3-level NPC inverter gives only 27 switching
states for 19 locations.
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Reduced Switch Count Three-level Space
phasor generation schemes with Common
Mode Voltage Elimination using cascaded
two-level inverters for an open- end winding
IM drive
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Common mode voltage- Definition
Common mode voltage is defined as
VAO +VBO +VCO
VCM =
3
where VAO ,VBO and VCO are the pole voltages
For an open end winding Common mode
voltage is defined as
VCM VCM 1 VCM 2
where VCM 1 is the common mode voltage of inverter 1 and
VCM 2 is the common mode voltage of inverter 2.
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Effect of common mode voltage
PWM inverters generate high frequency and high amplitude
common mode voltages, which induces ‗shaft voltages‘ on the
rotor side.
When the induced shaft voltage exceeds the breakdown
voltage of the lubricant in the bearings, result in large bearing
currents
This causes premature failure of the motor bearings and also
poses EMI issues.
In open end winding configuration, isolated DC links are
needed to avoid heavy currents due to the common mode
voltages in the phase windings.
The best solution for all these is to eliminate the CMV itself.
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CMV groups
The switching states of the inverter can be classified in terms of the
common mode voltage they generate.
Grou Switching states of 3–level inverter Common mode voltages
p generated
A +++ Vdc/2
B ++0, +0+, 0++ Vdc/3
C + – +, ++ –, – ++, 00+, 0+0, +00 Vdc/6
D 000, 0+ –, 0 – +, +0 –, + – 0, – 0+, – +0 0
E – – +, – + –, + – –, 00 –, 0–0, – 00, –Vdc/6
F – 0 –, 0 – –,0 – – –Vdc/3
G ––– –Vdc/2
If we select only those states with same common mode voltage then
the variation in CMV will not be there.
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2-level CMV elimination scheme
•We can select a 2-level structure
with zero common mode voltage
out of the 3-level structure.
•The common mode eliminated
structure has a 30 degree shift.
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Five-level inverter scheme
•This 5-level scheme needs 4 isolated DC links and 24 switches.
•Inverter is fed by two three-level inverters from both sides.
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5-level scheme hexagonal structure
•There are 729 states for 61 locations
compared to 125 switching states for the
conventional 5-level structure.
•A 3-level structure with switching
states of same CMV can be selected from
this 5-level structure.
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CMV groups for one inverter for open-end
winding configuration (CMV at the poles)
The switching states of the inverter can be classified in terms of the
common mode voltage they generate.
Group Switching states of 3–level inverter Number Common mode
of voltages
multiple generated
states
A +++ 1 Vdc/4
B ++0, +0+, 0++ 3 Vdc/6
C + – +, ++ –, – ++, 00+, 0+0, +00 6 Vdc/12
D 000, 0+ –, 0 – +, +0 –, + – 0, – 0+, – +0 7 0
E – – +, – + –, + – –, 00 –, 0–0, – 00 6 –Vdc/12
F – 0 –, 0 – –,0 – – 3 –Vdc/6
G ––– 1 –Vdc/4
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CMV eliminated hexagons
•Group C has CMV=+Vdc/12 in the
pole voltages.
•If the inverters on both sides uses
the states from group C CMV in the
phase voltage is eliminated.
•36 switching states for 19 locations.
•3 multiple switching states for each
location in the inner hexagon.
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CMV eliminated hexagons
•Group D has CMV=0 in the pole
voltages.
•If the inverters on both sides uses
the states from group D CMV in the
phase voltage is eliminated.
•49 switching states for 19 locations.
•4 multiple switching states for each
location in the inner hexagon.
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CMV eliminated hexagons
•Group E has CMV= -Vdc/12 in the
pole voltages.
•If the inverters on both sides uses
the states from group E CMV in the
phase voltage is eliminated.
•36 switching states for 19 locations.
•3 multiple switching states for each
location in the inner hexagon.
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3-level CMV eliminated scheme
•Since there is no CMV, isolated DC links are not needed.
•The scheme gives CMV elimination in all modulation range up to 6 step
mode.
•The linear modulation range is reduced to 0.5Vdc compared to SVPWM
scheme where the linear range is 0.577Vdc.
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Motivation for the Proposed scheme
Even after the selective switching for the common mode
voltage elimination, the three-level structure have higher
multiplicity in the switching states compared to the
conventional NPC three-level inverter without CMV
elimination.
This suggests that some optimization is possible in the
power circuit.
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States of individual switches for the group E CMV
eliminated structure
Switching Switching S11 S21 S31 S13 S23 S33 S11‘ S21‘ S31‘ S13‘ S23‘ S33‘
state of state of
Inverter I Inverter II
+–– ––+ 1 x x x 0 0 x x 1 0 0 x
00 – ––+ 0 0 x 1 1 0 x x 1 0 0 x
–+– ––+ x 1 x 0 x 0 x x 1 0 0 x
–+– 0–0 x 1 x 0 x 0 0 x 0 1 0 1
–+– +–– x 1 x 0 x 0 1 x x x 0 0
– 00 +–– x 0 0 0 1 1 1 x x x 0 0
––+ +–– x x 1 0 0 x 1 x x x 0 0
––+ 00 – x x 1 0 0 x 0 0 x 1 1 0
––+ –+– x x 1 0 0 x x 1 x 0 x 0
0–0 –+– 0 x 0 1 0 1 x 1 x 0 x 0
+–– –+– 1 x x x 0 0 x 1 x 0 x 0
+–– – 00 1 x x x 0 0 1 0 0 0 1 1
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Configuration I with switching states of group E
•The scheme has 18 switches and needs two isolated DC links.
•The inverters on either side share the top inverter.
•Thus both the inverters cannot be switched independently.
•Thus all the states are not possible for the second inverter once the
switching state of the other inverter is fixed.
