IGBT module stray capacitance extraction method based on external inductance resonance
Through the method based on external inductance resonance, using symmetric port measurement and vector network analyzer data, the error problem in parasitic common mode capacitor extraction of IGBT module is solved, and high-precision capacitance value extraction is achieved, which is suitable for high-power modules.
Patent Information
- Application Number
- CN202411415623.5
- Authority / Receiving Office
- CN · China
- Patent Type
- Applications(China)
- Current Assignee / Owner
- Filing Date
- 2024-10-11
- Publication Date
- 2024-12-10
- Estimated Expiration
- 2044-10-11
AI Technical Summary
When extracting parasitic common mode capacitors of IGBT modules, due to the asymmetric terminal measurement and the nonlinear characteristics of the freewheeling diode junction capacitance, the calculation error is large and the extraction value deviation is large.
Using an external inductance resonance method, the port impedance is measured between different terminals of the IGBT module through parallel resonant inductors, combined with vector network analyzer data, parasitic common mode capacitance is calculated, symmetric ports are selected for measurement to reduce errors, and multiple The group external inductance value verifies the accuracy of the extraction method.
It effectively eliminates the influence of the nonlinear characteristics of junction capacitors, improves the extraction accuracy of parasitic capacitors of IGBT modules, reduces measurement errors, and is suitable for the extraction of accurate capacitance values of high-power IGBT modules.
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Figure CN119104791A_ABST
Abstract
Description
Technical Field
[0001] The invention belongs to the technical field of power electronic simulation, and in particular relates to a method for extracting parasitic capacitance of an IGBT module based on external inductor resonance. Background Art
[0002] Insulated-Gate Bipolar Transistor (IGBT) combines the advantages of power MOSFET and bipolar transistor, and is widely used in power electronic devices and systems due to its high input impedance, high withstand voltage, large output current, small on-resistance, fast switching speed, etc. With the increase of switching frequency and power density, the voltage change rate (dv / dt) across the IGBT module and the current change rate (di / dt) flowing through the IGBT module are extremely large during switching. Due to the existence of circuit parasitic parameters, significant electromagnetic interference (EMI) is generated.
[0003] The positive, negative and midpoint of the two ends of the classic half-bridge IGBT module are led out from the direct bonding copper (DBC) and structural elements, and the bottom is fixed on the backplane (BP) copper layer. The parasitic common-mode capacitance formed between DBC and BP through the substrate is one of the key factors that determine the common-mode EMI performance of power electronic equipment. The common-mode EMI generated by the motor drive inverter is propagated to the heat sink and motor through these parasitic common-mode capacitances. Therefore, accurate extraction of parasitic common-mode capacitance is crucial for modeling and evaluating the EMI of power electronic equipment.
[0004] There are many studies on parasitic parameters in IGBT modules. For example, the literature [Q.Yang,L Wang,Z Qi et al.,“Analysis and Optimization of High-Frequency Switching Oscillation ConductedCM Current Considering Parasitic Parameters Based on a Half-Bridge Power Module,”IEEE Trans.Power Electron.,vol.38,no.10,pp.12659–12674,Oct.2023] uses finite element simulation to extract the parasitic inductance of the DBC inside the module and establishes an inductance distribution network; the literature [BT De Boi, ANLemmon,BW Nelson,CD New,and DMH Dudson,“Improved Methodology for Parasitic Characterization of High-Performance Power Modules,”IEEE Trans.Power Electron.,vol.35,no.12,pp.13400–13408,Dec.2020] measures the impedance of the IGBT module to obtain its parasitic inductance and capacitance parameters. However, there are few literatures on the parasitic common-mode capacitance of IGBT modules. Only one literature [A. Cataliotti, D. D. Cara, G. Marsala, A. Pecoraro, A. Ragusa, and G. Tine, "High-Frequency Experimental Characterization and Modeling of Six Pack IGBTs Power Modules," IEEE Trans. Ind. Electron., vol. 63, no. 11, pp. 6664–6673, Nov. 2016] proposed an original method for extracting parasitic common-mode capacitance based on external inductor resonance. This method extracts the value of parasitic common-mode capacitance by fitting the parasitic parameters measured from different terminals.
