CN114611055A - Modeling method for conducted electromagnetic interference of motor driving system of electric vehicle - Google Patents

Modeling method for conducted electromagnetic interference of motor driving system of electric vehicle Download PDF

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CN114611055A
CN114611055A CN202210078548.2A CN202210078548A CN114611055A CN 114611055 A CN114611055 A CN 114611055A CN 202210078548 A CN202210078548 A CN 202210078548A CN 114611055 A CN114611055 A CN 114611055A
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翟丽
杨霜洁
胡桂兴
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Beijing Institute of Technology BIT
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
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    • H02P27/04Arrangements or methods for the control of AC motors characterised by the kind of supply voltage using variable-frequency supply voltage, e.g. inverter or converter supply voltage
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Abstract

The invention provides a method for modeling conducted electromagnetic interference of a motor driving system of an electric vehicle, which provides a complete modeling mode for fully considering parasitic parameters of all parts of a motor controller, a motor, a busbar and a cable and electromagnetic disturbance generating factors aiming at the motor driving system of the electric vehicle, overcomes various defects existing in the prior art, can achieve a good electromagnetic conducted interference simulation effect in a wider frequency range based on the model obtained by the invention, and has high model accuracy and wider applicability.

Description

Modeling method for conducted electromagnetic interference of motor driving system of electric vehicle
Technical Field
The invention belongs to the technical field of electromagnetic interference (EMI) modeling, and particularly relates to a conducted electromagnetic interference modeling method for a motor driving system of an electric automobile.
Background
The motor controller is used as a key component of a new energy automobile, when the motor controller works, the inverter high-power semiconductor devices (such as IGBT and the like) are operated to be quickly switched on and off to generate transient current and transient voltage, and because various parasitic parameters exist in the system, the conduction emission and radiation emission of electromagnetic disturbance can be formed, so that how to restrain negative influence caused by electromagnetic interference (EMI) is a great challenge in the design of a motor driving system of the current electric automobile. In order to verify the effectiveness and feasibility of the EMI suppression technology, a relatively accurate electromagnetic interference prediction model of the motor drive system needs to be established, so as to predict and evaluate EMI at the initial stage of product design and guide the electromagnetic compatibility design of the system.
At present, the modeling methods of the motor driving system mainly include a full wave method, a partial unit equivalent circuit method, a model order reduction method and the like. The full-wave electromagnetic modeling method is accurate in calculation, but due to the fact that the structures of the motor and the inverter are complex, a large amount of calculation time and a large amount of memory are needed for application of the full-wave model. The partial cell equivalent circuit (PEEC) method requires hundreds or thousands of elements to represent a simple geometric body, and is not suitable for modeling a complex structure. Model reduction (MOR) techniques can be used for system equivalent circuit modeling, but cannot analyze the effects of system internal parasitic parameters on EMI. Meanwhile, the extraction of the high-frequency parasitic parameters of the system elements is very important for establishing a conducted electromagnetic interference model, and the prediction accuracy of the model is directly influenced. The current methods mainly include Finite Element Method (FEM) and curve fitting method. The equivalent circuit established based on the FEM is accurate, but has high complexity, high calculation difficulty and long time consumption, and is not suitable for engineering application. The curve fitting method is simple, but the established circuit model has no obvious correlation with the motor structure, and main elements of the motor causing electromagnetic interference cannot be found. Therefore, the existing EMI modeling methods have certain defects and cannot meet the requirements of the field of new energy automobiles.