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Possible switching states of inverter II
given the switching state of Inverter I
State of any phase of Possible states of
inverter- I inverter- II
+ +,–
0 0,–
– +,0, –
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Hexagonal space vector structure for Configuration I
•There is no multiplicity for the vector
locations except for zero state.
•Zero vector has a multiplicity of 3.
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PWM signal generation for the
proposed three-Level inverter with
common mode voltage elimination
A SVPWM generation algorithm is used to generate the switching
times for the phasor locations of the conventional three-level
inverter.
The PWM generation is based only on the sampled amplitude of the
reference voltages.
The algorithm has a linear relationship between output voltage
fundamental and reference input.
For generating PWM, the space phasor locations of the proposed
scheme is compared to that of a conventional three-level structure.
To compensate for the 30 degree shift, the reference itself is pre-
shifted by 30 degree.
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Mapping from conventional 3-level scheme
to CMV eliminated 3-level scheme
V S ' V S e j 30
The mapping of these signals of conventional three-level inverter to the proposed
three-level scheme is implemented using a look- up method implemented in
CPLD.
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Drive control scheme (V/f)
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Simulation and experimental
results for configuration I
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Results for 20Hz(2-level operation)-Configuration I
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
100V/division, X axis- 0.02s/div] 50V/division, X axis- 0.01s/div]
FFT of the pole voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 20Hz(2-level operation)-Configuration I
Phase voltage and phase current [Y axis- voltage Phase voltage and phase current [Y axis voltage
50V/div, current 1A/div, X axis – 0.05/div] 100V/div, current 1A/div, Y axis- 0.02s/div]
FFT of the phase voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 40Hz(3-level operation)-Configuration I
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
100V/division, X axis- 0.02s/div] voltage 100V/div, X axis- 0.01s/div]
FFT of the pole voltage waveform [X axis- order
of harmonic, Y axis- Normalized amplitude]
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Results for 40Hz(3-level operation)-Configuration I
Phase voltage and no load phase current [Y axis Phase voltage and no load phase current [Y axis
voltage 50V/div, current 1A/div, X axis- voltage 100V/div, current 1A/div, 0.01s/div]
0.01s/div]
FFT of the phase voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 46Hz(Overmodulation)-Configuration I
Pole voltages and phase voltage [Y axis- Pole voltages and phase voltage [Y axis
100V/div, X axis- .02s/div] voltage 100V/div, X axis- 0.01s/div]
FFT of the pole voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 46Hz(Overmodulation)-Configuration I
Phase voltage and no load phase current Y Phase voltage and no load phase current [Y axis
axis -50V/div, current 1A/div, X axis- voltage 100V/div, current 1A/div, X axis-
0.01s/div] 0.01s/div]
FFT of the phase voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 48Hz(Overmodulation)-Configuration I
Pole voltages and phase voltage [Y axis – Pole voltages and phase voltage [Y axis –
voltage 100V/div, X axis – 0.01s/div] voltage 100V/div, X axis – 0.01s/div]
FFT of the pole voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 48Hz(Overmodulation)-Configuration I
Phase voltage and no load phase current [Y Phase voltage and no load phase current [Y axis –
axis – voltage 100V/div, X axis – 0.01s/div] voltage 100V/div, current 1A/div, X axis –
0.01s/div]
FFT of the phase voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 50Hz (6step mode)-Configuration I
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
– 100V/div, X axis – 0.02s/div] – 100V/div, X axis – 0.01s/div]
FFT of the pole voltage waveform [X axis- order of
harmonic, Y axis- Normalized amplitude]
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Results for 50Hz (6step mode)-Configuration I
Phase voltage and no load phase Phase voltage and no load phase current [Y axis –
current [Y axis – 100V/div, X axis – voltage 100V/div, current 1A/div, X axis –
0.01s/div] 0.01s/div]
FFT of the phase voltage waveform [X axis- order
of harmonic, Y axis- Normalized amplitude]
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Acceleration from 20-30Hz (two-level to
three-level transition)
Phase voltage and no load phase current [Y axis – Phase voltage and no load phase current [Y axis –
Voltage 100V/div, current 1A/div, X axis – Voltage 100V/div, current 1A/div, X axis –
0.05s/div] 0.05s/div]
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Acceleration from 40-50Hz (linear range to 6
step through overmodulation)
Smooth transition of phase voltage and phase Smooth transition phase voltage and phase
current [Y axis – Voltage 100V/div, current current [Y axis – Voltage 100V/div, current
1A/div, X axis – 0.05s/div] 1A/div, X axis – 0.05s/div]
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Speed Reversal from -20 to 20Hz
The profile of the phase current during speed The profile of the phase current during speed
reversal when the system is given a reversal reversal when the system is given a reversal
command from 20Hz to -20 Hz [Y axis – command from 20Hz to -20 Hz [Y axis –
current 1A/div, X axis – 1s/div] current 1A/div, X axis – 1s/div]
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Upper cascaded structure
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Configuration II with switching states of CMV
group C
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Possible switching states of inverter II given
the switching state of Inverter I
State of any phase of Possible states of
inverter- I inverter- II
+ +,0, –
0 +,0
– +, –
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The space vector hexagon for Configuration II
• The hexagonal structure has no
multiplicity in switching states
for any phasor location but zero
phasor.
• The zero phasor has 3 switching
states.
