CN113064042A - Junction temperature extraction method of power semiconductor device - Google Patents

Junction temperature extraction method of power semiconductor device Download PDF

Info

Publication number
CN113064042A
CN113064042A CN202110134810.6A CN202110134810A CN113064042A CN 113064042 A CN113064042 A CN 113064042A CN 202110134810 A CN202110134810 A CN 202110134810A CN 113064042 A CN113064042 A CN 113064042A
Authority
CN
China
Prior art keywords
voltage
drain
source
gate
electrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN202110134810.6A
Other languages
Chinese (zh)
Other versions
CN113064042B (en
Inventor
刁利军
刘博�
王磊
刁利坚
刘新博
任家辉
张艳
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beijing Tongli Zhida Technology Co ltd
Beijing Jiaotong University
Original Assignee
Beijing Tongli Zhida Technology Co ltd
Beijing Jiaotong University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Beijing Tongli Zhida Technology Co ltd, Beijing Jiaotong University filed Critical Beijing Tongli Zhida Technology Co ltd
Priority to CN202110134810.6A priority Critical patent/CN113064042B/en
Publication of CN113064042A publication Critical patent/CN113064042A/en
Application granted granted Critical
Publication of CN113064042B publication Critical patent/CN113064042B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/26Testing of individual semiconductor devices
    • G01R31/2601Apparatus or methods therefor
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/30Circuit design
    • G06F30/36Circuit design at the analogue level
    • G06F30/367Design verification, e.g. using simulation, simulation program with integrated circuit emphasis [SPICE], direct methods or relaxation methods

Landscapes

  • Engineering & Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • Testing Of Individual Semiconductor Devices (AREA)

Abstract

The invention relates to a junction temperature extraction method of a power semiconductor device, which is characterized in that a double-pulse experimental circuit is built through simulation software, a SiC MOSFET is taken as an example, the SiC MOSFET is selected as a switching tube, and the drain-source voltage v of the power device is measureddsThe voltage peak and the junction temperature of the power semiconductor are analyzed to find out the causes of the voltage peak, including transconductance coefficient, gate threshold voltage and gate-drain capacitance, and the influencing factors are also influenced by the junction temperature, and the junction temperature and the turn-off voltage peak have negative corresponding relation through simulation experiment. The method has good shielding effect on voltage fluctuation at two ends of the switching tube, and only needs to measure the drain-source voltage vdsThe junction temperature can be obtained through the peak, and compared with other junction temperature extraction methods, the method has the advantages that the reading is easier and the accuracy is higher in the measurement process.