Disclosure of Invention
In view of the above, aiming at the technical problems in the prior art, the invention provides a modeling method for conducted electromagnetic interference of a motor driving system of an electric vehicle, which specifically comprises the following steps:
step 1, selecting a proper element, and initially establishing an electric vehicle driving system model topology consisting of a direct current bus, a direct current cable, a motor controller, a motor, an alternating current bus and an alternating current cable which are sequentially cascaded;
step 2, neglecting the distribution parameters of the direct-current busbar and the alternating-current busbar, and respectively establishing corresponding high-frequency parasitic parameter models only by using the concentration parameters and combining a busbar equivalent circuit;
step 3, aiming at the motor controller, establishing a collector-emitter interelectrode capacitance C aiming at the IGBT module of the motor controllerCEImpedance Z with positive pole to neutral pointUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNUModel relationship between them, and the positive-electrode-to-ground impedance Z of the IGBT modulePNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZUAnd IGBT module parasitic parameters: positive electrode capacitance to ground CPGNegative electrode-to-ground capacitor CNGAnd neutral point to ground capacitance CUGThe model relationship between them; performing a motor controller part modeling for measuring the impedance ZUP、ZUN、ZPNAnd ZP、ZN、ZUCan respectively output each parasitic parameter C of the IGBT moduleCEAnd CPG、CNG、CUG
Step 4, respectively measuring single-phase earth impedance and three-phase earth impedance of the motor, namely common mode impedance, and single-phase earth impedance of the motor, namely differential mode impedance; establishing a capacitance C to ground with the motor winding based on the common-mode impedanceGA model relationship therebetween; obtaining a model relation between the frequency-impedance curve resonance impedance peak and a motor single-phase winding RLC equivalent unit based on the frequency-impedance curve resonance impedance peak of the differential mode impedance;
step 5, measuring the impedance of a single cable with the length of 1m aiming at the alternating current cable, neglecting mutual inductance and mutual capacitance between two phases and establishing a three-phase alternating current cable model; and aiming at the direct current cable, measuring the impedance of a single cable with the length of 2m and establishing a direct current cable model. The modeling of the whole electric automobile motor driving system conducted electromagnetic interference is completed through the steps.
Further, it is characterized byThe capacitor CCEAnd positive electrode impedance to ground ZPNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZUThe relationship between them is derived by the following steps:
neglecting the capacitance to ground of the IGBT module, the capacitance CCEAnd positive pole to neutral point impedance Z of IGBT moduleUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNHas the following relationship:
Figure BDA0003485004750000021
thereby respectively obtaining the capacitance C of the positive electrode to the neutral pointUPNegative electrode to neutral point capacitor CUNPositive to negative capacitance CPN
Figure BDA0003485004750000022
Connecting the positive pole of the IGBT module to the groundPNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZURespectively expressed as:
Figure BDA0003485004750000023
the equivalent capacitance C of the IGBT module to the earthPNegative electrode-to-ground equivalent capacitor CNAnd neutral point to ground equivalent capacitance CURespectively as follows:
Figure BDA0003485004750000031
thereby by measuring ZP、ZN、ZUThen the C can be obtainedPG、CNG、CUG
Further, the motor winding single-phase model in the step 4 consists of three groups of cascaded RLC parallel resonance units;
considering 6 curve regions divided by the first three resonant impedance spikes for the frequency-impedance curve of the differential mode impedance, and sequentially performing the following steps:
firstly, selecting frequencies of two points and corresponding impedances in an inductive area of a first peak with the frequency less than the minimum frequency point, and calculating a main inductance L of a windingm
Figure BDA0003485004750000032
In the formula (f)P1、Z1And fP2、Z2The frequencies and corresponding impedances at two points on the curve of the region are shown.
② calculating a first peak frequency point f1Corresponding capacitance C ofm
Figure BDA0003485004750000033
From the first peak frequency point f1Determining the parasitic resistance of the main winding according to the peak amplitude;
thirdly, calculating a first trough frequency point f2Inductance L of1+L2
Figure BDA0003485004750000034
Fourthly, the second peak frequency point f3And a second valley frequency point f4Calculating the inductance L1And L2The proportion of (A):
Figure BDA0003485004750000035
fifthly, the second peak frequency point f3And the third sharp peak frequency point f5Calculating the capacitance C1And C2
Figure BDA0003485004750000036
Figure BDA0003485004750000037
From the second peak frequency f3And the third sharp peak frequency point f5Determining corresponding parasitic resistances respectively according to the peak amplitudes; using the measured frequency fP3Common mode impedance Z of3Calculating the grounding capacitance C of the motor windingGThe value of (c):
Figure BDA0003485004750000038
further, in the modeling, a direct-current bus supporting capacitor and an alternating-current bus supporting capacitor are respectively arranged between the direct-current bus and an IGBT module of the motor controller and between the IGBT module and the alternating-current bus for balancing bus voltage and eliminating ripples.
The modeling method for the conducted electromagnetic interference of the motor driving system of the electric automobile provided by the invention provides a complete modeling mode for fully considering the parasitic parameters of all parts of the motor controller, the motor, the busbar and the cable and the electromagnetic disturbance generating factors aiming at the motor driving system of the electric automobile, and overcomes various defects in the prior art.