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Simulation and experimental
results for configuration II
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20Hz(2-level operation)-Configuration II
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis-
50V/division, X axis- 0.016s/div] 50V/division, X axis- 0.01s/div ]
Phase voltage and no load phase current [Y axis Phase voltage and no load phase current [Y axis
voltage 100V/div, current 1A/div, Y axis- voltage 50V/div, current 1A/div, Y axis- 0.01s/div
0.014s/div] ]
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20Hz(3-level operation)-Configuration II
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
voltage 100V/div, X axis- 0.01s/div] voltage 100V/div, X axis- 0.005s/div ]
Phase voltage and no load phase current [ Y Phase voltage and no load phase current [Y axis
axis voltage 50V/div, current 1A/div, X voltage 50V/div, current 1A/div, 0.005s/div ]
axis-0.01s/div]
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46Hz(Overmodulation) operation-Configuration II
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
voltage 100V/div, X axis- 0.01s/div] voltage 100V/div, X axis- 0.005s/div ]
Phase voltage and no load phase current [ Y axis Phase voltage and no load phase current [Y axis
voltage 50V/div, current 1A/div, X axis-0.006s/div] voltage 50V/div, current 1A/div, X axis-
0.005s/div]
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48Hz(Overmodulation) operation-Configuration II
Pole voltages and phase voltage [Y axis Pole voltages and phase voltage [Y axis
– voltage 100V/div, X axis – 0.01s/div] – voltage 100V/div, X axis – 0.005s/div]
Phase voltage and no load phase current [Y axis – Phase voltage and no load phase current [Y axis –
voltage 50V/div, current 1A/div, X axis – voltage 50V/div, current 1A/div, X axis –
0.01s/div] 0.005s/div ]
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50Hz(6-step mode) operation-Configuration II
Pole voltages and phase voltage [Y Pole voltages and phase voltage [Y
axis – 100V/div, X axis – 0.01s/div] axis – 100V/div, X axis – 0.005s/div ]
Phase voltage and no load phase current [Y axis – Phase voltage and no load phase current [Y axis –
voltage 50V/div, current 1A/div, X axis – voltage 100V/div, current 1A/div, X axis –
0.01s/div] 0.005s/div ]
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Acceleration from 20-30Hz (two-level to
three-level transition)
Phase voltage and no load phase current [Y axis –
Voltage 100V/div, current 1A/div, X axis –
0.025s/div]
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Acceleration from 40-50Hz (linear range to 6
step through overmodulation)
Smooth transition phase voltage and phase current
[Y axis – Voltage 50V/div, current 1A/div, X axis –
0.025s/div]
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Reversal from -20 to 20Hz
The profile of the phase current during speed
reversal when the system is given a reversal
command from 20Hz to -20 Hz [Y axis –current
1A/div, X axis – 1s/div]
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Salient features of the drive schemes
Only 18 switches are needed for a CMV eliminated 3-
level drive scheme compared to the previous
configuration which has 24 switches.
CMV is eliminated in the entire modulation range upto 6
step mode.
Only two isolated dc-links are needed.
An SVPWM algorithm which uses only sampled
amplitude of the reference signals for switching time
computation is used which makes the implementation
faster compared to the conventional methods.
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A Four-level inverter scheme with Common
mode voltage elimination and capacitor
voltage balancing for an open-end winding
Induction machine
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Seven- level power circuit
• Six conventional two-level inverters and 6 isolated supplies to get a 7-level structure.
•Inverter A is a four -level inverter formed by cascading 3 two-level inverters.
•Motor is fed from both ends.
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CMV groups of the switching states
CMV group Generated Switching states
CMV
A +Vdc/2 333
B +4Vdc/9 332,323,233
C +7Vdc/18 322,232,223,331,133,313
D +Vdc/3 330,303,033,321,312,213,231,123,132,222
E +5Vdc/18 320,302,230,203,023,032,311,131,113,221,212,122
F +2Vdc/9 310,301,130,103,013,031,220,202,022,211,112,121
G +Vdc/6 300,030,003,210,201,120,102,012,021,111
H +Vdc/9 200,020,002,110,101,011
I +Vdc/18 100,010,001
J 0 000
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Four level CMV eliminated space vector structure
•4096 switching states for 127 vector locations.
•Four level CMV eliminated structure formed out of 7-level structure.
•Only 4 CMV groups namely D,E, F and G can form four-level structure.
• E and F have 144 switching states and D and G have 100 switching states for 37 locations.
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Four-level CMV eliminated scheme ( group F)
•Switching states of CMV group F are selected.
•Since there is no CMV, the dc links for Inverter A and Inverter B can be
connected together .
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Voltage phasor locations and number of redundant states
of the CMV eliminated 4-level inverter
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Switching states corresponding to the vector locations of
60o sector C1‘-O‘-C4‘
Phasor Switching states
location
O‘(12) (022,022), (220,220), (202,202), (112,112), (211,211),
(121,121), (013,013), (031,031), (103,103),
(130,130), (301,301), (310,310)
A1‘(8) (310,211), (220,121), (121,022), (211,112), (112,013),
(202,103), (130,031), (301,202)
A2‘(8) (121,112), (211,202), (220,211), (130,121), (031,022),
(310,301),(022,013), (112,103)
B1‘(4) (310,112), (220,022), (211,013), (301,103)
B2‘(5) (220,112), (310,202), (211, 103), (121,013), (130,022)
B3‘(4) (130,112), (121,103), (031,013),(220,202)
C1‘(1) (310,013)
C2‘(2) (220,013),(310,103)
C3‘(2) (220,103),(130,013)
C4‘(1) (130,103)
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Model of the four level inverter
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Phase winding connections for switching states
corresponding to phasor location O‘ (ZV)
•Switching states are has no effect of the capacitor currents.