Description

Junction temperature extraction method of power semiconductor device
Technical Field
The invention relates to the technical field of semiconductor device testing, in particular to a junction temperature extraction method of a power semiconductor device.
Background
Power semiconductor devices are widely used in many fields such as communications, traffic, and electric power, and are being developed in the direction of high voltage, high frequency, and high power. The high safety requirements of the above systems have increased the reliability requirements of the power devices. One of the main sources of failure of power converters is failure of the power devices, which is mainly from thermal stress. The higher the working junction temperature of the device is, the smaller the safe operation margin is; the larger the junction temperature fluctuation, the shorter the thermal cycle life. In the normal working temperature range, the failure rate of the device is doubled when the junction temperature of the device rises by 10 ℃. Therefore, monitoring the operating junction temperature of the power device is critical for failure mechanism analysis and life prediction. In addition, junction temperature monitoring provides data support for state monitoring, reliability evaluation and thermal balance control of the power device, and therefore the power device is possible.
At present, a heat sensor method, an infrared thermal imaging method, a thermal sensitive electrical parameter method and an RC thermal resistance network method are provided by research, wherein the thermal sensitive electrical parameter method is distinguished by different thermal sensitive electrical parameters, the method taking voltage change rate as the thermal sensitive electrical parameter is easily affected by disturbance, the method taking conduction voltage drop as the thermal sensitive electrical parameter is difficult to ensure precision, the method taking threshold voltage as the thermal sensitive electrical parameter is difficult to ensure precision, the method taking maximum current change rate as the thermal sensitive electrical parameter is difficult to integrate measurement, and a systematic comprehensive thermal sensitive electrical parameter method is not provided.
The problems that accuracy is difficult to guarantee due to low sensitivity of temperature-sensitive electrical parameters, integration of measuring devices is difficult due to high measuring difficulty, results are easily affected by disturbance due to selection of inappropriate temperature-sensitive electrical parameters, and the like, are urgently needed to be solved by technical personnel in the field, and therefore, a junction temperature extraction method designed for a power semiconductor device is very necessary.
Disclosure of Invention
Aiming at the defects in the prior art, the invention aims to provide a junction temperature extraction method of a power semiconductor device. The invention designs from the direction of software, measures the peak of the turn-off voltage, finds the corresponding relation between the peak of the turn-off voltage and the junction temperature through a simulation experiment, and further achieves the purpose of extracting the junction temperature. The measurement of the turn-off voltage spike can effectively avoid measurement errors caused by drain-source voltage fluctuation, and the measurement process is simple in reading and high in accuracy.
The invention analyzes the relation between the cut-off voltage peak and the extracted junction temperature through simulation software, and analyzes the relation between the extracted junction temperature and the transconductance coefficient, the threshold voltage and the gate-drain capacitance.
With the increase of the junction temperature of the semiconductor device, the transconductance coefficient is reduced, the threshold voltage is reduced, and the gate-drain capacitance is increased, the variation of the four intermediate quantities finally causes the peak of the turn-off voltage to be reduced, and the relation between the junction temperature and the peak of the turn-off voltage can be obtained according to the relation.
And (3) under the condition of considering different junction temperatures of the semiconductor device, combining a double-pulse test circuit and designing simulation software to carry out experiments.
In order to achieve the above purposes, the technical scheme adopted by the invention is as follows:
a double pulse test circuit comprising: DC power supply UsDouble pulse generator, support capacitor CoHollow inductor L0A silicon carbide MOSFET power cell and a negative voltage source DC,
the silicon carbide MOSFET power cell comprises an upper tube and a lower tube;
the DC power supply UsPositive electrode and supporting capacitor CoIs connected with the DC power supply UsNegative electrode of and supporting capacitor CoIs connected at the other endSupporting capacitor CoOne end of the capacitor is connected with the drain electrode of the upper tube to support the capacitor CoThe other end of the lower tube is connected with the source electrode of the lower tube;
the hollow inductor L0In parallel with the lower tube;
the double-pulse generator is connected with the grid of the upper tube;
the negative electrode of the negative voltage source DC is connected with the grid electrode of the lower tube, and the positive electrode of the negative voltage source DC is connected with the source electrode of the lower tube.
On the basis of the above scheme, the equivalent circuit of the upper tube is the same as that of the lower tube, and the equivalent circuit of the upper tube comprises: drive resistor RgGate inductance LgGate-drain capacitor CgdGate source capacitance CgsA drain electrode inductance LdDrain-source capacitance CdsMOSFET and source electrode inductance Ls