Drawings
FIG. 1 is a single bridge arm IGBT high frequency equivalent model implemented by the present invention;
FIG. 2 is an equivalent impedance calculation circuit between the ports of the IGBT module provided by the invention;
FIG. 3 is an equivalent impedance calculation circuit of the IGBT module port to ground provided by the invention;
FIG. 4 is a high frequency equivalent model of the DC bus and the AC bus according to the present invention;
FIG. 5 is a high frequency equivalent model of a DC bus support capacitor implemented in accordance with the present invention;
FIG. 6 is a high frequency equivalent model of a motor controller embodying the present invention;
FIG. 7 is an impedance magnitude-frequency curve of a single-phase winding of the motor provided by the present invention;
FIG. 8 illustrates a single-phase winding model of an electrical machine embodying the present invention;
FIG. 9 is a high frequency equivalent model of a three-phase motor winding embodying the present invention;
FIG. 10 is a high frequency equivalent model of a DC cable and an AC cable implemented in accordance with the present invention;
FIG. 11 is a high frequency equivalent model of a motor drive system embodying the present invention;
fig. 12 is a comparison of modeling simulation and experimental test curves of a high-frequency equivalent model of a motor driving system implemented by the invention.
Detailed Description
The technical solutions of the present invention will be described clearly and completely with reference to the accompanying drawings, and it should be understood that the described embodiments are some, but not all embodiments of the present invention. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
The invention provides a modeling method for conducting electromagnetic interference of a motor driving system of an electric automobile, which specifically comprises the following steps:
step 1, selecting a proper element, and preliminarily establishing an electric vehicle driving system model topology composed of a direct current bus, a direct current cable, a motor controller, a motor, an alternating current bus and an alternating current cable which are sequentially cascaded;
step 2, neglecting the distribution parameters of the direct-current busbar and the alternating-current busbar, and respectively establishing corresponding high-frequency parasitic parameter models only by using the concentration parameters and combining a busbar equivalent circuit;
step 3, aiming at the motor controller, establishing a collector-emitter interelectrode capacitance C aiming at the IGBT module of the motor controllerCEImpedance Z with positive pole to neutral pointUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNUModel relationship between them, and the positive-electrode-to-ground impedance Z of the IGBT modulePNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZUAnd IGBT module parasitic parameters: positive electrode capacitance to ground CPGNegative electrode-to-ground capacitor CNGAnd neutral point to ground capacitance CUGThe model relationship between them; performing a motor controller partial modeling for measuring the impedance ZUP、ZUN、ZPNAnd ZP、ZN、ZUCan respectively output each parasitic parameter C of the IGBT moduleCEAnd CPG、CNG、CUG
Step 4, respectively measuring single-phase earth impedance and three-phase earth impedance of the motor, namely common mode impedance, and single-phase earth impedance of the motor, namely differential mode impedance; establishing a capacitance C to ground with the motor winding based on the common-mode impedanceGThe model relationship between them; obtaining a model relation between the frequency-impedance curve resonance impedance peak and a motor single-phase winding RLC equivalent unit based on the frequency-impedance curve resonance impedance peak of the differential mode impedance;
step 5, measuring the impedance of a single cable with the length of 1m aiming at the alternating current cable, neglecting mutual inductance and mutual capacitance between two phases and establishing a three-phase alternating current cable model; and aiming at the direct current cable, measuring the impedance of a single cable with the length of 2m and establishing a direct current cable model. The modeling of the whole electric automobile motor driving system conducted electromagnetic interference is completed through the steps.
In a preferred embodiment of the invention, four parasitic capacitances are considered for the IGBT module of a single leg as shown in fig. 1: collector-emitter interelectrode capacitance CCEPositive electrode-to-ground capacitor CPGNegative electrode-to-ground capacitor CNGAnd neutral point to ground capacitance CUG. In general, CCEHas a capacitance value of about several tens nF, and a capacitance to ground CPG、CUG、CNGIs in the order of a few hundred pF, so the capacitance to ground C of the IGBT module is ignoredUG. Using vector network analyzer, respectively aligning IGBT modules (type: IGBT)FS800R07A2E3) equivalent impedance.