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Two-level(2L) group switching states (phasor location A1‘)
IC3= ia IC3= -ic IC3= ia- ic
IC2=–ic IC2= ia- ic IC2= ia- ic
IC1= ia- ic IC1= –ia IC1= 0
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Two-level(2L) group switching states (phasor location A1‘)
-Continued
IC3= ia- ic IC3= - ic IC3= ia- ic
IC2= - ic IC2= ia IC2= ia
IC1= ia IC1= ia- ic IC1= - ic
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Two-level(2L) group switching states (phasor location A1‘)
-Continued
IC3= ia IC3= ia- ic
IC2= ia- ic IC2= 0
IC1= - ic IC1= ia- ic
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Two-level(2L) group switching states
Vector Switching state DC-link Capacitor currents
IC3 IC2 IC1
Two-level(2L) group switching states
A1‘(1,0,-1) (202,103) ia -ic ia-ic
(310,211) -ic ia-ic ia
(130,031) ia-ic ia-ic 0
(220,121) ia-ic -ic ia
(301,202) -ic ia ia-ic
(121,022) ia-ic ia -ic
(112,013) ia ia-ic -ic
(211,112) ia-ic 0 ia-ic
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Three-level(3L) group switching states (phasor location B1‘)
IC3= - ic IC3= ia
IC2= 0 IC2= 0
IC1= ia IC1= - ic
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Three-level(3L) group switching states (phasor location B1‘)
IC3= ia- ic IC3= 0
IC2= 0 IC2= 0
IC1= 0 IC1= ia- ic
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Three-level(3L) group switching states (phasor location B2‘)
IC3= ia+ ib- ic IC3= ia- ic IC3= ib- ic
IC2= 0 IC2= ia+ ib IC2= ia+ ib
IC1= ia+ ib IC1= ib IC1= ia
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Three-level(3L) group switching states (phasor location B2‘)
IC3= ia+ ib
IC3= ia+ ib
IC2= ia
IC2= ib
IC1= ib-ic
IC1= ia-ic
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Three-level(3L) group switching states
Vector Switching state DC-link Capacitor currents
IC3 IC2 IC1
Three-level(3L) group switching states
B1‘(2,0,-2) (310,112) -ic 0 ia
(211,013) ia 0 -ic
(220,022) ia-ic 0 0
(301,103) 0 0 ia-ic
B2‘(1,1,-2) (220,112) ia+ib-ic 0 ia+ib
(130,022) ia-ic ia+ib ib
(310,202) ib-ic ia+ib ia
(211,103) ia+ib ib ia-ic
(121,013) ia+ib ia ib-ic
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Four-level(4L) group switching states
Phasor location C1’ Phasor location C2’
Vector Switching state DC-link Capacitor currents
IC3 IC2 IC1
Four-level(4L) group switching states
C1‘(3,0,-3) (310,013) 0 0 0
C2‘(2,1,-3) (220,013) ia+ib 0 ib
(310,103) ib ib ia
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Principle of capacitor voltage balancing
•If the capacitor is sized for the reactive
current, the DC- link capacitor voltages will
not get unbalanced under no load conditions.
•Only active component of the load causes
capacitor voltage imbalance.
• At any instant, active component of the
current vector is in the same direction as that
of the voltage phasor.
•Projections of active component on the axes
are ιd cos(φ ), ιd cos(120 φ ), ιd cos(120 φ )
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Capacitor current as a function of active components of the
motor phase currents
IC3= ia
IC2= - ic
IC3= ia–ic
•Vector here is (1,0,-1)
•φ =30o
IC1= ia‘
IC2= ic‘
IC3= ia‘+ ic‘
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Capacitor currents- Two-level(2L) group switching states
Vector Switching DC-link Capacitor currents Relative magnitudes of
state IC3 IC2 IC1 active components of
the phase currents
Two-level(2L) group switching states
A1‘(1,0,-1) (202,103) i+a' ic' ia'+ic' ib'=0,ia'=ic'
(310,211) ic' ia'+ic' ia' ib'=0,ia'=ic'
(130,031) ia'+ic' ia'+ic' 0 ib'=0,ia'=ic'
(220,121) ia'+ic' ic' ia' ib'=0,ia'=ic'
(301,202) ic' ia' ia'+ic' ib'=0,ia'=ic'
(121,022) ia'+ic‘ ia' ic' ib'=0,ia'=ic'
(112,013) ia' ia'+ic' ic' ib'=0,ia'=ic'
(211,112) ia'+ic' 0 ia'+ic' ib'=0,ia'=ic'
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Capacitor currents- Three-level(3L) group switching states
Vector Switching DC-link Capacitor currents Relative magnitudes of
state IC3 IC2 IC1 active components of
the phase currents
Three-level(3L) group switching states
B1‘(2,0,-2) (310,112) ic' 0 ia' ib'<ia'=ic'
(211,013) ia' 0 ic' ib'<ia'=ic'
(220,022) ia'+ic' 0 0 ib'<ia'=ic'
(301,103) 0 0 ia'+ic' ib'<ia'=ic'
B2‘(1,1,-2) (220,112) ia'+ib'+ic' 0 ia'+ib' ib=ia'<ic'
(130,022) ia'+ic' ia'+ib' ib' ib'=ia'<ic'
(310,202) ib'+ic' ia'+ib' ia' ib'=ia'<ic'
(211,103) ia'+ib' ib' ia'+ic' ib'=ia'<ic'
(121,013) ia'+ib' ia' ib'+ic' ib'=ia'<ic'
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Capacitor currents- Four-level(4L) group switching states
Vector Switching DC-link Capacitor currents Relative magnitudes of
state IC3 IC2 IC1 active components of
the phase currents
Four-level(4L) group switching states
C1‘(3,0,-3) (310,013) 0 0 0 ib'=0,ia'=ic'
C2‘(2,1,-3) (220,013) ia'+ib' 0 ib' ib'<ia'<ic'
(310,103) ib' ib' ia‘ ib'<ia'<ic'
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Operation at sector B1‘- C1‘- C2‘
Vector Switching IC3 IC2 IC1 Relative
state magnitude
B1‘(2,0,-2) (310,112) ic' 0 ia' ib'<ia'=ic'
(211,013) ia' 0 ic' ib'<ia'=ic'
(220,022) ia'+ic' 0 0 ib'<ia'=ic'
(301,103) 0 0 ia'+ic' ib'<ia'=ic'
C1‘(3,0,-3) (310,013) 0 0 0 ib'=0,ia'=ic'
C2‘(2,1,-3) (220,013) ia'+ib' 0 ib' ib'<ia'<ic'
(310,103) ib' ib' ia‘ ib'<ia'<ic'
•It can be seen that none of the switching states of
vector B1‘ affect the middle capacitor C2, but affects
the top and bottom capacitors.
