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Влияние ЭМИ от Электропривода

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energies
Article
The Effect of Distributed Parameters on Conducted
EMI from DC-Fed Motor Drive Systems in
Electric Vehicles
Li Zhai 1,2, *, Liwen Lin 1,2 , Xinyu Zhang 3 and Chao Song 1,2
1
2
3
*
National Engineering Laboratory for Electric Vehicle, Beijing Institute of Technology, Beijing 100081, China;
[email protected] (L.L.); [email protected] (C.S.)
Co-Innovation Center of Electric Vehicles in Beijing, Beijing Institute of Technology, Beijing 100081, China
Beijing Institute of Radio Metrology and Measurement, Beijing 100854, China; [email protected]
Correspondence: [email protected]; Tel.: +86-10-6891-5202
Academic Editor: Joeri Van Mierlo
Received: 18 August 2016; Accepted: 12 December 2016; Published: 22 December 2016
Abstract: The large dv/dt and di/dt outputs of power devices in DC-fed motor drive systems in
electric vehicles (EVs) always introduce conducted electromagnetic interference (EMI) emissions and
may lead to motor drive system energy transmission losses. The effect of distributed parameters on
conducted EMI from the DC-fed high voltage motor drive systems in EVs is studied. A complete test
for conducted EMI from the direct current fed(DC-fed) alternating current (AC) motor drive system in
an electric vehicle (EV) under load conditions is set up to measure the conducted EMI of high voltage
DC cables and the EMI noise peaks due to resonances in a frequency range of 150 kHz–108 MHz.
The distributed parameters of the motor can induce bearing currents under low frequency sine
wave operation. However the impedance of the distributed parameters of the motor is very high at
resonance frequencies of 500 kHz and 30 MHz, and the effect of the bearing current can be ignored,
so the research mainly focuses on the distributed parameters in inverters and cables at 500 kHz and
30 MHz, not the effect of distributed parameters of the motor on resonances. The corresponding
equivalent circuits for differential mode (DM) and common mode (CM) EMI at resonance frequencies
of 500 kHz and 30 MHz are established to determine the EMI propagation paths and analyze the
effect of distributed parameters on conducted EMI. The dominant distributed parameters of elements
responsible for the appearing resonances at 500 kHz and 30 MHz are determined. The effect of the
dominant distributed parameters on conducted EMI are presented and verified by simulation and
experiment. The conduced voltage at frequencies from 150 kHz to 108 MHz can be mitigated to
below the limit level-3 of CISPR25 by changing the dominant distributed parameters.
Keywords: electric vehicle; DC-fed; motor drive system; conducted electromagnetic interference
(EMI); distributed parameter
1. Introduction
In the face of the worldwide demand for reduction in greenhouse gas emissions and PM2.5
production [1], recently many countries have adopted policies, mainly in the form of tax incentives for
the purchase, to increase the number of electric vehicles (EVs) and thus reduce pollutant emissions
and improve the air quality, especially in urban areas [2–5]. Electromagnetic interference (EMI)
considerations in EVs have become increasingly important, as the electromagnetic compatibility (EMC)
regulations for EVs (typically defined from 10 kHz to 30 MHz) have become more stringent [6].
The DC-fed motor drive system of EVs, consisting of the electric motor, power inverter, and electronic
controller has an essential role in EVs [7]. Large dv/dt and di/dt due to high-speed switching of power
devices within a DC-fed voltage-type pulse width modulation (PWM) inverter of high-power-density
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and high-efficiency motor drive system always introduce unwanted higher-order harmonics currents
and high frequency noise currents through parasitic/distributed parameters of the motor system [8–10],
and are mainly responsible for the conducted and/or radiated electromagnetic interference (EMI)
emissions which will greatly affect the behavior of low voltage supply electronic equipment (such as
board bus system, sensors, vehicle control units (VCUs), battery management systems (BMSs), power
batteries, and the drive motor in EVs [6,11]. Additionally, the unwanted higher-order harmonics
current from the motor drive system due to the switching of insulated gate bipolar transistors (IGBTs)
can not only generate common mode (CM) EMI and differential mode (DM) EMI emissions, but also
increase the motor losses, which may lead to energy transmission losses and thermal problems in the
power inverter system.
1.1. Literature Review
Much valuable work involving the EMI emissions of the motor drive system for conventional
industrial applications has been widely conducted by many researchers [12–14]. However, the EMI
from the drive motor system under varying load conditions for EVs is different from that of a
conventional industrial motor with no load or invariant load conditions. Previous studies on EMI
emissions from vehicle components are based on the measurements specified in the EMC standard
CISPR25 (International Special Committee on Radio Interference 25) [15,16], which are implemented
for low voltage components in EVs and not suitable for the high voltage applications in EVs (e.g., motor
system, charging system), so we cannot correctly predict the EMI emissions from the high voltage
motor system in EVs due to the fact few EMC laboratories have the dynamometer needed to study
EVs under varying loading conditions, so the present study on the EMI mechanism and propagation
path of the motor system is much less than that on the total EMC performance of EVs [17,18]. The EMI
emissions from the high voltage cables of the AC motor drive system of EVs under load condition
have not been considered in previous works.
Various parasitics and distributed parameters exist inside the motor system and they play a very
important role in the generation of EMI. The high-frequency leakage currents flowing to the ground
could be generated through distributed parameters between the components of the motor drive system
(such as the motor, inverter, cables, etc.) and the chassis of the body of the EV at high frequency,
and introduce the radiation of power cables, shaft voltage and bearing currents in the motor [19,20].
Additionally the EMI emission peaks due to resonances caused by distributed parameters may cause
some energy losses of the motor drive system and decrease the efficiency of the system [21–23], so the
distributed parameters at high frequency in the system should not be neglected anymore for EVs.
Therefore, the effect of the distributed parameters on EMI emissions is important for identification
of EMI propagation paths and the critical distributed parameters of elements responsible for EMI,
and mitigation of EMI emissions [24].
Models of the motor drive system are necessary to analyze and predict the EMI sources and
propagation inside the motor drive system to find the elements responsible for the EMI. Since the
most basic and widely applied full-wave models based on the “black box” approach cannot show
the location of the noise source or the propagation path inside the motor power inverter [20,25],
some terminal modeling techniques for a two-port network were proposed to predict the conducted
EMI [14,21,26]. However, there has never been a theoretical analysis of the parasitic effects of the
distributed parameters on EMI noise suppression. An equivalent simulation program with integrated
circuit (SPICE)-based model is a better approach to find the parts and elements of the motor inverter
system responsible for EMI [12] and analyze the effects of the distributed parameters on the EMI noise.
A rather simple measurement-based SPICE model of the motor power inverter has been presented [12]
to quickly identify the parts responsible for EMI and help predict resonances between the two ports
of the motor power inverter by a straightforward correlation between the system geometry and the
parasitic circuit elements [27]. A detailed analysis of current paths and the equivalent circuits at three
important resonance frequencies have been presented to determine the EMI propagation path in the
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motor drive system [6]. A combination of mitigation strategies was designed to mitigate the CM
conducted emission by IGBT switching and the radiated emissions of AC cables.
Most of the above work focuses on analyses of CM and DM EMI propagation paths in the system
based on a “black box” approach, terminal modeling techniques and SPICE-based models, which have
not considered the effect of the distributed parameters of the high voltage motor drive system in EVs on
EMI noise, so the previous equivalent circuits of the EMI could not be correctly proposed to accurately
and effectively predict the actual source and propagation of the EMI in the system. The effects of the
distributed parameters on the conducted EMI noise have not been adequately considered previously
because of a lack of the modeling of the conducted EMI from the high voltage motor drive system with
suitable parameters and better analysis methods.
1.2. Motivation and Innovation
This study proposes a new method to analyze the effect of distributed parameters on conducted
EMI from the DC-fed high voltage motor drive systems in EVs. A complete test for conducted EMI
emissions from the AC motor drive system of an EV under load conditions will be set up to measure the
conducted EMI of high voltage DC cables and EMI noise peaks due to resonances in a frequency range
of 150 kHz–108 MHz. The corresponding equivalent circuits for DM and CM EMI at the resonance
frequencies of 500 kHz and 30 MHz are established to determine the EMI propagation paths and
analyze the effect of distributed parameters on conducted EMI. The dominant distributed parameters
of elements responsible for the resonances appearing at 500 kHz and 30 MHz will be determined.
The effect of the dominant distributed parameters on conducted EMI will be verified by simulations
and experiments.
1.3. Organization of the Paper
The organization of this study is as follows: Section 2 illustrates the structure of the complete test
setup for conducted EMI emissions from the AC motor drive system of an EV. Then, the corresponding
current paths and equivalent circuits of DM and CM EMI at resonance frequencies of 500 kHz and
30 MHz, and the effect of distributed parameters on CM EMI will be presented in Section 3. After that,
the simulation verification and discussion will be illustrated in Section 4. The experiment verification
will be discussed in Section 5. Finally, conclusions are provided in Section 6.