Respectively obtaining positive pole to neutral point impedance Z through impedance measurement between portsUPNegative electrode to neutral point impedance ZUNPositive to negative impedance ZPN. Establishing impedance Z from positive pole of IGBT module to neutral pointUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNThe calculating circuits (2) are shown in FIGS. 2(a), (b), and (c), respectively. According to the analysis of the equivalent impedance calculation circuit, the following results are obtained:
Figure BDA0003485004750000051
calculating to obtain equivalent capacitance CUPAnd CUNHas a capacitance value of 23nF, CPNAnd 11.5 nF. :
Figure BDA0003485004750000052
calculating to obtain CCEAnd 23 nF. (ii) a
And respectively obtaining the positive pole earth impedance, the negative pole earth impedance and the neutral point earth impedance through the measurement of the port earth impedance. Establishing positive earth impedance Z of IGBT modulePNegative electrode impedance to ground ZNAnd neutral-to-ground impedance ZUThe calculating circuits (2) are shown in FIGS. 3(a), (b), and (c), respectively. Connecting the positive pole of the IGBT module to the groundPNegative electrode impedance to ground ZNAnd neutral-to-ground impedance ZURespectively expressed as:
Figure BDA0003485004750000061
calculating to obtain equivalent capacitance CP≈1.2272nF,CN≈1.2029nF,CU≈1.2429nF。
The equivalent capacitance C of the IGBT module to the earthPNegative electrode-to-ground equivalent capacitor CNAnd a neutral point-to-ground equivalent capacitance CURespectively as follows:
Figure BDA0003485004750000062
calculating to obtain CPG=480pF,CNG=240pF,CUG=540pF。
Thereby by measuring ZP、ZN、ZUThen the C can be obtainedPG、CNG、CUG
And establishing a three-dimensional model of the direct-current busbar and the alternating-current copper busbar shown in the figure 4 by using software ANSYS/Q3D, and extracting high-frequency parasitic parameters. Since the dc bus bar and the ac bus bar have short lengths, only lumped parameter models are created as shown in fig. 4(a) and (b). Wherein L isBPIs self-inductance of the positive copper bar, LBNFor self-inductance of the negative copper bar, MPNFor mutual inductance of positive and negative copper bars, CBPIs a positive electrode copper bar capacitor to ground CBNIs a ground capacitor of the negative copper bar, CPNIs a capacitance between the positive and negative copper bars, LBUIs self-inductance of U-phase copper bar, LBVIs self-inductance of the V-phase copper bar, LBWSelf-inductance of W-phase copper bar, CBUIs a ground capacitor, C of the U-phase copper barBVIs a ground capacitor of V-phase copper bar, CBWIs a W-phase copper bar earth capacitance.
The direct-current bus supporting capacitor is arranged between the direct-current copper bar and the IGBT module and used for smoothing bus voltage and eliminating bus ripples. The parasitic inductance and the parasitic capacitance of the support capacitor are obtained by adopting the same measurement and calculation method of the IGBT module, and a high-frequency equivalent circuit model of the direct-current bus support capacitor shown in figure 5 is established.
After connecting the IGBT module model, the dc bus bar model, the ac bus bar model, and the dc bus bar support capacitor model, the high-frequency equivalent model of the motor controller may be as shown in fig. 6. The main parameters are shown in table 1:
TABLE 1 high-frequency model parameter table of motor controller
Figure BDA0003485004750000071
In step 4, a vector network analyzer is used to measure the impedance of the motor between single phase and three phase (i.e. common mode impedance) and between single phase and two phase and single phase (differential mode impedance) respectively. There are three resonance peaks in the port differential mode impedance curves of the motor U-phase and W-phase windings, as shown in fig. 7. The single-phase model of the motor winding is composed of three groups of cascaded RLC parallel resonance units, as shown in FIG. 8.