•Switching state of vector C1‘ do not affect any
capacitor voltages.
•It can be seen that it is not possible to operate only
with DC-link.
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Modified power circuit
•The middle capacitor is
supplied with a DC- source of
voltage rating Vdc/6.
•Now, the Capacitor balancing
problem is between C1 and C3.
•Even in this case, there are cases
where the currents of the
redundant states are not exactly
opposite.
•Thus an open loop capacitor
voltage balancing scheme is not
possible.
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Operation in open -loop
Vector Switching IC3 IC1 Relative
state magnitude
B1‘(2,0,-2) (310,112) ic' ia' ib'<ia'=ic' Complementary
(211,013) ia' ic' ib'<ia'=ic' pair
(220,022) ia'+ic' 0 ib'<ia'=ic'
(301,103) 0 ia'+ic' ib'<ia'=ic'
C1‘(3,0,-3) (310,013) 0 0 ib'=0,ia'=ic'
C2‘(2,1,-3) (220,013) ia'+ib' ib' ib'<ia'<ic'
(310,103) ib' ia‘ ib'<ia'<ic'
•Capacitor balancing problem is between C1 and C3.
•Even in this case there are cases where the currents
of the redundant states are not exactly opposite.
•Thus an open loop capacitor voltage balancing
scheme is not possible.
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Operation in open-loop
Vector Switching IC3 IC1 Relative
state magnitude
B1‘(2,0,-2) (310,112) ic' ia' ib'<ia'=ic'
(211,013) ia' ic' ib'<ia'=ic'
(220,022) ia'+ic' 0 ib'<ia'=ic' Complementary
(301,103) 0 ia'+ic' ib'<ia'=ic' pair
C1‘(3,0,-3) (310,013) 0 0 ib'=0,ia'=ic'
C2‘(2,1,-3) (220,013) ia'+ib' ib' ib'<ia'<ic'
(310,103) ib' ia‘ ib'<ia'<ic'
•Capacitor balancing problem is between C1 and C3.
•Even in this case there are cases where the currents
of the redundant states are not exactly opposite.
•Thus an open loop capacitor voltage balancing
scheme is not possible.
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Operation in open-loop
Vector Switching IC3 IC1 Relative
state magnitude
B1‘(2,0,-2) (310,112) ic' ia' ib'<ia'=ic'
(211,013) ia' ic' ib'<ia'=ic'
(220,022) ia'+ic' 0 ib'<ia'=ic'
(301,103) 0 ia'+ic' ib'<ia'=ic'
C1‘(3,0,-3) (310,013) 0 0 ib'=0,ia'=ic' No effect
C2‘(2,1,-3) (220,013) ia'+ib' ib' ib'<ia'<ic'
(310,103) ib' ia‘ ib'<ia'<ic'
•Capacitor balancing problem is between C1 and C3.
•Even in this case there are cases where the currents
of the redundant states are not exactly opposite.
•Thus an open loop capacitor voltage balancing
scheme is not possible.
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Operation at sector B1‘- C1‘- C2‘
Vector Switching IC3 IC1 Relative
state magnitude
B1‘(2,0,-2) (310,112) ic' ia' ib'<ia'=ic'
(211,013) ia' ic' ib'<ia'=ic'
(220,022) ia'+ic' 0 ib'<ia'=ic'
(301,103) 0 ia'+ic' ib'<ia'=ic'
C1‘(3,0,-3) (310,013) 0 0 ib'=0,ia'=ic'
C2‘(2,1,-3) (220,013) ia'+ib' ib' ib'<ia'<ic' No
Complementary
(310,103) ib' ia‘ ib'<ia'<ic'
states
•Capacitor balancing problem is between C1 and C3.
•Even in this case there are cases where the currents
of the redundant states are not exactly opposite.
•Thus an open loop capacitor voltage balancing
scheme is not possible.