2. System Conducted Emission Measurement
2.1. Conducted EMI Emission Setup
The complete test setup for conducted EMI emissions from the DC-fed AC motor drive system
on an EV in an EMI laboratory is shown in Figure 1 and mainly consists of a DC power supply
such as a Li-ion battery, DC cables, a DC-fed voltage-type PWM three-phase power inverter, AC
cables, and an AC motor. Measurements were performed to comply with the CISPR 25 standard
which provides conducted EMI emission limits for vehicle components in a frequency range of 150
kHz to 108 MHz [28]. Two standard line impedance stabilization networks (LISNs) terminated with
50 Ω resistances provide DC power from a battery or DC power supply to the three-phase power
inverter using two shielded cables (2 m). The power inverter with 330 V DC input is connected to
a 50 kW/100 kW permanent magnet synchronous motor (PMSM) using three shielded cables (1 m).
As required by the EMC regulations of CISPR 25, all components are connected to a large copper
sheet as ground reference plane, except for the AC motor which is located on an insulated bench
covered with ferrite material and connected to an electric dynamometer supplying a mechanical load.
The output speed and torque of the AC motor can be measured by a meter between the dynamometer
and the insulated output shaft of the AC motor. With this configuration, the total conducted EMI noise
voltage signals in DC cables can be picked up by any one of the line impedance stabilization network
(LISN) impedances connected to an EMI receiver [29].
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Figure 1. Conducted EMI emission system test setup for the AC motor drive system.
Figure 1. Conducted EMI emission system test setup for the AC motor drive system.
2.2. Conducted EMI Experiment Results
Figure
1. Conducted
EMI emission system test setup for the AC motor drive system.
2.2. Conducted EMI
Experiment
Results
1. Conducted
emission system
test setup
for the AC
motor
driveand
system.
The ACFigure
motor
is operatedEMI
continuously
at 2000
rpm speed
with
no-load
60 N·m loaded
The
ACasmotor
is Experiment
operated
continuously
at 2000
rpm speed with
no-load
60 N·mEMI
loaded
2.2.
Conducted
EMI
Results
torque,
shown
in
Figure 2.
Figure 3 shows
the experimental
comparison
in and
conducted
2.2.
EMI
Experiment
Resultsand load conditions. This experimental result indicates that the
emission
levels
between
the
no-load
torque,
asConducted
shown
in
Figure
2.
Figure
3
shows
the
experimental
comparison
in
conducted
EMI
emission
The AC motor is operated continuously at 2000 rpm speed with no-load and 60 N·m loaded
conducted
EMI
noiseis voltage
of continuously
the
power inverter
is rpm
dominant
aresult
frequency
range
ofN·m
150
kHz
to
TheasAC
motor
operated
atThis
2000
speedinwith
no-load
and
60
levelstorque,
between
the
no-load
and load
conditions.
indicates
that
theloaded
conducted
shown
in Figure
2. Figure
3 shows
theexperimental
experimental
comparison
in conducted
EMI
108
MHz
and
is
not
compliant
with
CISPR25,
as
shown
in
Table
1.
Therefore
the
conducted
EMI
torque,
aslevels
shown
in power
Figure
2. Figure
shows
theinexperimental
comparison
conducted
EMI
EMI noise
voltage
ofbetween
the
inverter
is3dominant
a frequency
range of
150inindicates
kHz
to 108
emission
the no-load
and
load
conditions.
This experimental
result
thatMHz
the and
emission levels
levels between
in the load
areload
more
severe and
higher
than those
in the
no-loadthat
mode.
the condition
no-load
and
conditions.
This
experimental
result
indicates
is notemission
compliant
with
CISPR25,
asthe
shown
ininverter
Table
1.
conducted
EMI
conducted
EMI
noise
voltage
of
power
is Therefore
dominant
inthe
a frequency
range
of emission
150 kHzthe
tolevels
Two noise voltage
peaks
at frequency
around
500 kHz
and 30 MHz
can
be observed
and
may
mainly
conducted
EMI
noise
voltage
of
the
power
inverter
is
dominant
in
a
frequency
range
of
150
kHz
to
MHz
and is not
withand
CISPR25,
shown
in Table
Therefore
the conducted
in the108
load
condition
arecompliant
more severe
higherasthan
those
in the1.no-load
mode.
Two noiseEMI
voltage
be caused
by PWM
switching harmonics
or parasitic
resonances
due1.toTherefore
the distributed
parameters
of
108
MHz levels
and
isinnot
with CISPR25,
shown
inhigher
Table
EMI
thecompliant
load
condition
are
more as
severe
and
thanmay
those
inthe
theconducted
no-load
mode.
peaksemission
at
frequency
around
500
kHz
and
30
MHz
can
be
observed
and
mainly
be
caused
by
the
motor
system
[30].
It
is
critical
to
analyze
the
source
and
propagation
mechanism
of
EMI
toPWM
emission
levels
in peaks
the load
condition around
are more
severe
and30
higher
than
those
in theand
no-load
mode.
Two
noise
voltage
at
frequency
500
kHz
and
MHz
can
be
observed
may
mainly
switching
harmonics
or parasitic
resonances
to kHz
the distributed
parameters
of parameters
the
motor
system
predict
thevoltage
conducted
EMI
emissions
anddue
determine
the 30
dominant
distributed
of the [30].
Two
noise
at frequency
around
500
and
MHz
be observed
and
may mainly
be caused
by PWMpeaks
switching
harmonics
or parasitic
resonances
duecan
to the
distributed
parameters
of
It is critical
to
analyze
the
source
and
propagation
mechanism
of
EMI
to
predict
the
conducted
EMI
elements
in
the
motor
system
responsible
for
the
resonances.
be
PWM[30].
switching
harmonics
or parasitic
resonances
to the distributed
parameters
thecaused
motor by
system
It is critical
to analyze
the source
and due
propagation
mechanism
of EMI of
to
emissions
and
determine
the
dominant
distributed
parameters
of
the
elements
in
the
motor
system
the
motor
[30]. EMI
It is emissions
critical to and
analyze
the source
and propagation
mechanism
of EMI
to
predict
thesystem
conducted
determine
the dominant
distributed
parameters
of the
responsible
for
the
resonances.
predict
the
conducted
EMI
emissions
and
determine
the
dominant
distributed
parameters
of
the
elements in the motor system responsible for the resonances.
elements in the motor system responsible for the resonances.
Figure 2. The test platform for conducted EMI emission.
Figure 2. The test platform for conducted EMI emission.
Figure
2. 2.The
for conducted
conductedEMI
EMI
emission.
Figure
Thetest
testplatform
platform for
emission.
Figure 3. Comparison of measurement with load and measurement without load.
Figure 3. Comparison of measurement with load and measurement without load.
Figure
3. Comparison
ofofmeasurement
withload
loadand
andmeasurement
measurement
without
Figure
3. Comparison
measurement with
without
load.load.
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Table 1. CISPR25 class3-peak limits for conducted disturbances.
Service Band
Frequency/MHz
Limit/dB (µv)
Broadcast
0.15–0.30
0.53–1.80
5.9–6.2
41–88
76–108
90
70
65
46
50
Mobile services
26–28
30–54
68–87
56
56
50
3. System Conducted Emission Analysis
3.1. Noise Source
Figure 1 shows the circuit of a full bridge IGBT-based inverter in the motor controller model.
The DC-fed PWM power inverter is designed to have a rated 250 V output voltage. The DC bus
input voltage is 330 V. The six switches S1 –S6 in the inverter are 1200 V/600 A full bridge IGBT
modules (Infineon) with sinusoidal pulse width-modulation (SPWM) control. Although control
methods (like space vector pulse width modulation (SVPWM), direct torque control (DTC), indirect
field oriented control (IFOC), etc.) have better characteristics for mitigating harmonics, this is not the
case for the EMI noise at high frequency. Therefore, we focus on the effect of characteristics of the
trapezoidal wave for PWM on the EMI. We just take SPWM as an example for explaining the principle
of the spectrum of the trapezoidal wave. The switching frequency of IGBT was set to 20 kHz and the
line frequency for the AC motor was 400 Hz. The SPWM control signals are generated by compared a
sinusoidal reference with a 20 kHz triangular carrier signal as illustrated in Figure 4a, which shows
the PWM waveforms in a half-period, which have nine duty cycles corresponding to nine pulses with
different pulse-widths. The noise source due to the SPWM control is often simplified by assuming a
trapezoidal shape for the switching transients [26]. Each PWM pulse can be described as a trapezoidal
pulse by an amplitude A, a frequency f, a pulse rise-time τr , a pulse fall-time τ f and a pulse-wide τ.
T represents the period of the trapezoidal pulse. The continuous envelope spectrum for a trapezoidal
pulse can be given by the following equations [31]:
Envelope = 2A
τ sin(πτ f ) sin(πτr f )
T
πτ f
πτr f
20 log10 (envelope) = 20 log10 (2A Tτ ) + 20 log10 (
(πτr f )
)
+20 log10 ( sinπτ
rf
(1)
sin(πτ f )
πτ f )
(2)
The τ is smaller under unloaded operation conditions than that under load operation by SPWM
control, as shown in Figure 4. Then from (1) and (2) the magnitude of the EMI noise voltage decreases
as the value of τ decreases, and is lower under unloaded operation than that under load operation.