Considering 6 curve regions divided by the first three resonant impedance spikes for the frequency-impedance curve of the differential mode impedance, and sequentially performing the following steps:
firstly, selecting frequencies of two points and corresponding impedances in an inductive area of a first peak with the frequency less than the minimum frequency point, and calculating a main inductance L of a windingm
Figure BDA0003485004750000072
In the formula (f)P1、Z1And fP2、Z2The frequencies and corresponding impedances at two points on the curve of the region are shown. L can be calculated by selecting two points of (30kHz, 13 omega) and (200kHz, 85 omega)m=67μH。
② first peak frequency point f1The spike at 450kHz frequency point is caused by the main inductance L of the windingmAnd a capacitor CmCaused by resonance, C can be calculated according to the following formulamCalculating the first peak frequency f at 1.8nF1The corresponding capacitance of (C) can be obtainedm=1.8nF:
Figure BDA0003485004750000073
Wherein the parasitic resistance of the main winding is related to the amplitude of the resonance point, Rm=310Ω;
③ first wave trough frequency point f2The trough at the frequency point of 1.1MHz is formed by CmAnd an inductance L1And L2Caused by resonance, calculatingFirst trough frequency point f2The inductance of can be L1+L2=113nH:
Figure BDA0003485004750000074
Fourthly, the second peak frequency point f346MHz and a second valley frequency f4Calculating the inductance L at 100MHz1And L2The proportion of (A):
Figure BDA0003485004750000081
can be calculated to obtain: l is1=97nH,L2=16nH。
Due to C1And L1The resonance forms a second peak frequency point f3Peak at 46MHz, C2And L2The resonance forms a third peak frequency point f5Peak at 166MHz, so C1And C2Can calculate the capacitance C from the second peak and the third peak, respectively1And C2
Figure BDA0003485004750000082
Figure BDA0003485004750000083
According to the second peak frequency point f346MHz and third sharp peak frequency point f5Peak amplitude at 166MHz can be found: r1=350Ω,R2=150Ω。
Using the measured frequency fP3Common mode impedance Z of3Calculating the grounding capacitance C of the motor windingGThe value of (c):
Figure BDA0003485004750000084
frequency point f can be selected in the frequency range of three phases to the ground of 10kHz-1MHzP3Common mode impedance Z measured at 100kHz3120 omega, the grounding capacitance C of the motor winding is calculatedG=13.2nF。
The high-frequency equivalent circuit model of the permanent magnet synchronous motor is shown in fig. 9, and the element parameters in the model are shown in table 2. In the frequency range of 10kHz-200MHz, the deviation between the simulation result and the experimental result of the motor common mode equivalent impedance is small, and the established motor common mode impedance equivalent circuit model is relatively accurate.
TABLE 2 model parameters of PMSM
Figure BDA0003485004750000085
The method comprises the steps of establishing a high-frequency equivalent circuit model of a high-voltage cable with the length of 1m for the cable by adopting a measuring and calculating method similar to modeling of a permanent magnet synchronous motor, carrying out simulation test, and proving that the accuracy of the high-frequency equivalent circuit model of the cable is higher because the deviation between a cable impedance simulation result and a test result is smaller. Because the vehicle high-voltage power cables are all shielded wires, mutual inductance and mutual capacitance between different wires can be ignored. Therefore, from the model of the single cable, a three-phase alternating current cable model as shown in fig. 10(a) can be established. And by measuring the impedance of a 2m single cable, a high voltage direct current cable model can be established in the same way, as shown in fig. 10 (b).
The high-frequency equivalent circuit model of the motor driving system is composed of the established subsystem models, the models are established in ANSYS/Simplorer, the motor control module is established in Matlab software, and driving signals of 6 IGBT tubes are provided, as shown in FIG. 11. Through the collaborative simulation of Matlab and ANSYS software, the prediction of the transmission disturbance of the motor driving system can be realized.
In the specific implementation of the invention, the conducted emission test was carried out under the rated operating condition (53Nm 1900rpm) of the motor 1/4 with reference to the standard GB/T36282-2018. The comparison of the simulation result and the experiment result is shown in fig. 12, and it can be seen that the simulation result and the experiment result are good in correspondence within the frequency range of 150kHz to 108MHz, the error of the simulation result below 30MHz is less than 10dB, the accuracy of the high-frequency equivalent circuit model of the motor driving system is high, and the high-frequency equivalent circuit model can be used for simulating the conduction emission of the actual motor driving system.
It should be understood that, the sequence numbers of the steps in the embodiment of the present invention do not mean the execution sequence, and the execution sequence of each process should be determined by its function and inherent logic, and should not constitute any limitation to the implementation process of the embodiment of the present invention.
Although embodiments of the present invention have been shown and described, it will be appreciated by those skilled in the art that changes, modifications, substitutions and alterations can be made in these embodiments without departing from the principles and spirit of the invention, the scope of which is defined in the appended claims and their equivalents.