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Closed loop control of the capacitor voltages
• ΔV= VC3-VC1
•If ΔV>0 then controller
state is CH
•If ΔV=0 then controller
state is CN
•If ΔV<0 then controller
state is CL
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Switching state and the corrective action
Vector Switching state Relative magnitudes of the Corrective action for
capacitor currents
A1‘(1,0,-1) (202,103) IC3< IC1 CH
(310,211) IC3= IC1 CN
(130,031) IC3> IC1 CL
(220,121) IC3> IC1 CL
(301,202) IC3< IC1 CH
(121,022) IC3> IC1 CL
(112,013) IC3= IC1 CN
(211,112) IC3= IC1 CN
B1‘(2,0,-2) (310,112) IC3= IC1 CN
(211,013) IC3= IC1 CN
(220,022) IC3> IC1 CL
(301,103) IC3< IC1 CH
B2‘(1,1,-2) (220,112) IC3> IC1 CL
(130,022) IC3> IC1 CL
(310,202) IC3> IC1 CL
(211,103) IC3< IC1 CH
(121,013) IC3< IC1 CH
C1‘(3,0,-3) (310,013) IC3= IC1 CN
C2‘(2,1,-3) (220,013) IC3> IC1 CL
(310,103) IC3< IC1 CH
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Simulation results
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Steady state results-Two- level operation
VAO
VAA
VAA
VA‘O Ia
Controller
state
Pole voltages, phase voltage and controller state Phase voltage and no load phase current (X- axis 50
(X- axis 50 ms/div, Y axis- 100V/div) ms/div, Y axis- voltage- 100V/div, current- 1A/div
FFT of the phase voltage (X axis- order of harmonics,
Y axis- normalized magnitude)
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Steady state results -Three-level operation
VAO
VAA
VAA
VA‘O
Controller Ia
state
Pole voltages, phase voltage and controller state Phase voltage and no load phase current (X axis- 50
(X axis- 50 ms/div, Y axis- 100V/div) ms/div, Y axis- voltage- 100V/div, current- 1A/div
)
FFT of the phase voltage (X axis- order of harmonics,
Y axis- normalized magnitude)
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Steady state results -Four-level operation
VAO
VAA
VAA
VA‘O
Controller Ia
state
Pole voltages, phase voltage and controller state Phase voltage and no load phase current (X axis- 10
(X axis- 10 ms/div, Y axis- 200V/div) ms/div, Y axis- voltage- 100V/div, current-
2A/div)
FFT of the phase voltage (X axis- order of harmonics,
Y axis- normalized magnitude)
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Steady state results-18-step operation
VAO
VAA VAA
VA‘O
Controller Ia
state
Pole voltages, phase voltage and controller state Phase voltage and no load phase current (X axis- 20
(X axis- 10 ms/div, Y axis- 200V/div) ms/div, Y axis- voltage- 100V/div, current- 2A/div)
FFT of the phase voltage (X axis- order of harmonics,
Y axis- normalized magnitude)
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Capacitor voltage balancing during two-level
operation
•During two-level operation, since the
second source is across the C2 capacitor, the
power is directly delivered to the load from
the source.
•Again, all the locations in the two-level case
have complementary switching pairs.
•So chance of getting large unbalanced state
is minimal.
(X axis- 0.2 s/div, Y axis- 2V/div)
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Capacitor voltage balancing during three-level
operation
When the controller is disabled
Normal operation momentarily and enabled again
X axis- 0.2 s/div, Y axis- 20V/div X axis- 0.2 s/div, Y axis- 20V/div
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Capacitor voltage balancing during four-level
operation
Normal operation When the controller is disabled
momentarily and enabled again
(X axis- 0.2 s/div, Y axis- 5V/div) (X axis- 0.1 s/div, Y axis- 20V/div)
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Capacitor voltage balancing during 18-step mode of
operation
Normal operation When the controller is disabled
momentarily and enabled again
(X axis- 0.2 s/div, Y axis- 5V/div) (X axis- 0.1 s/div, Y axis- 20V/div)
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Experimental results
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Two-level operation
VA‘O
VAO
VAA‘
Controller state
(X- axis – 25ms/div, Y- axis- trace 1- 50V/div, trace 2-
50V/div, trace 3 - 50V/div, trace 4- 1V/div)
VAA‘
VC3,VC1
Ia
(X- axis – 25ms/div, Y- axis- trace 1- 50V/div, trace
2- 10V/div, trace 3- 10V/div, trace 4- 500mA/div)
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Three-level operation
VA‘O
VAO
VAA‘
Controller state
(Y axis -Trace 1- 50V/div, Trace 2 - 50V/div, trace 3-
100V/div, trace 4- 1V/div, X axis - 10ms/div)
VAA‘
VC3,VC1
Ia
(X- axis –10ms/div, Y- axis- trace 1- 50V/div, trace
2- 10V/div, trace 3- 10V/div, trace 4- 500mA/div)
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Four-level operation
VA‘O
VAO
VAA‘
Controller state
(X- axis –5ms/div, Y- axis- trace 1- 50V/div, trace 2-
50V/div, trace 3- 100V/div, trace 4- 1V/div)
VAA‘
VC3,VC1
Ia
(X- axis –10ms/div, Y- axis- trace 1- 100V/div, trace
2- 10V/div, trace 3- 10V/div, trace 4- 500mA/div)
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18 step operation
VA‘O
VAO
VAA‘
Controller state
(X- axis –5ms/div, Y- axis- trace 1- 50V/div, trace 2-
50V/div, trace 3- 50V/div, trace 4- 1V/div)
VAA‘
VC3,VC1
Ia
(X- axis –10ms/div, Y- axis- trace 1- 100V/div, trace
2- 10V/div, trace 3- 10V/div, trace 4- 500mA/div)
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Corrective action of the controller when the control is
disabled and enabled again-Three-level operation
VC3,VC1
VAA‘
(X- axis –250ms/div, Y- axis- trace 1- 20V/div,
trace 2- 20V/div, trace 3-- 500mA/div)
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Corrective action of the controller when the control is
disabled and enabled again-Four-level operation
VC3,VC1
VAA‘
(X- axis –250ms/div, Y- axis- trace 1- 20V/div,
trace 2- 20V/div, trace 3— 500mA/div)
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Corrective action of the controller when the control is
disabled and enabled again-18 step operation
VC3,VC1
VAA‘
(X- axis –250ms/div, Y- axis- trace 1- 20V/div,
trace 2- 20V/div, trace 3—500mA/div)
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Acceleration from three-level operation to
four-level operation
Phase voltage and phase current (X axis-
100ms/div, Y axis- trace 1- 50V/div, trace 2-
1A/div
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Salient features of the drive schemes
A four-level CMV eliminated drive scheme using 6 two-level
inverters is proposed. The scheme needs 36 switches.
CMV is eliminated in the entire modulation range upto 6 step
mode.
The capacitor balancing is not possible since all the locations do
not have redundant switching states with opposite/no effect on
the capacitor voltages.
A closed loop capacitor voltage balancing scheme is
implemented. This achieves the capacitor balancing and thus
needs only two-isolated DC- sources.