From (1) and (2), the first break point in the frequency spectral bound is related to τ and is 1/πτ.
The higher the τ, the wider the span related to the DC term, as shown in Figure 4b. The τ is smaller
under unloaded operation conditions. Then the magnitude of the EMI noise voltage is lower under
unloaded operation than that under load operation, as shown in Figure 3. The second breakpoint in
the frequency spectral bound is related to rise/fall time and is 1/πτr .The smaller the rise/fall time,
the larger the high-frequency spectral content, as shown in Figure 4c. The frequency band of the EMI
noise source due to IGBT switching is from 0 Hz to 1 GHz. Then the resonances could be caused up to
1 GHz by parasitic distributed parameters of the AC motor system and may result in peak voltages
exceeding the limit levels specified in the CISPR25 standard, as shown in Table 1.
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result
voltages exceeding the limit levels specified in the CISPR25 standard, as shown in 6 of 17
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2017,in
10,peak
1
Table 1.
1
1
2
3
4
5
6
7
8
9
10
11
12
13 14
15
16
17 18
0.5
0
-0.5
-1
0
0.2
0.4
0.6
0.8
Time/(s)
1
1.2
1.4
1.6
-3
x 10
(a)
1
0.5
0
-0.5
-1
0
0.2
0.4
0.6
0.8
Time/(s)
1
1.2
1.4
1.6
-3
x 10
1.2
1.4
1.6
-3
x 10
1
0.5
0
-0.5
-1
0
0.2
0.4
0.6
0.8
Time/(s)
1
(b)
(c)
Figure 4. Spectral bounds for a trapezoidal wave: (a) SPWM in half-period; (b) The effect of
Figure
4. Spectral bounds for a trapezoidal wave: (a) SPWM in half-period; (b) The effect of pulse-width;
pulse-width; (c) The effect of rise-time.
(c) The effect of rise-time.
3.2. Analysis of the Current Path of Conducted Emissions
3.2. Analysis of the Current Path of Conducted Emissions
The self-inductance and mutual inductance are equivalent to one inductance in order to simplify
the equivalent circuit for analyzing EMI propagation path. The motor drive system is constructed
in DM and CM situation, as shown in Figure 5 and Figure 7, where, S1 –S6 represent six IGBTs in
the inverter, C1 –C6 represent the distributed capacitance between the collector and emitter of S1 –S6 ,
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The
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2017,self-inductance
10, 1
and mutual inductance are equivalent to one inductance in order
to
7 of 17
simplify the equivalent circuit for analyzing EMI propagation path. The motor drive system is
constructed in DM and CM situation, as shown in Figures 5 and 7, where, S1–S6 represent six IGBTs
CY1 and CY2 represent the filter Y capacitors between the positive/negative DC cable and chassis,
in the inverter, C1–C6 represent the distributed capacitance between the collector and emitter of S1–
LY1 and LY2 represent the equivalent series inductances (ESLs) of CY1 and CY2 , CX represents the
S6, CY1 and CY2 represent the filter Y capacitors between the positive/negative DC cable and chassis,
filter X capacitor between the DC buses, LX represents the equivalent series resistance (ESR) of CX .
LY1 and LY2 represent the equivalent series inductances (ESLs) of CY1 and CY2, CX represents the filter
Two LISNs can be represented by the circuit composed of RL1 , CL1 , RL2 , CL2 , C7 , C8 and C9 to represent
X capacitor between the DC buses, LX represents the equivalent series resistance (ESR) of CX. Two
the distributed capacitance from the collector and emitter of the IGBT to the chassis, C10 represents the
LISNs can be represented by the circuit composed of RL1, CL1, RL2, CL2, C7, C8 and C9 to represent the
distributed
motor and
chassis.
LM IGBT
represents
inductance
of the motor
distributedcapacitance
capacitancebetween
from thethe
collector
andthe
emitter
of the
to thethe
chassis,
C10 represents
the
phase
winding,
L
and
L
represent
the
DC
bus
bars’
inductance,
which
includes
DC bus bar+
bar− and the chassis. LM represents the inductance
distributed capacitance
between DC
thebusmotor
of the
self-inductance
and mutual
inductance
between two DC bus bars, so its value is larger than that of the
motor phase winding,
LDC bus
bar+ and LDC bus bar− represent the DC bus bars’ inductance, which includes
lead
stray
inductance
of
IGBT,
which
is
smaller
andtwo
can DC
be ignored,
compared
the inductance
of the
self-inductance and mutual inductance between
bus bars,
so its value
is larger than
thatDC
of
bus
bars.
C
and
C
represent
the
DC
cables’
capacitance,
L
and
L
represent
the
DC
cables’
DC+
DC
−
DC+
DC
−
the lead stray inductance of IGBT, which is smaller and can be ignored, compared the inductance of
inductance,
RDC1 Cand
RDC2 represent the DC cables’ resistance. The main distributed parameters’
the DC bus bars.
DC+ and CDC− represent the DC cables’ capacitance, LDC+ and LDC− represent the DC
values
are
measured
by
in Table
EMI noise
propagation
pathsdistributed
based on
cables’ inductance, RDC1VNA
and and
RDC2shown
represent
the 2.DCThe
cables’
resistance.
The main
distributed
parameters
and
the
equivalent
circuits
of
DM
and
CM
noise
current
are
respectively
parameters’ values are measured by VNA and shown in Table 2. The EMI noise propagation paths
presented
follows. parameters and the equivalent circuits of DM and CM noise current are
based on as
distributed
respectively presented as follows.
Table 2. Parameters in the motor drive system.
Parameter
Table Value
2. Parameters in the motor
drive system.
Parameter
LY1 , LY2 Parameter
LY1, LY2
C7
C7
C8
C8
C9
C9
C10
C10
CY1 , CY2
LDC+ , LDC− CY1, CY2
RDC+ , RDC−LDC+, LDC−
RDC+, RDC−
200 nHValue
30 pF200 nH
20 pF 30 pF
20 pF 20 pF
200 pF 20 pF
100 pF200 pF
50 nH100 pF
0.0002 Ω50 nH
0.0002 Ω
Parameter
CX
CX
LX
LX6
C1 –C
–CL2
6
RL1C,1R
RL1
, RL2
CL1
,C
L2
CLL1, CL2
M
CDC+ , LCMDC−
CDC+
DC−
LDC bus bar+
, L, C
DC bus bar−
LDC bus bar+, LDC bus bar−
Value
Value
1028 µF
1028 µF20 nH
20 nH 20 pF
20 pF 50 Ω
50 Ω0.47 µF
0.47 µF1 mH
1 mH100 nF
100 nF104 nH
104 nH
3.2.1. Analysis of the DM Current Path for 500 kHz
3.2.1. Analysis of the DM Current Path for 500 kHz
The DM EMI emission from the phase node P between the two IGBTs of one phase bridge leg
The DM EMI emission from the phase node P between the two IGBTs of one phase bridge leg
can be equivalent to a DM noise current source IDM between the phase node P and DC bus minus the
can be equivalent to a DM noise current source IDM between the phase node P and DC bus minus the
distributed parameters of the inner elements of the motor system, as shown in Figure 5a. The DM
distributed parameters of the inner elements of the motor system, as shown in Figure 5a. The DM
current loop can be illustrated by calculating the impedance of each circuit element ignoring the
current loop can be illustrated by calculating the impedance of each circuit element ignoring the
distributed parameters at 500 kHz, so the DM current flows though the distributed parameters of
distributed parameters at 500 kHz, so the DM current flows though the distributed parameters of the
the motor system is shown in Figure 5b. IDM acts as a driving force to form the following three
motor system is shown in Figure 5b. IDM acts as a driving force to form the following three current
current loops:
loops:
•
current loop I: IDM →C4 →LDC bus bar− →RDC2 →LX →CX →RDC1 →LDC bus bar+ →C1 →IDM
•
current loop I: IDM→C4→LDC bus bar−→RDC2→LX→CX→RDC1→LDC bus bar+→C1→IDM
•
current loop II: IDM →LM →C6 →LDC bus bar− →RDC2 →LX →CX →RDC1 →LDC bus bar+ →C1 →IDM
•
current loop II: IDM→LM→C6→LDC bus bar−→RDC2→LX→CX→RDC1→LDC bus bar+→C1→IDM
•• current
→LM →C2 →L busbus
→→L
RDC2 →LX →CX →RDC1 →LDC bus bar+ →C1 →IDM
bar−DC2
current loop
loop III:
III: IIDM
DM→LM→C2→LDCDC
bar−→R
X→CX→RDC1→LDC bus bar+→C1→IDM
IDM
(a)
(b)
Figure 5.
5. (a)
(a) Equivalent
Equivalent circuit
circuit for
for DM;
DM; (b)
(b) DM
DM interference
interference propagation
propagation path
path at
at 500
500kHz.
kHz.