[0005] However, in the original method, asymmetric terminals were selected for measurement, resulting in significantly different voltages applied to the junction capacitance in different terminal measurements. Due to the nonlinear characteristics of the junction capacitance of the freewheeling diode (FWD), the value of the junction capacitance will also change during measurement, resulting in non-negligible calculation errors, which ultimately leads to large deviations in the parasitic common-mode capacitance value extracted by the original method. Summary of the invention
[0006] In view of the above, the present invention provides a method for extracting parasitic capacitance of an IGBT module based on external inductor resonance, which can greatly eliminate the influence of the nonlinear characteristics of the junction capacitance and accurately extract the parasitic capacitance value of the IGBT module.
[0007] A method for extracting parasitic capacitance of an IGBT module based on external inductor resonance, wherein the IGBT module is composed of two IGBT tubes T1 and T2 connected, the collector of T1 is the terminal P of the IGBT module, the emitter of T1 is connected to the collector of T2 as the terminal O of the IGBT module, and the emitter of T2 is the terminal N of the IGBT module. The method for extracting parasitic capacitance of the IGBT module comprises the following steps:
[0008] (1) Measure the total parasitic capacitance C between the IGBT module copper layer and the backplane copper layer T ;
[0009] (2) Connect a parallel resonant inductor between terminals P and O to achieve parallel resonance. Measure the port impedance Z between terminal P and the backplane copper layer. PB , measure the port impedance Z from terminal O to the backplane copper layer OB(PB) ;
[0010] (3) According to the port impedance Z at the resonant frequency PB and Z OB(PB) , combined with the measured value, calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal P on the backplane copper layer P ;
[0011] (4) Reconnect the resonant inductor and connect it in parallel between the terminals N and O. Measure the port impedance Z between the terminals N and the backplane copper layer. NB , measure the port impedance Z from terminal O to the backplane copper layer OB(NB) ;
[0012] (5) According to the port impedance Z at the resonant frequency NB and Z OB(NB) , combined with the measured value, calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal N on the backplane copper layer N ;
[0013] (6) Based on the total parasitic capacitance C T And the parasitic common-mode capacitance C calculated above P and C N , calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal O on the backplane copper layer O .
[0014] Furthermore, in step (1), since the junction capacitance of the freewheeling diodes T1 and T2 is much larger than the parasitic common-mode capacitance, the junction capacitance is regarded as a short circuit at high frequencies. Therefore, one terminal is selected from the terminals P, O, and N of the IGBT module, and the total parasitic capacitance C is measured between the terminal and the backplane copper layer. T , the measurement results are the same.
[0015] Furthermore, in step (2), a vector network analyzer is used to measure the port impedance Z at different frequencies from the terminal P and the backplane copper layer. PB , measure the port impedance Z at different frequencies from the terminal O and the backplane copper layer OB(PB) , record the data and draw a graph; in the step (4), a vector network analyzer is used to measure the port impedance Z at different frequencies from the terminal N and the backplane copper layer. NB , measure the port impedance Z at different frequencies from the terminal O and the backplane copper layer OB(NB) , record the data and draw a graph.
[0016] Furthermore, in step (3), the parasitic common mode capacitance C is calculated by the following expression: P :
[0017]
[0018] Where: Z PB (jω r1 ) represents the frequency jω r1 Lower port impedance Z PB The measured value, Z OB(PB) (jω r1 ) represents the frequency jω r1 Lower port impedance Z OB(PB) The measured value, ω r1 is the resonant angular frequency, j is an imaginary unit, and Re[] represents the real part.
[0019] Furthermore, in step (5), the parasitic common mode capacitance C is calculated by the following expression: N :
[0020]
[0021] Where: Z NB (jω r2 ) represents the frequency jωr2 Lower port impedance Z NB The measured value, Z OB(NB) (jω r2 ) represents the frequency jω r2 Lower port impedance Z OB(NB) The measured value, ω r2 is the resonant angular frequency.
[0022] Furthermore, the resonant angular frequency ω r1 and ω r2 The expression is as follows:
[0023]
[0024] Where: C D1 and C D2 are the capacitance values of the freewheeling diode junction capacitances of T1 and T2, L r is the inductance value of the resonant inductor.
[0025] Furthermore, in step (6), the parasitic common mode capacitance C is calculated by the following expression: O :
[0026] C O =C T -C P -C N
[0027] Furthermore, the resonant inductance is changed, and five groups of inductance values are selected from 3.3 to 100 uH as the resonant inductance values to repeat steps (2) to (6), thereby verifying the accuracy and stability of the IGBT module parasitic capacitance extraction method.