Claims (4)

1. A modeling method for conducted electromagnetic interference of a motor driving system of an electric automobile is characterized by comprising the following steps: the method specifically comprises the following steps:
step 1, selecting a proper element, and preliminarily establishing an electric vehicle driving system model topology composed of a direct current bus, a direct current cable, a motor controller, a motor, an alternating current bus and an alternating current cable which are sequentially cascaded;
step 2, neglecting the distribution parameters of the direct-current busbar and the alternating-current busbar, and respectively establishing corresponding high-frequency parasitic parameter models only by using the concentration parameters and combining a busbar equivalent circuit;
step 3, aiming at the motor controller, establishing a collector-emitter interelectrode capacitance C aiming at the IGBT module of the motor controllerCEImpedance Z with positive pole to neutral pointUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNUModel relationship between them, and the positive-electrode-to-ground impedance Z of the IGBT modulePNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZUAnd IGBT module parasitic parameters: positive electrode capacitance to ground CPGNegative electrode-to-ground capacitor CNGAnd neutral point to ground capacitance CUGThe model relationship between them; complete the motor controller partFractional modeling for measuring the impedance ZUP、ZUN、ZPNAnd ZP、ZN、ZUCan respectively output each parasitic parameter C of the IGBT moduleCEAnd CPG、CNG、CUG
Step 4, respectively measuring single-phase earth impedance and three-phase earth impedance of the motor, namely common mode impedance, and single-phase earth impedance of the motor, namely differential mode impedance; establishing a capacitance C to ground with the motor winding based on the common-mode impedanceGThe model relationship between them; obtaining a model relation between the frequency-impedance curve resonance impedance peak and a motor single-phase winding RLC equivalent unit based on the frequency-impedance curve resonance impedance peak of the differential mode impedance;
step 5, measuring the impedance of a single cable with the length of 1m aiming at the alternating current cable, neglecting mutual inductance and mutual capacitance between two phases and establishing a three-phase alternating current cable model; and aiming at the direct current cable, measuring the impedance of a single cable with the length of 2m and establishing a direct current cable model.
2. The method of claim 1, wherein: the capacitor CCEAnd positive electrode impedance to ground ZPNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZUThe relationship between them is derived by the following steps:
neglecting the capacitance to ground of the IGBT module, the capacitance CCEAnd positive pole to neutral point impedance Z of IGBT moduleUPNegative electrode to neutral point impedance ZUNAnd positive to negative impedance ZPNHas the following relationship:
Figure FDA0003485004740000011
thereby respectively obtaining the positive electrode to neutral point capacitance CUPNegative electrode to neutral point capacitor CUNPositive to negative capacitance CPN
Figure FDA0003485004740000021
Connecting the positive pole of the IGBT module to the groundPNegative electrode impedance to ground ZNAnd neutral point to ground impedance ZURespectively expressed as:
Figure FDA0003485004740000022
the equivalent capacitance C of the IGBT module to the earthPNegative electrode-to-ground equivalent capacitor CNAnd neutral point to ground equivalent capacitance CURespectively as follows:
Figure FDA0003485004740000023
thereby by measuring ZP、ZN、ZUThen the C can be obtainedPG、CNG、CUG
3. The method of claim 1, wherein: the motor winding single-phase model in the step 4 consists of three groups of cascaded RLC parallel resonance units;
considering 6 curve regions divided by the first three resonant impedance spikes for the frequency-impedance curve of the differential mode impedance, and sequentially performing the following steps:
firstly, selecting frequencies of two points and corresponding impedances in an inductive area of a first peak with the frequency less than the minimum frequency point, and calculating a main inductance L of a windingm
Figure FDA0003485004740000024
In the formula, fP1、Z1And fP2、Z2The frequencies and corresponding impedances at two points on the curve of the region are shown.
② calculating the first peak frequencyPoint f1Corresponding capacitance C ofm
Figure FDA0003485004740000025
From the first peak frequency point f1Determining the parasitic resistance of the main winding according to the peak amplitude;
thirdly, calculating a first trough frequency point f2Inductance L of1+L2
Figure FDA0003485004740000031
Fourthly, the second peak frequency point f3And a second valley frequency point f4Calculating the inductance L1And L2The proportion of (A):
Figure FDA0003485004740000032
fifthly, the second peak frequency point f3And the third sharp peak frequency point f5Calculating the capacitance C1And C2
Figure FDA0003485004740000033
Figure FDA0003485004740000034
From the second peak frequency f3And the third sharp peak frequency point f5Determining corresponding parasitic resistances respectively according to the peak amplitudes;
using the measured frequency fP3Common mode impedance Z of3Calculating the grounding capacitance C of the motor windingGThe value of (c):
Figure FDA0003485004740000035
4. the method of claim 1, wherein: in modeling, a direct-current bus supporting capacitor and an alternating-current bus supporting capacitor are respectively arranged between the direct-current bus and an IGBT module of a motor controller and between the IGBT module and the alternating-current bus for balancing bus voltage and eliminating ripples.
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