Figure
Energies 2016, 10, 1
8 of 17
Energies 2017, 10, 1
8 of 17
3.2.2. Analysis of DM Current Path for 30 MHz
The impedance
of each circuit
element
at 30 MHz is calculated as shown in Figure 6. IDM acts as
3.2.2. Analysis
of DM Current
Path for
30 MHz
a driving force to form the following three current loops at 30 MHz:
The impedance of each circuit element at 30 MHz is calculated as shown in Figure 6. IDM acts as a
•
current loop I: IDM→C4→LDC bus bar−→RDC2→LX→CX→RDC1→LDC bus bar+→C1→IDM
driving
force
to form the following three current loops at 30 MHz:
•
current loop II: IDM→C4→C6→C3→C1→IDM
•
•
•
•
current loop III: IDM→C4→C2→C5→C1→IDM
current
loop I: I →C4 →LDC bus bar− →RDC2 →LX →CX →RDC1 →LDC bus bar+ →C1 →IDM
Energies 2016, 10, 1DM
8 of 17
The loop
harmonic
content
ofCthe
DM current at 500 kHz and 30 MHz flowing through the 50 Ω
current
II: IDM
→C4 →
6 →C3 →C1 →IDM
impedance
of LISN
is
also
very smallfor
the filtering effect of the X capacitor. Then the resonant
3.2.2. loop
Analysis
DM
→Current
C4 →C2Path
→C5due
→30CtoMHz
current
III: of
IDM
1 →IDM
peak at about 500 kHz and 30 MHz is not dominated by the DM current.
The impedance of each circuit element at 30 MHz is calculated as shown in Figure 6. IDM acts as
a driving force to form the following three current loops at 30 MHz:
•
•
•
current loop I: IDM→C4→LDC bus bar−→RDC2→LX→CX→RDC1→LDC bus bar+→C1→IDM
current loop II: IDM→C4→C6→C3→C1→IDM
current loop III: IDM→C4→C2→C5→C1→IDM
The harmonic content of the DM current at 500 kHz and 30 MHz flowing through the 50 Ω
impedance of LISN is also very small due to the filtering effect of the X capacitor. Then the resonant
peak at about 500 kHz and 30 MHz is not dominated by the DM current.
Figure6.6.DM
DMinterference
interference propagation
at at
30 30
MHz.
Figure
propagationpath
path
MHz.
3.2.3. Analysis of CM Current Path for 500 kHz
The harmonic content of the DM current at 500 kHz and 30 MHz flowing through the 50 Ω
TheofCM
noise
is always
generated
high frequency
and
through the
distributed
impedance
LISN
is current
also very
small due
to theatfiltering
effect of
theflows
X capacitor.
Then
the resonant
parameters to the ground [32]. The CM emission from the phase node P of two IGBTs of one phase
peak at about 500 kHz and 30 MHz is not dominated by the DM current.
bridge leg can be equivalent to a CM voltage source UDM between the phase node P and chassis with
ignored distributed parameters of inner elements of the motor system, as shown in Figure 7a,b. The
3.2.3. Analysis of CM Current Path for 500 kHz
CM current loop can be illustrated
calculating
the impedance
of each circuit element with
Figure 6. DMby
interference
propagation
path at 30 MHz.
The CM noise
currentatis500
always
high force
frequency
flows
through
the shown
distributed
distributed
parameters
kHz. Ugenerated
CM acts as a at
driving
to formand
three
CM current
loops
3.2.3.to
Analysis
of current
CM Current
Path
for
500 kHz
in Figure
7c,
where
loop1
(red
line),
currentfrom
loop2
(blue
line)node
and current
loop3
(purple
line)phase
parameters
the
ground
[32].
The
CM
emission
the
phase
P of two
IGBTs
of one
areleg
considered
parallel.
The
current
flowing
pathsU
at
500
kHz
are
composed
of
a
DC
side
path
The be
CMin
noise
current
generated
at high
frequency
and
flows
through
the
distributed
bridge
can
equivalent
toisCM
aalways
CM
voltage
source
between
the
phase
node
P
and
chassis
DM
and
an
AC
side
path.
The
effective
impedance
of
inductance
for
one
branch
of
the
current
loop
(red)
parameters
to
the
ground
[32].
The
CM
emission
from
the
phase
node
P
of
two
IGBTs
of
one
phase
with ignored distributed parameters of inner elements of the motor system, as shown in Figure 7a,b.
dominatedleg
by LDCbe
busequivalent
bar+ or LDC bus
is voltage
about j0.32
ΩU
and
the effective
impedance
capacitance
to abar−
CM
source
DM between
the phase
P of
and
chassis withfor
The CMbridge
current can
loop can
be illustrated
by calculating
the impedance
ofnode
each
circuit
element with
parameters
of inner
elements of
system,
as shown inisFigure
TheΩ.
oneignored
branchdistributed
of the current
loop (red)
dominated
bythe
themotor
DC cable
capacitance
about7a,b.
−j0.32
distributed
parameters
at
500
kHz.
U
acts
as
a
driving
force
to
form
three
CM
current
loops
shown
CM current
loopvoltage
can beatillustrated
calculating
impedance
of each
circuit element
with
Therefore
the peak
aboutCM
500 by
kHz
is mainlythe
caused
by the series
resonance
in the current
in Figure
7c, where
current loop1
(redUline),
current
loop2
(blue
line)
andCM
current
(purple line)
parameters
at 500 kHz.
CM acts
as a driving
force
to form
three
currentloop3
loops shown
loopdistributed
(red).
are considered
The CM
current
flowing
500line)
kHz
arecurrent
composed
of a DC
side path
in Figurein
7c,parallel.
where current
loop1
(red line),
currentpaths
loop2 at
(blue
and
loop3 (purple
line)
are
considered
in
parallel.
The
CM
current
flowing
paths
at
500
kHz
are
composed
of
a
DC
side
path
and an AC side path. The effective impedance of inductance for one branch of the current loop (red)
and by
an AC
path. The effective impedance of inductance for one branch of the current loop (red)
dominated
LDCside
bus bar+ or LDC bus bar− is about j0.32 Ω and the effective impedance of capacitance
dominated by LDC bus bar+ or LDC bus bar− is about j0.32 Ω and the effective impedance of capacitance for
for one branch of the current loop (red) dominated by the DC cable capacitance is about −j0.32 Ω.
one branch of the current loop (red) dominated by the DC cable capacitance is about −j0.32 Ω.
Therefore
the peak
at about
500500
kHz
causedbyby
series
resonance
the current
Therefore
the voltage
peak voltage
at about
kHzisismainly
mainly caused
thethe
series
resonance
in the in
current
loop (red).
loop (red).
(a)
(b)
(a)
(b)
Figure 7. Cont.
Energies 2016, 10, 1
Energies 2017, 10, 1
9 of 17
9 of 17
Energies 2016, 10, 1
9 of 17
(c)
(c)
Figure 7. (a) Equivalent circuit for CM; (b) Equivalent circuit for CM; (c) CM interference
Figure
7.7.(a)(a)
Equivalent
circuit
for CM;
Equivalent
circuit forcircuit
CM; (c)
CM
interference
Figurepropagation
Equivalent
circuit
for (b)
CM;
(b) Equivalent
for
CM;
(c) CM propagation
interference
path at 500 KHz.
path
at 500 KHz.
propagation
path at 500 KHz.
The elements responsible for the resonance at 500 kHz mainly are the capacitance between the
DC
cables
andresponsible
the chassis, and
inductance
of
thekHz
DC bus
bar ofare
IGBT.
resonance peak
Theelements
elements
forthe
thestray
resonance
at 500
500
mainly
theThe
capacitance
between the
the
The
responsible
for
the
resonance
at
kHz
mainly
are
the
capacitance
between
at about 500 kHz is mainly dominated by the CM current. The effect of the current loop2 (blue line)
DCcables
cablesand
and the
thechassis,
chassis, and
and the
the stray
stray inductance
inductance of
of the
the DC
DC bus
bus bar
bar of
of IGBT.
IGBT. The
The resonance
resonance peak
peak
DC
and current loop3 (purple line) is smaller and can be ignored in the equivalent circuit of CM current
atabout
about
500kHz
kHz
mainly
dominated
bythe
theCM
CM current.
current. The
The effect
effect of
of the
the current
current loop2
loop2 (blue line)
at
kHz
isismainly
dominated
by
at500
500
shown
in Figure
8.
andcurrent
currentloop3
loop3(purple
(purpleline)
line)isissmaller
smallerand
andcan
canbebeignored
ignored
the
equivalent
circuit
CM
current
and
inin
the
equivalent
circuit
of of
CM
current
at
at 500
kHz
shown
in Figure
500
kHz
shown
in Figure
8. 8.
I1
I1I
2
I
2
Figure 8. Equivalent circuit of CM interference at 500 KHz.
The CM current at about 500 kHz flowing on LISN can be expressed by the following equation:
Z 1U CM
lim
I1 =
x→ ∞
Figure
8.
Equivalent
circuit
of
CM interference
at 500 KHz.
(
Z
ZCM
Figure 8. Equivalent circuit1 +of
2 ) Z 3interference at 500 KHz.