[0028] A computer device comprises a memory and a processor, wherein the memory stores a computer program, and the processor is used to execute the computer program to implement the above-mentioned IGBT module parasitic capacitance extraction method.
[0029] A computer-readable storage medium stores a computer program, and when the computer program is executed by a processor, the above-mentioned IGBT module parasitic capacitance extraction method is implemented.
[0030] Compared with the existing extraction methods, the parasitic capacitance extraction method of the IGBT module of the present invention selects symmetrical ports with close impedance for measurement, and the error is much smaller than that of the existing extraction method. It can greatly eliminate the influence of the nonlinear characteristics of the junction capacitance, and the extraction result is not affected by the external inductance value. It can be used to accurately extract the parasitic capacitance value of the IGBT module, especially the high-power IGBT module, with good accuracy. BRIEF DESCRIPTION OF THE DRAWINGS
[0031] Figure 1The figure is a flow chart of a method for extracting parasitic capacitance of an IGBT module based on external inductor resonance according to the present invention.
[0032] Figure 2 This is a schematic diagram of the topological structure of an actual half-bridge IGBT module power electronic system.
[0033] Figure 3 The parallel resonant inductor L is connected between terminals P and O. r Then measure the port impedance Z from both ends of terminals P and BP PB Schematic diagram of the test circuit.
[0034] Figure 4 The parallel resonant inductor L is connected between terminals P and O. r Then measure the port impedance Z from both ends of terminals O and BP OB(PB) Schematic diagram of the test circuit.
[0035] Figure 5 The port impedance Z PB and Z OB(PB) Schematic diagram of the comparison spectrum.
[0036] Figure 6 is the resonant frequency f under five sets of external inductors rPB and f ROB(PB) Schematic diagram of the experimental results.
[0037] Figure 7 The figure is a schematic diagram of parasitic capacitance value curves extracted by the method of the present invention under five groups of external inductances. DETAILED DESCRIPTION
[0038] In order to describe the present invention more specifically, the technical solution of the present invention is described in detail below in conjunction with the accompanying drawings and specific implementation methods.
[0039] like Figure 1 As shown, the method for extracting parasitic capacitance of an IGBT module based on external inductor resonance of the present invention includes the following specific steps:
[0040] (1) Measure the total parasitic capacitance C between DBC and BP from the IGBT module terminals P and BP T , C T According to the positive electrode P, negative electrode N and midpoint O, it is divided into C P , C N and C O .
[0041] The IGBT module model used in this embodiment is 2MB600XNG170-50, and the power level of the module is 1700V and 600A. Figure 2As shown in the figure, a typical half-bridge IGBT module has terminals P, N and O. The DBC connected to these three terminals is separated by the two IGBTs T1 and T2, and three parasitic common-mode capacitors C are formed on the BP copper layer. P , C N and C O The junction capacitance of FWD is C D1 and C D2 Connect to the parasitic common mode capacitor C P , C N and C O , due to the junction capacitance C D1 and C D2 Very large, reaching tens of nF, much larger than the parasitic common-mode capacitance of hundreds of pF. At high frequencies, C D1 and C D2 The value of can be regarded as a short circuit. Therefore, the measurement result from the terminal P, N or O to the BP copper layer is the same, that is, the sum of all three parasitic capacitances. The method of this embodiment measures the total parasitic capacitance C between DBC and BP from both ends of the terminal P and BP. T , while C T Satisfaction relationship: C T =C P +C O +C N .
[0042] (2) Connect a parallel resonant inductor L across terminals P and O r To achieve parallel resonance, measure the port impedance Z from terminals P and BP. PB , measure the port impedance Z from terminals O and BP OB(PB) .
[0043] A parallel resonant inductor L is connected across terminals P and O. r Then, measure the port impedance Z from terminals P and BP. PB The test circuit is as follows Figure 3 As shown, the port impedance Z is measured from terminals O and BP. OB(PB) The test circuit is as follows Figure 4 As shown. Definition C ON is the equivalent capacitance from terminals O and N to BP. Due to the high frequency junction capacitance C D1 and C D2 can be ignored, then C ON It can be expressed as:
[0044] C ON =C O +C N / / C D2 ≈C O +C N
[0045] Use a vector network analyzer to measure the port impedance Z at different frequencies from both ends of terminals P and BP PB And measure the port impedance Z at different frequencies from both ends of terminals O and BP OB(PB) , record the data and plot it as Figure 5 As shown, the real part of the impedance Re[Z PB ] and Re[Z OB(PB) ].