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A Reduced Five-level inverter
scheme for an open- end winding
Induction machine
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A five-level inverter circuit
•One 3-level NPC inverter from one side and a 2-level inverter from the other side.
•The devices of the two-level inverter has to withstand the whole DC-link voltage
•Two isolated supplies are used.
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Space vector locations for individual inverters
Inverter I Inverter II
•27 switching states for 19 locations •8 switching states for 7 locations
•27 Together they constitute a five-level structure
with 216 switching states for 61 locations
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One leg of the power circuit for the five-
level inverter scheme
Voltage
Inverter I Inverter II
level
+Vdc/2 S11 S2‘
+Vdc/4 S12&S13 S2‘
S14 S2‘
0
S11 S1‘
-Vdc/4 S12&S13 S1‘
-Vdc/2 S14 S1‘
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Space vector structure generated by the five-level
scheme
• 216 switching states corresponding to the 61 vector locations.
•Multiplicity is very less compared to the 5- level structure given in the first
scheme, which has a multiplicity of 729 for 61 vector locations.
•But still high as compared to conventional NPC inverter scheme where the
number of switching states are 125 for 61 locations.
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Comparison with conventional Five-level schemes
Configuration Number of Number of Number Number of
controlled power diodes capacitors DC sources
switches
MPC (Multi-point clamped) 24 18(36) 4 4
Cascaded H- bridge 24 Nil 6 6
Cascaded structure with two 2-level 24 6 4 4
and one 3-level NPC structure
Flying capacitor topology 24 Nil 1+9 1
capacitors
(4+18 cap)
Open-end winding (symmetric 24 12 4 4
case)
Open-end winding (asymmetric- 12+6 6 3(4) 3
two-level on one side)
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Challenges in implementation
If isolated supplies are used from both sides, then there
will be phase opposition of the DC-sources which will
cause voltage variations in DC- links.
One solution is to use the same DC- link for inverters of
both the side thereby avoiding subtraction. But, if
isolation is not provided, there will be huge triplen
currents through the phases.
This triplen currents has to be taken care of.
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Power circuit for the five- level inverter
scheme
•One 3-level NPC inverter from one side and a 2-level inverter from the other side.
•The devices of the two-level inverter has to withstand the whole DC-link voltage
•Two isolated supplies are used.
•By using Sine-triangle modulation scheme, the CMV is eliminated in an average
sense
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Five-level sine-triangle modulation
Triangle 1
Triangle 2
(Primary
triangle)
Triangle 2
Triangle 4
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CMV elimination in an average sense
Sine triangle modulation scheme is used for modulation
Since the pole voltages are equal to the reference sinusoids in an average
sense, the sum (VAO+VBO+VCO)= (Vas+Vbs+Vcs) in an average sense.
For a balance three-phase system, (Vas+Vbs+Vcs) =0
By definition, VCM= (VAO+VBO+VCO)/3
Therefore, VCM =0 in the average sense.
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CMV elimination in an average sense
(n 1)
Vas Vm Sin t Tga Tas [ Ia ] TS
2
2 (n 1)
Vbs VmSin( t ) Tgb Tbs [ Ib ] TS
3 2
4 (n 1)
Vcs VmSin( t ) Tgc Tcs [ I c ] TS
3 2
Vdc n1
Ts (n 1) V AO( avg ) [Tga TS ( Ia )]
Tas Vas Ts (n 1) 2
Vdc Vdc n1
T (n 1) VBO( avg ) [Tgb TS ( Ib )]
Tbs Vbs s Ts (n 1) 2
Vdc
and
T (n 1)
Tcs Vcs s Vdc n1
Vdc VCO( avg ) [Tgc TS ( I c )]
Ts (n 1) 2
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CMV elimination in an average sense
1 Vdc n1 n1
VCM ( avg ) [Tas ( Ia ) TS Tbs ( Ib ) TS
3 Ts (n 1) 2 2
n1 n1 n1 n1
Tcs ( I c ) TS +TS ( Ia ) TS ( Ib ) TS ( I c )]
2 2 2 2
1 Vdc 3(n 1)
[Tas Tbs Tcs ( Ia Ib I c ) TS TS
3 Ts (n 1) 2
3(n 1)
TS ( Ia Ib I c ) TS ]
2
1 Vdc
[T Tbs Tcs ]
3 Ts (n 1) as
For a balanced system
(n 1)Ts
Tas Tbs Tcs Vas Vbs Vcs 0
Vdc
1 Vdc
VCM ( avg ) [Tas Tbs Tcs ] 0
3 Ts (n 1)
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V/f control scheme
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Simulation results
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20Hz operation- steady state results
VAO
VAA‘
VAA‘
VA‘O
Ia
Icm VCM
Trace 1- Phase voltage, trace 2- no load Trace1-pole voltage of inverter I, trace 2-
phase current, trace 3- common mode phase voltage, trace 3- pole voltage of
current (X axis- 0.01s/div,Y axis- inverter II, trace 4- common mode voltage (X
10V/div,1A/div) axis- 0.01s/div, Y axis- 20V/div)
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40Hz operation- steady state results
VAO
VAA‘
VAA‘
VA‘O
Ia
VCM
Icm
Trace 1- Phase voltage, trace 2- no load Trace1-pole voltage of Inverter I, trace 2-
phase current, trace 3- common mode phase voltage, trace 3 pole voltage of Inverter
current (X axis- 0.01s/div,Y axis- II, trace 4- common mode voltage (X axis-
20V/div,1A/div) 0.01s/div, Y axis- 40V/div)
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50Hz operation- steady state results
VAO
VAA‘
VAA‘
VA‘O
Ia
Icm VCM
Trace 1- Phase voltage, trace 2- no load Trace1-pole voltage of Inverter I, trace 2-
phase current, trace 3- common mode phase voltage, trace 3- pole voltage of