(3)
where Z1 denotes series-parallel impedance of RL1, CL1 and CDC+, Z2 denotes series impedance of LDC
The
CM DC1
current
at about
500 kHz
flowing
on of
LISN
can be
expressed by the following equation:
bus CM
bar+, Rcurrent
and Cat
1, Z
3 denotes
series
impedance
RL1 can
and C
The
about
500the
kHz
flowing
on LISN
beL1.expressed by the following equation:
Z 1U CM
= Z U
lim
I 1 MHz
3.2.4. Analysis of CM Current Path for 30
(3)
CM) Z x → ∞
I1 = ( Z 11+ Z
(3)
2
3 lim
x →∞ shown in Figure 9. It is difficult to
Z2 ) Z3 loops
UDM acts as a driving force to form the( ZCM
1 +current
where determine
Z1 denotes
impedance
of Relements
L1, CL1 and
CDC+, Zfor
2 denotes
series at
impedance
theseries-parallel
main CM current
loop and the
responsible
the resonance
30 MHz of LDC
where
Z
series-parallel
impedance
of RL1 ,circuit
CL1
, Z denotes series impedance of
1 denotes
because
complexity
CM
current
equivalent
dominated
bus bar+, R
DC1
andofCthe
1, Z
3 denotesof
the
series
impedance
of
RL1and
andCCDC+
L1. by 2C1, C4, LDC bus bar+ , LDC bus bar−,
DC2,, R
, Rand
DC2, LC
DC+
LDC−
, CY1, LY1, the
CY2, series
LY2, C7,impedance
C8 and C9. The
of the
LDC bus R
RDC1
of model
RL1 and
CL1CM
. current equivalent
DC1
1, Z
3 denotes
bar+
circuit is of
essential
to studyPath
the main
CM current loop at 30 MHz to determine the
3.2.4. Analysis
CM Current
for 30dominated
MHz
distributed
responsible
resonance peak at 30 MHz.
3.2.4. Analysis
of parameters
CM Current
Path forfor30the
MHz
The as
equivalent
circuit
of CM
at 30CM
MHz
is shown
in Figure
10 and
CM current
30
UDM acts
a driving
force
to current
form the
current
loops
shown
in the
Figure
9. It isat difficult
to
UDM
acts
as a through
drivingthe
force
toresistor
form can
thebeCM
current
loops
shownequation:
in Figure 9. It is difficult to
MHz
flowing
LISN
expressed
by
the
following
determine the main CM current loop and the elements responsible for the resonance at 30 MHz
determine the main CM current loop and the elements responsible for the resonance at 30 MHz because
because of the complexity of CM current equivalent circuit dominated by C1, C4, LDC bus bar+ , LDC bus bar−,
of the complexity of CM current equivalent circuit dominated by C1 , C4 , LDC bus bar+ , LDC bus bar− ,
RDC2, RDC1, RDC2, LDC+, LDC−, CY1, LY1, CY2, LY2, C7, C8 and C9. The model of the CM current equivalent
RDC2 , RDC1 , RDC2 , LDC+ , LDC− , CY1 , LY1 , CY2 , LY2 , C7 , C8 and C9 . The model of the CM current
circuit is essential to study the main dominated CM current loop at 30 MHz to determine the
equivalent circuit is essential to study the main dominated CM current loop at 30 MHz to determine
distributed parameters responsible for the resonance peak at 30 MHz.
the distributed parameters responsible for the resonance peak at 30 MHz.
The equivalent circuit of CM current at 30 MHz is shown in Figure 10 and the CM current at 30
MHz flowing through the LISN resistor can be expressed by the following equation:
I2 =
Z1UCM
(Z1 + ZC1 )(Z2 + Z3 )Z4
(4)
Z1 denotes series-parallel impedance of C8, LDC bus bar+, RDC1, LDC+, CY1, LY1, CL1and RL1. Z2 denotes
Energies
2016, 10, 1 of LDC bus bar+ and RDC1. Z3 denotes series-parallel impedance of LDC+, CL1, RL1, CY110and
of 17
series
impedance
Energies 2017, 10, 1
10 of 17
LY1. Z4 denotes series impedance of LDC+, CL1 and RL1.
I2 =
Z1UCM
(Z1 + ZC1 )(Z2 + Z3 )Z4
(4)
Z1 denotes series-parallel impedance of C8, LDC bus bar+, RDC1, LDC+, CY1, LY1, CL1and RL1. Z2 denotes
series impedance of LDC bus bar+ and RDC1. Z3 denotes series-parallel impedance of LDC+, CL1, RL1, CY1 and
LY1. Z4 denotes series impedance of LDC+, CL1 and RL1.
Figure
Figure 9.
9. CM
CM interference
interference propagation
propagation path at 30 MHz.
The equivalent circuit of CM current at 30 MHz is shown in Figure 10 and the CM current at
30 MHz flowing through the LISN resistor can be expressed by the following equation:
I3
Z1 UCM
( Z1 + ZC1
)( Z2 + Z3 )path
Z4 at 30 MHz.
Figure 9. CM interference
propagation
I2 =
(4)
I4
I3
Figure 10. Equivalent circuit of CM interference at 30 MHz.
From Equation (3), CDC+, LDC bus bar+, CDC− and LDC bus bar− are the
dominant distributed parameters
I
causing the series resonance at 500 kHz and the effect on the CM current I1. Therefore C1 and C4 have
a very small effect on I1 and can be ignored. Changing of any parameter among CDC+, LDC bus bar+, CDC−
and LDC bus bar+ can reduce the value of I1 at 500 kHz. From Equation (4), LDC+, CY1, LY1, LDC−, CY2, LY2, C8
and C9 are the effective distributed parameters at 30 MHz and with an effect on I1.
Figure10.
10.Equivalent
Equivalent circuitof
ofCM
CMinterference
interferenceat
at 30MHz.
MHz.
Figure
The effect from distributed
parameterscircuit
on conducted
voltage UR30
according to above equivalent
circuits
andEquation
calculation
kHz and 30 MHz is shown in Table 3. In a motor drive system, the
From
(3),atC500
DC+, LDC bus bar+, CDC− and LDC bus bar− are the dominant distributed parameters
Z1 denotes
series-parallel
impedance
of C8 , Lcannot
,controlled,
RDC1 , LDC+and
, CY1
, LY1the
, CL1
and RL1 .
parameters
such
as
C
1–C6, CX, L
X and LM usually
beCM
only
distributed
DCon
busthe
bar+
causing the series resonance at 500
kHz and the effect
current I1. Therefore
C1 and
C4 have
Z2 denotes series
of LC
series-parallel
impedance
of Lwith
parameters
busimpedance
bar+, LDC bus bar−
DC+
, Cbar+
DC−,and
CChanging
8, R
CDC1
9, L.Y1Z
, of
Y2, CY1, C
Y2 could be changed
along
3Ldenotes
DC+ ,
DC
bus
a very smallLDC
effect
on I1 and can, be
ignored.
any parameter
among CDC+, LDC
bus bar+, CDC−
C
,
R
,
C
and
L
.
Z
denotes
series
impedance
of
L
,
C
and
R
.
different
arrangements,
L1 LL1
Y1
Y1
4filtering and shielding.
DC+
L1
L1
and
DC bus bar+ can reduce the value of I1 at 500 kHz. From Equation (4), LDC+, CY1, LY1, LDC−, CY2, LY2, C8
From Equation (3), CDC+ , LDC bus bar+ , CDC− and LDC bus bar− are the dominant distributed
and C9 are the effective distributed parameters at 30 MHz and with an effect on I1.
Table 3.the
Theseries
effect of
the main at
distribution
parameter
on conducted
EMI
emission.
parameters causing
resonance
500 kHz and
the effect
on the CM
current
I1 . Therefore C1
The effect from distributed parameters on conducted voltage UR according to above
equivalent
and C4 have a very small effect on I1 and can be ignored. Changing of any parameter among CDC+ ,
circuits and calculation atChanging
500 kHzof
and
30 MHz is shown
in Table
3. In a motor drive system, the
Parameters
Current
Voltage
LDC bus bar+ , CDC− and LDC bus bar+ can reduce the value of I1 at 500 kHz. From Equation (4), LDC+ , CY1 ,
parameters such as C1–C6, CXL, DCLXbusand
bar+ ↑ L
orM ↓usually cannot
I1 ↓ be controlled,
UR ↓ and only the distributed
LY1 , LDC− , CY2 , LY2 , C8 and C9 are the effective distributed parameters at 30 MHz and with an effect
parameters LDC bus bar+, LDC bus bar−
CDC+
DC−↓, C8, C9, LY1, IL
be changed along with
LDC, bus
bar−, ↑Cor
1 Y2
↓ , CY1, CY2Ucould
R ↓
on I1 .
DC+ ↑shielding.
or ↓
I1 ↓
UR ↓
different arrangements, filteringCand
The effect from distributed parameters
URUaccording
to above equivalent
CDC−↑ or ↓ on conductedI1voltage
↓
R ↓
circuits and calculation
at
500
kHz
and
30
MHz
is
shown
in
Table
3.
In
a
motor
drive system,
8 ↑
I2 ↓ on conducted
UR ↓ EMI emission.