[0046] (3) Derivation of Z at the resonant frequency PB , Z OB(PB) The parasitic capacitance C is calculated by combining the measured value P The value of .
[0047] In this implementation case, considering the junction capacitance C D1 and parasitic capacitance C P , C ON The value of the port impedance Z at both ends of the terminal P and BP PB It can be derived as:
[0048]
[0049] When the external inductor L r and junction capacitance C D1 When resonance occurs between rPB The relationship should be satisfied:
[0050] s=jω rPB =j2πf rPB
[0051] s 2 L r C D1(PB) +1=0
[0052] Therefore, when resonance occurs, Z PB (jω rPB ) can be expressed as:
[0053]
[0054] Similarly, the port impedance Z at terminals O and BP is OB(PB) It can be expressed as:
[0055]
[0056] Comparing equation (2) and equation (3), we can find that the real part difference only exists in C ON and C P Since this test uses symmetrical ports with similar impedance for measurement, the value of D1 The voltage across the two ends remains basically unchanged, which means that CD1(PB) =C D1(OB) , while ω rPB =ω rOB =ω r Therefore, according to equations (2) and (3), the parasitic capacitance C can be obtained P and the total value C T The relationship between them is as follows:
[0057]
[0058] Rearranging the above formula, we get the parasitic capacitance C P The values are:
[0059]
[0060] (4) Reconnect the resonant inductor L r , the resonant inductor L r Connect in parallel across terminals N and O, and measure the port impedance Z from terminals N and BP NB , measure the port impedance Z from both ends of terminals O and BP OB(NB) .
[0061] Definition C OP is the equivalent capacitance from terminals O and P to BP. Due to the high frequency junction capacitance C D1 and C D2 Can be ignored, similarly C OP It can be expressed as:
[0062] C OP =C O +C P / / C D1 ≈C O +C P
[0063] Use a vector network analyzer to measure the port impedance Z at different frequencies from both ends of the terminals N and BP NB And measure the port impedance Z at different frequencies from both ends of terminals O and BP OB(NB) , we can get the real part of the impedance Re[Z NB ] and Re[Z OB(NB) ].
[0064] (5) Derivation of Z at the resonant frequency NB , Z OB(NB) The parasitic capacitance C is calculated by combining the measured value N The value of .
[0065] Z NB The expression is as follows:
[0066]
[0067] Z OB(NB) The expression is:
[0068]
[0069] Similarly, according to equations (6) and (7), the parasitic capacitance C can be obtained N and the total value C T The relationship between them is as follows:
[0070]
[0071] After rearranging the above formula, we can get the parasitic capacitance C N The values are:
[0072]
[0073] (6) According to the total value C T and the resulting C P , C N Calculate the value of parasitic capacitance C O The value of .
[0074] According to C O =C T -C P -C N Get the parasitic capacitance C O Based on this, all parasitic capacitance values are extracted.
[0075] (7) Change the external resonant inductor value and repeat the experiment to verify the accuracy of the proposed method.
[0076] To further verify the accuracy of the method of the present invention, five groups of inductance values were selected from 3.3 to 100uH as external resonant inductance values, and the experiment was repeated; Figure 6 The resonant frequency f under five sets of external inductors is shown rPB and f ROB(PB) The comparison results are Figure 7 The parasitic capacitance values extracted by the method of the present invention under five groups of external inductors are shown.
[0077] The above description of the embodiments is to facilitate the understanding and application of the present invention by those skilled in the art. It is obvious that those skilled in the art can easily make various modifications to the above embodiments and apply the general principles described herein to other embodiments without creative work. Therefore, the present invention is not limited to the above embodiments. Improvements and modifications made by those skilled in the art to the present invention based on the disclosure of the present invention should be within the protection scope of the present invention.