The driving resistor RgAnd gate inductance LgIs connected to the gate inductance LgThe other end of the MOSFET is connected with the grid electrode of the MOSFET, and a grid leakage capacitor C is arranged between the grid electrode and the drain electrode of the MOSFETgdA gate-source capacitor C is arranged between the gate and the source of the MOSFETgsA drain-source capacitor C is arranged between the drain electrode and the source electrode of the MOSFETdsThe drain electrode of the MOSFET is also connected with a drain electrode inductor LdThe source electrode of the MOSFET is also connected with a source electrode inductor Ls
On the basis of the scheme, the double-pulse generator and the driving resistor RgConnection, drain inductance LdAnd a support capacitor CoIs connected to the source electrode inductance LsConnected to the drain of the lower tube.
A junction temperature extraction method of a power semiconductor device applies the double-pulse test circuit and comprises the following steps:
step 1, building a double-pulse test circuit by using Simplorer simulation software;
before the measurement is started, 5V negative pressure is provided for a grid electrode of the lower tube, and the turn-off of the lower tube is ensured;
sending double pulse signals to the upper tube, observing the current i flowing through the upper tube by an oscilloscopedAnd an upper pipeVoltage v acrossdsThe waveform of (a);
step 2, after reading the turn-off voltage peak, analyzing according to a formula (1);
Figure BDA0002926470250000031
wherein igRepresents the drive current, CgsRepresenting gate-source capacitance, vgsRepresenting the gate-source voltage, CgdIndicating gate-drain capacitance, vdsRepresenting the drain-source voltage, VPLIndicating driving negative pressure, RgDenotes the drive resistance, LsRepresents the source inductance, igsIndicating the flow through the gate-source capacitance CgsCurrent of (i)dDenotes the drain current, VDCRepresenting a direct voltage, LloopRepresenting power loop inductance, gfsRepresenting the transconductance coefficient;
the formula of the current transformation rate is derived from the formula (1):
Figure BDA0002926470250000041
wherein, VmWhich is a representation of the voltage of the miller voltage,
the turn-off voltage spike Δ V is derived from equation (2)dsThe formula:
Figure BDA0002926470250000042
wherein ILRepresenting the load current, VthWhich is indicative of the threshold voltage of the transistor,
this equation shows that the turn-off voltage spike is subject to a threshold voltage VthGate-drain capacitor CgdAnd a transconductance coefficient gfsThe influence of (c).
The formula [ Delta ] V is obtained from the formula (3)ds=f(gfs,Cgd,Vth) And f represents a functional relationship,
by analyzing the internal working process of the MOSFET, the following results are obtained: threshold voltage VthTransconductance coefficient gfsHaving a negative temperature coefficient, gate-drain capacitance CgdHaving a positive temperature coefficient, threshold voltage VthTransconductance coefficient gfsReduced sum-gate-drain capacitance CgdBoth increases cause a reduction in the off-voltage spike;
thus, the junction temperature TjThe rise will result in Δ VdsDecrease;
for off peak voltage Δ Vds=f(gfs,Cgd,Vth)=g(Tj) Is transformed to obtain Tj=h(gfs,Cgd,Vth)=k(ΔVds),TjRepresenting a functional relation of g, h and k for the junction temperature of the semiconductor device;
step 3, after the measurement is finished, releasing the support capacitor C to ensure the safety of the working personneloTo the energy of (c).
The invention has the beneficial effects that:
1. the technical scheme has simple measurement and convenient data acquisition;
2. the method has good shielding effect on voltage fluctuation at two ends when the switching tube is turned off;
3. the selected thermosensitive electrical parameters have good sensitivity and high accuracy;
4. a plurality of intermediate variables are considered in a single thermosensitive electrical parameter, so that the system performance is better, and the accuracy is high;
5. and a plurality of intermediate variables are not required to be measured, so that the measurement cost is reduced.
Drawings
The invention has the following drawings:
FIG. 1 is a schematic diagram of a test circuit of the present invention;
FIG. 2 is a diagram of an equivalent circuit of a SiC MOSFET tested in accordance with the present invention;
FIG. 3 is an idealized overall process waveform diagram of the test circuit of the present invention;
FIG. 4 is a graph of drain-source voltage waveforms at different temperatures for the test circuit of the present invention;
FIG. 5 is a schematic diagram of the turn-off voltage spike and its influencing factors of the present invention;
fig. 6 is a plot of junction temperature versus turn-off voltage spike for the present invention.
Detailed Description
The invention is described in further detail below with reference to figures 1-6.
The embodiment of the invention provides a junction temperature extraction method of a power semiconductor device, which comprises the following steps: the corresponding relation between the turn-off voltage peak and the junction temperature is found through simulation experiments, and the purpose of extracting the junction temperature is further achieved. The measurement of the turn-off voltage spike can effectively avoid measurement errors caused by drain-source voltage fluctuation, and the measurement process is simple in reading and high in accuracy.
Firstly, the relation between a turn-off voltage peak and the extracted junction temperature is analyzed through simulation software, and the relation between the extracted junction temperature and a transconductance coefficient, a threshold voltage and a gate-drain capacitance is analyzed, wherein fig. 1 is a double-pulse test circuit built in a verification experiment of the method. The test circuit includes: DC power supply UsDouble pulse generator, support capacitor CoHollow inductor L0A silicon carbide MOSFET power cell and a negative voltage source DC,
the silicon carbide MOSFET power cell comprises an upper tube and a lower tube;