Table 3. The effect of theCmain
distribution parameter
the parameters such as C1 –C6 , CX , LCX9 and
↑ LM usually cannot
I2 ↓ be controlled,
UR ↓ and only the distributed
Changing, of
Parameters
Current
Voltage
parameters LDC bus bar+ , LDC
C
,
C
,
C
,
C
,
L
,
L
,
C
, CY2 could be changed along
DC+
DC
−
8
9
Y1
Y2
Y1
bus bar−
LDC bus bar+
↑ or
↓
I1 ↓
UR ↓
with different arrangements, filtering
and
shielding.
4
LDC bus bar− ↑ or ↓
CDC+ ↑ or ↓
CDC−↑ or ↓
C8 ↑
C9 ↑
I1 ↓
I1 ↓
I1 ↓
I2 ↓
I2 ↓
UR ↓
UR ↓
UR ↓
UR ↓
UR ↓
Energies 2017, 10, 1
11 of 17
Table 3. The effect of the main distribution parameter on conducted EMI emission.
Changing of Parameters
LDC bus bar+ ↑ or ↓
LDC bus bar− ↑ or ↓
CDC+ ↑ or ↓
CDC− ↑ or ↓
C8 ↑
C9 ↑
LY1 ↑ LY1 ↑
LY2 ↑ LY2 ↑
CY1 ↑CY1 ↑
CY2 ↑
CY2 ↑
LDC bus bar+ ↑
L
DC bus bar+ ↑
LDC bus bar− ↑
Energies 2016, 10, 1
LDC bus bar− ↑
Current
I1
I1
I1
I1
I2
I2
I2
I2
I2
I2
I2
I2
↓
↓
↓
↓
↓
↓
↓I2 ↓
↓I2 ↓
↓I2 ↓
↓I2 ↓
↓
↓I2 ↓
I2 ↓
Voltage
UR
UR
UR
UR
UR
UR
URU↓R
URU↓R
URU↓R
URU↓R
U
URU↓R
R
UR ↓
↓
↓
↓
↓
↓
↓
↓
↓
↓
↓
↓
↓
11 of 17
4. Simulation of the Effect of Distributed Parameters
4. Simulation of the Effect of Distributed Parameters
4.1. System
System Conducted
Conducted EMI
EMI Modeling
Modeling
4.1.
According to the structure of the system and the distributed parameters, the power inverter
system was modeled as a simplified single-arm bridge of the power inverter system using the EMC
simulation software “Computer Simulation
Simulation Technology” (CST)
(CST) that predicts the noise in the entire
simulation
conducted
emissions
range
from
150
kHz
to
108
MHz,
as
conducted emissions range from
MHz, as illustrated
illustrated in
in Figure
Figure 11.
11. The conducted
emission (CE) voltage on the resistor of the LISN in the DM and CM network equivalent circuits can
time-domain
simulation,
followed
by fast
transform(FFT)
in the designer
be obtained
obtainedbybyusing
using
time-domain
simulation,
followed
byfourier
fast fourier
transform(FFT)
in the
platform
provided
in
the
CST
software.
The
CM
EMI
source
is
equivalent
to
an
ideal
trapezoidal
designer platform provided in the CST software. The CM EMI source is equivalent to an shape
ideal
wave
and theshape
EMI voltage
measured
by avoltage
probe Pmeasured
emission
voltage.
The EMI
trapezoidal
wave and
the EMI
by a conducted
probe P1 is
the positive
conducted
1 is the positive
voltage simulation
result
shown in
Figure 12.result
Tableis 3shown
and Figure
12 suggest
that3 the
emission
voltage. The
EMIis voltage
simulation
in Figure
12. Table
andconducted
Figure 12
EMI voltage
spectrum
of theEMI
motor
drivespectrum
system inofEV
be divided
into two
frequency
suggest
that the
conducted
voltage
thecan
motor
drive system
in different
EV can be
divided
ranges:
low frequency
range
around
500 frequency
kHz that isrange
dominated
DC
cables’
capacitance
into
twothe
different
frequency
ranges:
the low
aroundby
500
kHz
that is
dominatedand
by
DC bus
bars,
and
the
high
frequency
range
around
30
MHz
that
is
related
to
parasitic
resonances
due
cables’ capacitance and DC bus bars, and the high frequency range around 30 MHz that is
to the distributed
parameters
of due
Y capacitors
and distributed
capacitance
from the IGBT
node
related
to parasitic
resonances
to the distributed
parameters
of Y capacitors
and phase
distributed
to the chassis.
Thethe
EMIIGBT
voltage
peaks
obtained
in Figure
12 correspond
to those
capacitance
from
phase
node
to the through
chassis. simulation
The EMI voltage
peaks
obtained through
of measurements
at 500
and 30 to
MHz.
There
are some larger
between
results
simulation
in Figure
12 kHz
correspond
those
of measurements
at errors
500 kHz
and 30simulation
MHz. There
are
and measurement
because
the measurement
voltage is the
totalbecause
of the EMI
from the
some
larger errorsresults
between
simulation
results and EMI
measurement
results
the noise
measurement
threevoltage
arms ofisthe
power
Conversely,
the
simulated
EMI
is obtained
from
a single-arm.
EMI
the
total inverter.
of the EMI
noise from
the
three arms
ofvoltage
the power
inverter.
Conversely,
the
It can be seen
the model
is efficient
enough
to be used
to predict
thethat
CM the
current
paths
and the
simulated
EMIthat
voltage
is obtained
from
a single-arm.
It can
be seen
model
is efficient
elementstoresponsible
the EMI.
enough
be used to for
predict
the CM current paths and the elements responsible for the EMI.
Figure
Figure 11.
11. CM
CM circuit
circuit model
model of
of single-arm
single-arm bridge
bridge of
of power
power inverter.
inverter.
100
Vp/(dBμV)
80
60
40
Energies 2017, 10, 1
12 of 17
Figure 11. CM circuit model of single-arm bridge of power inverter.
100
Vp/(dBμV)
80
60
40
20
0
Simulation
Measurement
-20
10
0
frequency/(MHz)
Energies 2016, 10, 1
10
1
2
10
12 of 17
Figure 12. Comparison of measurement and simulation.
Figure 12. Comparison of measurement and simulation.
4.2.
The Effect
Effect of
of Distributed
Distributed Parameters
Parameters
4.2. The
DC bus
and
LDCLDC
bus bar−
4.2.1. The Effect of LDC
and
busbar+
bar+
bus bar−
According to
toTable
Table3,3,changing
changing
value
DC bus
bar+and
andLDC
LDCbus
bus bar
bar−−can
According
thethe
value
of LofDCLbus
canmitigate
mitigatethe
the resonance
bar+
low frequency.
frequency. Therefore,
and reduce the conducted emissions at low
Therefore, the
the EMI voltage peak due to
resonance at
at 500
500kHz
kHzcould
couldbe
besuppressed.
suppressed.The
Thevoltage
voltagevalue
value
conducted
emission
kHz
resonance
ofof
conducted
emission
at at
500500
kHz
cancan
be
be rapidly
decreased
about
50 dB
increasing
value
bar+ and
and LLDC
DC bus
104104
nHnH
to
rapidly
decreased
by by
about
50 dB
by by
increasing
thethe
value
of LofDCLDC
busbus
bar+
busbar−
barfrom
− from
220220
nHnH
to to
comply
with
thethe
limit
level-3
of of
CISPR25
regulatory
standards,
as as
shown
in in
Figure
13.13.
It
to
comply
with
limit
level-3
CISPR25
regulatory
standards,
shown
Figure
suggests
that
two
CM
inductors
It
suggests
that
two
CM
inductorscan
canbebeplaced
placedon
onthe
theDC
DCbus
busbar
barof
of the
the power
power inverter
inverter of the AC
current and
and conducted
conducted emission
emission at
at 500
500 kHz.
kHz.
motor to reduce the CM current
100
Vp/(dBμV)
80
60
40
20
0
-20
LDC
bus bar+
=104nH and LDC
bus bar-
LDC
bus bar+
=220nH and LDC
bus bar-
=104nH
=220nH
0
10
frequency/(MHz)
10
1
Figure 13. Positive conducted emission(CE) voltage after LDC bus bar+ and LDC bus bar− were increased.
Figure 13. Positive conducted emission(CE) voltage after LDC bus bar+ and LDC bus bar− were increased.
4.2.2. The Effect of LY1 and LY2
4.2.2. The Effect of LY1 and LY2
According to Table 3, LY1 and LY2 can be increased to mitigate the resonance and reduce the
According to Table 3, LY1 and LY2 can be increased to mitigate the resonance and reduce the
conducted emission at high frequency.
Therefore, the EMI voltage peak due to resonance at 30 MHz
conducted emission at high frequency. Therefore, the EMI voltage peak due to resonance at 30 MHz
could be suppressed. The voltage value of conducted emission at 30 MHz can be rapidly decreased
could be suppressed. The voltage value of conducted emission at 30 MHz can be rapidly decreased by
by about 64 dB by increasing the value of LY1 and LY2 from 200 nH to 300 nH to comply with the
about 64 dB by increasing the value of LY1 and LY2 from 200 nH to 300 nH to comply with the level-3
level-3 limit of CISPR25, as shown in Figure 14. It suggests that the equivalent series inductance of Y
limit of CISPR25, as shown in Figure 14. It suggests that the equivalent series inductance of Y capacitor
capacitor can affect the conducted EMI at 30 MHz. A better design of the parameters of the Y
can affect the conducted EMI at 30 MHz. A better design of the parameters of the Y capacitor can
capacitor can reduce the conducted emissions at high frequency.
reduce the conducted emissions at high frequency.