Claims
1. A method for extracting parasitic capacitance of an IGBT module based on external inductor resonance, wherein the IGBT module is composed of two IGBT tubes T1 and T2 connected, the collector of T1 is the terminal P of the IGBT module, the emitter of T1 is connected to the collector of T2 as the terminal O of the IGBT module, and the emitter of T2 is the terminal N of the IGBT module, characterized in that: The IGBT module parasitic capacitance extraction method comprises the following steps: (1) Measure the total parasitic capacitance C between the IGBT module copper layer and the backplane copper layer T ; (2) Connect a parallel resonant inductor between terminals P and O to achieve parallel resonance. Measure the port impedance Z between terminal P and the backplane copper layer. PB , measure the port impedance Z from terminal O to the backplane copper layer OB(PB) ; (3) According to the port impedance Z at the resonant frequency PB and Z OB(PB) , combined with the measured value, calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal P on the backplane copper layer P ; (4) Reconnect the resonant inductor and connect it in parallel between the terminals N and O. Measure the port impedance Z between the terminals N and the backplane copper layer. NB , measure the port impedance Z from terminal O to the backplane copper layer OB(NB) ; (5) According to the port impedance Z at the resonant frequency NB and Z OB(NB) , combined with the measured value, calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal N on the backplane copper layer N ; (6) Based on the total parasitic capacitance C T And the parasitic common-mode capacitance C calculated above P and C N , calculate the parasitic common mode capacitance C formed by the copper layer of the connection terminal O on the backplane copper layer O .
2. The method for extracting parasitic capacitance of an IGBT module according to claim 1, characterized in that: In step (1), since the junction capacitance of the freewheeling diodes T1 and T2 is much larger than the parasitic common-mode capacitance, the junction capacitance is regarded as a short circuit at high frequencies. Therefore, one terminal is selected from the terminals P, O, and N of the IGBT module, and the total parasitic capacitance C is measured between the terminal and the backplane copper layer. T , the measurement results are the same.
3. The method for extracting parasitic capacitance of an IGBT module according to claim 1, characterized in that: In step (2), a vector network analyzer is used to measure the port impedance Z at different frequencies from the terminal P and the backplane copper layer. PB , measure the port impedance Z at different frequencies from the terminal O and the backplane copper layer OB(PB) , record the data and draw a graph; in the step (4), a vector network analyzer is used to measure the port impedance Z at different frequencies from the terminal N and the backplane copper layer. NB , measure the port impedance Z at different frequencies from the terminal O and the backplane copper layer OB(NB) , record the data and draw a graph.
4. The method for extracting parasitic capacitance of an IGBT module according to claim 1, characterized in that: In step (3), the parasitic common-mode capacitance C is calculated by the following expression: P : Where: Z PB (jω r1 ) represents the frequency jω r1 Lower port impedance Z PB The measured value, Z OB(PB) (jω r1 ) represents the frequency jω r1 Lower port impedance Z OB(PB) The measured value, ω r1 is the resonant angular frequency, j is an imaginary unit, and Re[] represents the real part.
5. The method for extracting parasitic capacitance of an IGBT module according to claim 4, characterized in that: In step (5), the parasitic common mode capacitance C is calculated by the following expression: N : Where: Z NB (jω r2 ) represents the frequency jω r2 Lower port impedance Z NB The measured value, Z OB(NB) (jω r2 ) represents the frequency jω r2 Lower port impedance Z OB(NB) The measured value, ω r2 is the resonant angular frequency.
6. The method for extracting parasitic capacitance of an IGBT module according to claim 5, characterized in that: The resonant angular frequency ω r1 and ω r2 The expression is as follows: Where: C D1 and C D2 are the capacitance values of the freewheeling diode junction capacitances of T1 and T2, L r is the inductance value of the resonant inductor.
7. The method for extracting parasitic capacitance of an IGBT module according to claim 1, characterized in that: In step (6), the parasitic common-mode capacitance C is calculated by the following expression: O : C O =C T -C P -C N 。 8. The method for extracting parasitic capacitance of an IGBT module according to claim 1, characterized in that: The resonant inductance is changed, and five groups of inductance values are selected from 3.3 to 100 uH as the resonant inductance value to repeat steps (2) to (6), thereby verifying the accuracy and stability of the IGBT module parasitic capacitance extraction method.
9. A computer device comprising a memory and a processor, characterized in that: The memory stores a computer program, and the processor is used to execute the computer program to implement the IGBT module parasitic capacitance extraction method according to any one of claims 1 to 8.
10. A computer-readable storage medium storing a computer program, characterized in that: When the computer program is executed by a processor, the method for extracting parasitic capacitance of an IGBT module according to any one of claims 1 to 8 is implemented.
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