current (X axis- 0.01s/div,Y axis- Inverter II, trace 4- common mode voltage (X
20V/div,1A/div) axis- 0.01s/div, Y axis- 40V/div)
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Transient results
Phase voltage, no load phase current and Phase voltage, no load phase current
common mode current while the machine and common mode current during
is accelerated from 20Hz to 30Hz. speed reversal(-20Hz to 20Hz
Trace 1- Phase voltage, trace 2- phase Trace 1- Phase voltage, trace 2- phase
current, trace 3- common mode current (X current, trace 3- common mode current (X
axis- 0.05s/div,Y axis- 20V/div,1A/div) axis- 0.05s/div,Y axis- 20V/div,1A/div)
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Experimental results
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20Hz operation- steady state results
VA‘O VAA’
VAA‘ VBB’
VAO VCC’
Ia
VCM
Trace 1- pole voltage of Inverter II (X axis- Trace1-pole voltage of inverter I, trace 2-
10ms/div,Y axis- 50V/div), trace 2- pole phase voltage, trace 3- pole voltage of
voltage of Inverter II (X axis-10ms/div,Y inverter II, trace 4- common mode voltage (X
axis- 50V/div), trace 3-phase voltage(X axis- 0.01s/div, Y axis- 50V/div)
axis-10ms/div,Y axis- 100V/div), trace 4-
no load phase current(X axis-10ms/div,Y
axis- 1A/div)
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20 Hz FFT of the pole voltages and phase voltage
FFT of Pole voltage of inverter I FFT of Pole voltage of inverter II
(X axis-harmonic
order, Y axis-
Relative magnitude
normalized to the
phase voltage
fundamental)
FFT of phase voltage
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40Hz operation- steady state results
VA‘O VAA’
VAA‘ VBB’
VAO VCC’
Ia VCM
Trace 1- pole voltage of Inverter II (X Trace1-pole voltage of inverter I, trace 2- phase voltage,
axis-10ms/div,Y axis- 50V/div), trace 2- trace 3- pole voltage of inverter II, trace 4- common mode
pole voltage of Inverter II (X axis- voltage (X axis- 0.01s/div, Y axis- 50V/div)
10ms/div,Y axis- 50V/div), trace 3-phase
voltage (X axis-10ms/div,Y axis-
100V/div), trace 4- no load phase current
(X axis-10ms/div,Y axis- 1A/div)
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40 Hz FFT of the pole voltages and phase voltage
FFT of Pole voltage of inverter I FFT of Pole voltage of inverter II
(X axis-harmonic
order, Y axis-
Relative magnitude
normalized to the
phase voltage
fundamental)
FFT of phase voltage
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50Hz operation- steady state results
VA‘O VAA’
VAA‘ VBB’
VAO VCC’
Ia VCM
Trace 1- pole voltage of Inverter II (X Trace1-pole voltage of inverter I, trace 2- phase voltage,
axis-10ms/div,Y axis- 50V/div), trace 2- trace 3- pole voltage of inverter II, trace 4- common mode
pole voltage of Inverter II (X axis- voltage (X axis- 0.01s/div, Y axis- 50V/div)
10ms/div,Y axis- 50V/div), trace 3-phase
voltage (X axis-10ms/div,Y axis-
100V/div), trace 4- no load phase current
(X axis-10ms/div,Y axis- 1A/div)
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50 Hz FFT of the pole voltages and phase voltage
FFT of Pole voltage of inverter I FFT of Pole voltage of inverter II
(X axis-harmonic
order, Y axis-
Relative magnitude
normalized to the
phase voltage
fundamental)
FFT of phase voltage
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Triplen current in the phase current at the no load
current
Triplen current (trace 1) and phase current (trace 2) at
modulation index 1(X axis- 5ms/div,Y axis- 1A/div)
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Transient results – acceleration and Speed reversal
VAA‘
Ia
Phase voltage (trace 1- X axis- 5ms/div,Y Phase voltage (trace 1- X axis- 5ms/div,Y axis-
axis- 50V/div) and phase current (trace 2- 50V/div) and phase current (trace 2- X axis-
X axis- 5ms/div,Y axis- 1A/div) during 5ms/div,Y axis- 2A/div) during speed reversal
the acceleration from modulation index
0.4 to modulation index 0.8
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Salient features of the drive schemes
The scheme needs a conventional three- level NPC inverter on one side
and a two-level inverter.
The DC- link voltage requirement is only half compared to the
conventional schemes.
Only two isolated dc-links are needed.
The common mode voltage is suppressed in an average sense using sine-
triangle modulation technique.
Hence isolated power supplies are not needed.
Inverter II (the two-level inverter) is always in square wave operation
irrespective of the modulation index.
This scheme can be extended to higher level by only changing inverter I.
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Publications
S. Figarado, T. Bhattacharya, G. Mondal and K. Gopakumar, ―Three-level
inverter scheme with reduced power device count for an induction motor
drive with common-mode voltage elimination‖ IET Power Electron., 2008,
Vol. 1, No. 1, pp. 84–92.
Sheron Figarado, K. Gopakumar*, Gopal Mondal, K. Sivakumar,N.S
Dinesh, ‖Three-Level Inverter Fed Open- end Winding IM Drive with
Common Mode Voltage Elimination and Reduced Power Device Count‖
The 33rd Annual Conference of the IEEE Industrial Electronics Society
(IECON), Nov. 5-8, 2007, Taipei, Taiwan
Sheron Figarado, K. Sivakumar, Rijil Ramchand,Anandarup das,Chantan
Patel and K. Gopakumar, ―A Five-level inverter scheme for an open- end
winding Induction machine drive with less number of switches.‖ Accepted
in IET Power Electronics,UK.
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and Technology
Thank You
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