100
Vp/(dBμV)
80
60
40
20
0
-20
LY1=200nH and LY2=200nH
LY1=300nH and LY2=300nH
10
0
frequency/(MHz)
10
1
10
Figure 14. Positive CE voltage after LY1 and LY2 were increased.
2
conducted emission at high frequency. Therefore, the EMI voltage peak due to resonance at 30 MHz
could be suppressed. The voltage value of conducted emission at 30 MHz can be rapidly decreased
by about 64 dB by increasing the value of LY1 and LY2 from 200 nH to 300 nH to comply with the
level-3 limit of CISPR25, as shown in Figure 14. It suggests that the equivalent series inductance of Y
capacitor
the
Y
Energies
2017,can
10, 1affect the conducted EMI at 30 MHz. A better design of the parameters of 13
of 17
capacitor can reduce the conducted emissions at high frequency.
100
Vp/(dBμV)
80
60
40
20
0
-20
LY1=200nH and LY2=200nH
LY1=300nH and LY2=300nH
10
0
frequency/(MHz)
10
1
10
2
Figure 14. Positive CE voltage after LY1 and LY2 were increased.
Figure 14. Positive CE voltage after LY1 and LY2 were increased.
4.2.3. The Effect of Combination of LDC bus bar+, LDC bus bar−, LY1 and LY2
4.2.3. The Effect of Combination of LDC bus bar+ , LDC bus bar− , LY1 and LY2
Increasing of the value of LDC bus bar+, LDC bus bar− (each 220 nH) and LY1, LY2 (each 300 nH) can
Increasing of the value of LDC bus bar+ , LDC bus bar− (each 220 nH) and LY1 , LY2 (each 300 nH) can
decrease the conduced emissions
at frequencies from 150 kHz to 108 MHz to below the limit level-3
decrease the conduced emissions at frequencies from 150 kHz to 108 MHz to below the limit level-3 of
of CISPR25. Then there are no resonances previously caused by LDC bus bar+ and LDC bus bar− at 500 kHz,
CISPR25. Then there are no resonances previously caused by LDC bus bar+ and LDC bus bar− at 500 kHz,
LY1 and LY2 at 30 MHz. Although there still is a resonance point at around 55 MHz, the value of
LY1 and LY2 at 30 MHz. Although there still is a resonance point at around 55 MHz, the value of
conducted voltage is decreased below the level-3 limit of CISPR25, as shown in Figure 15.
conducted
is decreased below the level-3 limit of CISPR25, as shown in Figure 15.
Energies 2016,voltage
10, 1
13 of 17
100
80
Vp/(dBμV)
60
40
20
0
L
L
-20
DC bus bar+
DC bus bar+
=104nH and L
=220nH and L
DC bus barDC bus bar-
10
=104nH,L =200nH and L =200nH
Y1
Y2
=220nH,L =300nH and L =300nH
Y1
0
f/(MHz)
Y2
10
1
10
2
Figure
Positive
voltage
after
DC bus bar+, LDC bus bar−, LY1 and LY2 were increased.
Figure
15. 15.
Positive
CE CE
voltage
after
LDCLbus
bar+ , LDC bus bar− , LY1 and LY2 were increased.
4.2.4. The
The Effect
Effect of
of C
CDC+ and
CDC−
4.2.4.
DC+ and CDC−
From Table
Table3,3,the
thedistributed
distributedcapacitances
capacitancesfrom
fromDC
DCcables
cables(C(CDC+, ,CCDC−)) can
affect the conducted
From
DC+
DC− can affect the conducted
emissions.
Changing
the
value
of
C
DC+ and CDC− can mitigate the resonance at 500 kHz and reduce
emissions. Changing the value of CDC+ and CDC− can mitigate the resonance at 500 kHz and reduce
the conducted
conducted emission
emissionatatlow
lowfrequency.
frequency.The
Thevoltage
voltagevalue
value
conducted
emission
at 500
kHz
the
ofof
conducted
emission
at 500
kHz
cancan
be
be
decreased
by
about
25
dB
by
increasing
the
value
of
C
DC+ and CDC− from 100 nF to 250 nF to
decreased by about 25 dB by increasing the value of CDC+ and CDC− from 100 nF to 250 nF to comply
comply
with level-3
the limit
level-3 ofasCISPR25,
shown
Figure 16.
suggests
that
filteringofand
with
the limit
of CISPR25,
shown inas
Figure
16. in
It suggests
thatItfiltering
and
shielding
the
shielding
of
the
DC
input
of
the
power
inverter
of
the
AC
motor
can
be
used
to
change the
DC input of the power inverter of the AC motor can be used to change the distributed parameters
distributed
of DC
the CM current
at lowthe
frequency
and suppress
of
DC cablesparameters
to reduce the
CMcables
currenttoatreduce
low frequency
and suppress
EMI voltage
peak duethe
to
EMI voltage
peak
dueFor
to resonance
kHz. For
example,
a Ybetween
capacitor
be added
between
resonance
at 500
kHz.
example, aatY 500
capacitor
could
be added
thecould
DC cable
and chassis
to
the DCconducted
cable and chassis
to reduce
conducted
emissions,
the Yground
capacitor
may cause
a high
reduce
emissions,
although
the Y capacitor
mayalthough
cause a high
leakage
current.
ground leakage current.
comply with the limit level-3 of CISPR25, as shown in Figure 16. It suggests that filtering and
shielding of the DC input of the power inverter of the AC motor can be used to change the
distributed parameters of DC cables to reduce the CM current at low frequency and suppress the
EMI voltage peak due to resonance at 500 kHz. For example, a Y capacitor could be added between
the DC2017,
cable
chassis to reduce conducted emissions, although the Y capacitor may cause 14
a high
Energies
10, and
1
of 17
ground leakage current.
Figure16.
16.Positive
PositiveCE
CEvoltage
voltageafter
afterCDC+
CDC+and
andCCDC
DC−−were
Figure
wereincreased.
increased.
4.2.5. The
The Effect
Effect of
of the
the Combination
Combination of
of CCY1
Y1,, C
, C8 and C9
4.2.5.
CY2
Y2 , C8 and C9
From Table
Table3,3,the
the
capacitances
of the
Y capacitors
, CY2) and the distributed capacitance
From
capacitances
of the
Y capacitors
(CY1(C
, CY1
Y2 ) and the distributed capacitance from
from
the
collector
and
emitter
of
the
IGBT
to
the
chassis
(C
8
,
C
can affect
the conduced
emissions
at
the collector and emitter of the IGBT to the chassis (C8 , C9 ) can9)affect
the conduced
emissions
at high
high
frequency.
The
voltage
value
of
conducted
emissions
at
high
frequency
can
be
decreased
to
frequency. The voltage value of conducted emissions at high frequency can be decreased to comply
comply
with CISPR25
by increasing
of CY1 and CY2 from 100 nF to 500 nF and the value of
with
CISPR25
by increasing
the value the
of Cvalue
Y1 and CY2 from 100 nF to 500 nF and the value of C8 and C9
C
8
and
C
9
from
20
pF
to
100
pF,
as
shown
in
Figure
17.that
It shows
thatvalue
the peak
value
of the conducted
from 20 pF to 100 pF, as shown in Figure 17. It shows
the peak
of the
conducted
voltage is
voltage is
20 dB
at about
30 MHz.YTherefore,
capacitors
could
be added
betweenand
the
reduced
byreduced
20 dB atby
about
30 MHz.
Therefore,
capacitors Y
could
be added
between
the collector
collector
and
emitter
of
the
IGBT
and
chassis,
and
between
DC
input
and
chassis
to
reduce
emitter of the IGBT and chassis, and between DC input and chassis to reduce conducted emissions at
conducted
emissions at high frequency.
high
frequency.
Energies 2016, 10, 1
14 of 17
100
80
Vp/(dBμV)
60
40
20
0
-20
CY1=100nF,CY2=100nF,C8=20pF and C9=20pF
-40 1
10
CY1=500nF,CY2=500nF,C8=100pF and C9=100pF
f/(MHz)
Figure 17. Positive CE voltage after CY1, CY2, C8 and C9 were increased.
Figure 17. Positive CE voltage after CY1 , CY2 , C8 and C9 were increased.
4.2.6. The Effect of the Combination of CDC+, CDC−, CY1, CY2, C8 and C9
4.2.6. The Effect of the Combination of CDC+ , CDC− , CY1 , CY2 , C8 and C9
It is a better mitigation method to change the value of the distributed parameters (CDC+, CDC−, CY1,
It is a better mitigation method to change the value of the distributed parameters (CDC+ , CDC− ,
CY2, C8 and C9) to reduce the conducted emission at frequencies from 150 kHz to 108 MHz defined in
CY1 , CY2 , C8 and C9 ) to reduce the conducted emission at frequencies from 150 kHz to 108 MHz defined
CISPR25. The conducted voltage is reduced by increasing the capacitances (CDC+ = CDC− = 250 nF, CY1 =
in CISPR25. The conducted voltage is reduced by increasing the capacitances (CDC+ = CDC− = 250 nF,
CY2 = 500 nF, C8 = C9 = 100 pF), as shown in Figure 18.
CY1 = CY2 = 500 nF, C8 = C9 = 100 pF), as shown in Figure 18.
100
80
Vp/(dBμV)
60
40
20
0
-20
C
=100nf,C
C
=250nF,C
DC+
DC+
=100nf,C =100nF,C =100nF,C =20pF and C =20pF
DC-
Y1
Y2
8
9
=250nF,C =500nF,C =500nF,C =100pF and C =100pF
DC-
Y1
Y2
10
8
0
frequency/(MHz)
9
10
1
10
2
Figure 18. Positive CE voltage after CDC+, CDC−, CY1, CY2, C8 and C9 were increased.
4.2.6. The Effect of the Combination of CDC+, CDC−, CY1, CY2, C8 and C9
4.2.6. The Effect of the Combination of CDC+, CDC−, CY1, CY2, C8 and C9
It is a better mitigation method to change the value of the distributed parameters (CDC+, CDC−, CY1,
It is a better mitigation method to change the value of the distributed parameters (CDC+, CDC−, CY1,
CY2, C8 and C9) to reduce the conducted emission at frequencies from 150 kHz to 108 MHz defined in
CY2, C8 and C9) to reduce the conducted emission at frequencies from 150 kHz to 108 MHz defined in
CISPR25.
The
conducted voltage is reduced by increasing the capacitances (CDC+ = CDC− = 250 nF,
CY1 =
Energies
2017,The
10, 1conducted voltage is reduced by increasing the capacitances (CDC+ = CDC− = 250 nF,
15CofY117
CISPR25.
=
CY2 = 500 nF, C8 = C9 = 100 pF), as shown in Figure 18.
CY2 = 500 nF, C8 = C9 = 100 pF), as shown in Figure 18.
100
100
Vp/(dBμV)
Vp/(dBμV)
80
80
60
60
40
40
20
20
0
0
-20
-20
C
=100nf,C =100nf,C =100nF,C =100nF,C =20pF and C =20pF
DC+
DCY1
Y2
8
9
CC =100nf,C
=100nf,C
=100nF,C =100nF,C
=20pF and C =20pF
=250nF,C
=250nF,C
DC+
DCY1 Y1=500nF,C
Y2 Y2=500nF,C
8 8=100pF and
9 C9=100pF
DC+
DCC
=250nF,C =250nF,C =500nF,C
=500nF,C =100pF and C =100pF 1
0
DC+
DCY1
Y2
8
9
10
10
0
1
frequency/(MHz)
10
10
frequency/(MHz)
2
10
2
10
Figure
18.
Positive
CE
voltage
after
CDC+
, CDC−,, C
CY1,, C
Y2, C8 and C9 were increased.
Figure
18.18.
Positive
CECE
voltage
after
CDC+
,C
,C
increased.
DC
−, CY1
Y1, CCY2
Y2
8 and
9 were
Figure
Positive
voltage
after
CDC+
,C
DC−
,C
8 and
C9Cwere
increased.
5. Experimental Verification
5. Experimental Verification
Verification
According to the above analysis of the effect of distributed parameters on the power inverter
According to the above
above analysis
analysis of the
the effect
effect of
of distributed
distributed parameters
parameters on the
the power
power inverter
inverter
system of AC motors for EVs, changing the combination of CDC+, CDC−, CY1, CY2, C7 and C8 should be a
system of AC motors for EVs, changing the combination
combination of
of C
CDC+
,C
, C, Y1
C7 and
C8 should
,C
DC−
,C
CY2, ,CC
C8 should
be a
DC+
DC
− Y1
Y27 ,and
better way to suppress the voltage peak at 500 kHz and 30 MHz to comply with the limit level-3 of
be
a better
to suppress
the voltage
at 500
30 MHz
to comply
with
limit
level-3
better
wayway
to suppress
the voltage
peakpeak
at 500
kHzkHz
andand
30 MHz
to comply
with
thethe
limit
level-3
of
CISPR 25. A new pair of Y capacitors are added between the collector and emitter of the IGBT and
of
CISPR
25.
A
new
pair
of
Y
capacitors
are
added
between
the
collector
and
emitter
of
the
IGBT
CISPR 25. A new pair of Y capacitors are added between the collector and emitter of the IGBT and
DC bus bar and the chassis to increase the capacitances between the inverter and the chassis.
and
chassis
increase
thecapacitances
capacitancesbetween
betweenthe
theinverter
inverterand
and the
the chassis.
DC DC
bus bus
bar bar
andand
thethe
chassis
to to
increase
the
Experimental verification is conducted and the results are shown in Figure 19. The conducted
Experimental
conducted
andand
the results
are shown
in Figure
The conducted
emission
Experimentalverification
verificationis is
conducted
the results
are shown
in 19.
Figure
19. The conducted
emission characteristics at around 500 kHz and 30 MHz in Figure 19 are approximately as predicted
characteristics
at
around
500
kHz
and
30
MHz
in
Figure
19
are
approximately
as
predicted
by the
emission characteristics at around 500 kHz and 30 MHz in Figure 19 are approximately as predicted
by the simulation in Figure 18.
simulation
in Figure
18.
by the simulation
in Figure
18.
100
100
Vp/(dBμV)
Vp/(dBμV)
80
80
60
60
40
40
20
20
0
0
-20
-20
After increasing C
,C ,C ,C ,C and C
DC+
DC- Y1
Y2 8
9
After increasing C
,C ,C ,C ,C and C
DC- Y1
Y2 8,C and9C
Before increasingDC+
C
,C
,C ,C
DC+
DC- Y1
Y2 8
9
Before increasing C
,C ,C ,C ,C and C
DC+
DC- Y1
Y2 8
9
Limit level 3-CISPR25
0
Limit level 3-CISPR25
100
frequency/(MHz)
10
frequency/(MHz)
1
101
10
2
102
10
Figure 19. Positive CE voltage after CDC+, CDC−, CY1, CY2, C8 and C9 were increased.
Figure
Positive
voltage
after
CDC+
, CDC−,, C
Y1, CY2, C8 and C9 were increased.
Figure
19.19.
Positive
CECE
voltage
after
CDC+
,C
DC− CY1 , CY2 , C8 and C9 were increased.
6. Conclusions
This study proposed a new method to analyze the effects of distributed parameters on conducted
EMI from the DC-fed high voltage motor drive systems in EVs. The conducted EMI of high voltage DC
cables of the motor drive system in a frequency range of 150 kHz–108 MHz and two EMI noise peaks
at resonances frequencies 500 kHz and 30 MHz have been measured by a complete test for conducted
EMI emissions from the AC motor drive system of an EV under load conditions. The research mainly
focuses on the effects of distributed parameters in the inverter and cables on the resonances at 500 kHz
and 30 MHz, nor the distributed parameters of the motor due to the high impedance of the motor
model at 500 kHz and 30 MHz. The corresponding equivalent circuits for DM and CM EMI at resonance
frequencies of 500 kHz and 30 MHz are established to determine the EMI propagation paths and the
dominant distributed parameters of elements responsible for the resonances appearing at 500 kHz and
30 MHz.
The distributed parameters LDC bus bar+ , LDC bus bar− , CDC+ , CDC− , C8 , C9 , LY1 , LY2 , CY1 and CY2
can affect the EMI emissions from the high voltage motor drive system. The effect of the dominant
Energies 2017, 10, 1
16 of 17
distributed parameters on conducted voltage is verified by modeling of the CM circuit of a single-arm
bridge of the high voltage motor power inverter. Increasing the value of LDC bus bar+ , LDC bus bar− from
104 nH to 220 nH and LY1 , LY2 from 200 nH to 300 nH or increasing the capacitances (CDC+ , CDC−
from 100 nF to 250 nF, CY1 , CY2 from 100 nF to 500 nF, C8 , C9 from 20 pF to 100 pF) can mitigate the
two resonance peaks at the frequencies of 500 kHz and 30 MHz and decrease the conduced voltage
at frequencies from 150 kHz to 108 MHz to below the limit level-3 of CISPR25. The effect of the
combination of CDC+ , CDC− , CY1 , CY2 , C8 and C9 on conducted voltage is verified by experiments.
In future work, modeling of a CM circuit of three-arm bridge of the high voltage motor power inverter
in EV will be developed. After that the effect of distributed parameters on EMI noise will be further
simulated and tested.
Acknowledgments: This study is supported by National Natural Science of Foundation of China and Outstanding
Talents Project of Beijing.
Author Contributions: Li Zhai analyzed the system conducted emission; Liwen Lin and Xinyu Zhang performed
the modeling; Li Zhai and Chao Song performed the experiments; Li Zhai and Liwen Lin analyzed the data;
Li Zhai wrote the paper.
Conflicts of Interest: The authors declare no conflict of interest.
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