the DC power supply UsPositive electrode and supporting capacitor CoIs connected with the DC power supply UsNegative electrode of and supporting capacitor CoIs connected with the other end of the supporting capacitor CoOne end of the capacitor is connected with the drain electrode of the upper tube to support the capacitor CoThe other end of the lower tube is connected with the source electrode of the lower tube;
the hollow inductor L0In parallel with the lower tube;
the double-pulse generator is connected with the grid of the upper tube;
the negative electrode of the negative voltage source DC is connected with the grid electrode of the lower tube, and the positive electrode of the negative voltage source DC is connected with the source electrode of the lower tube.
On the basis of the above scheme, the equivalent circuit of the upper tube is the same as that of the lower tube, and as shown in fig. 2, the equivalent circuit of the upper tube includes: drive resistor RgGate inductance LgGate-drain capacitor CgdGate source capacitance CgsA drain electrode inductance LdDrain-source capacitance CdsMOSFET and source electrode inductance Ls
The driving resistor RgAnd gate inductance LgIs connected to the gate inductance LgThe other end of the MOSFET is connected with the grid electrode of the MOSFET, and a grid leakage capacitor C is arranged between the grid electrode and the drain electrode of the MOSFETgdA gate-source capacitor C is arranged between the gate and the source of the MOSFETgsA drain-source capacitor C is arranged between the drain electrode and the source electrode of the MOSFETdsThe drain electrode of the MOSFET is also connected with a drain electrode inductor LdThe source electrode of the MOSFET is also connected with a source electrode inductor Ls
On the basis of the scheme, the double-pulse generator and the driving resistor RgConnection, drain inductance LdAnd a support capacitor CoIs connected to the source electrode inductance LsConnected to the drain of the lower tube.
With the increase of the junction temperature of the semiconductor device, the transconductance coefficient is reduced, the threshold voltage is reduced, and the gate-drain capacitance is increased, the variation of the four intermediate quantities finally causes the peak of the turn-off voltage to be reduced, and the relation between the junction temperature and the peak of the turn-off voltage can be obtained according to the relation.
And (3) under the condition of considering different junction temperatures of the semiconductor device, combining a double-pulse test circuit and designing simulation software to carry out experiments.
The test method is a method for analyzing the relation between the junction temperature of a semiconductor and a turn-off voltage peak through simulation experiment test and further determining the junction temperature through the turn-off voltage peak, and specifically comprises the following steps of:
step 1, building a double-pulse test circuit by using Simplorer simulation software;
before the measurement is started, 5V negative pressure is provided for a grid electrode of the lower tube, and the turn-off of the lower tube is ensured;
sending double pulse signals to the upper tube, observing the current i flowing through the lower tube by an oscilloscopedAnd the voltage v across the lower tubedsThe waveform of (a);
hollow inductor L0Freewheeling through a schottky freewheeling diode in the lower tube;
in the testing process, the tube is reliably turned off, and a Schottky freewheeling diode in the tube plays a freewheeling role;
FIG. 3 is an idealized overall process waveform diagram of the test circuit of the present invention;
the circuit working process can be divided into three stages, as shown in fig. 3;
t0at the moment, the grid of the upper tube Q1 receives the first pulse, Q1 is in saturated conduction, and the capacitor C is supportedoThe voltage U is applied to the hollow inductor L0Two-terminal, air-core inductor L0Current (sum i) ofdIs the same current) rises linearly;
t1tube Q1 is turned off at any moment, and air core inductor L0The current on the inductor is follow current of a Q2 parallel diode and an air core inductor L0The current above decays slowly, as t in fig. 31And t2I measured as a dashed line between timesdThen decay to 0 soon;
t2at the moment the tube Q1 is turned on again, the diode of Q2 enters reverse recovery, which will pass through Q1, resulting in a current i of Q1dA sharp rise, as shown in fig. 3;
t3at the moment, the tube is turned off again, and because the current of the Q1 turned off at the moment is large, v of the Q1 can be caused due to the existence of stray inductance of the busdsGenerating a voltage spike;
step 2, after the off-voltage peak is read by an oscilloscope, analyzing according to a formula (1);
Figure BDA0002926470250000071
the formula of the current change rate can be obtained by the formula (1)
Figure BDA0002926470250000072
Formula (2) can be used to derive the formula of the turn-off voltage spike
Figure BDA0002926470250000073
This equation shows that the turn-off voltage spike is subject to a threshold voltage VthGate-drain capacitor CgdAnd a transconductance coefficient gfsThe influence of (c).
The formula [ Delta ] V is obtained from the formula (3)ds=f(gfs,Cgd,Vth) And f represents a functional relationship.
Obtained by analyzing the internal working process of the MOSFET, Vth、gfsHaving a negative temperature coefficient and a gate-drain capacitance CgdHaving a positive temperature coefficient, i.e. Vth、gfsDecrease and CgdThe increase will cause a reduction in the off-voltage spike.
Thus, the junction temperature TjThe rise will result in Δ VdsAnd decreases.
For off peak voltage Δ Vds=f(gfs,Cgd,Vth)=g(Tj) Is transformed to obtain Tj=h(gfs,Cgd,Vth)=k(ΔVds),TjRepresenting a functional relation of g, h and k for the junction temperature of the semiconductor device;
step 3, after the measurement is finished, releasing the support capacitor C to ensure the safety of the working personneloTo the energy of (c).
FIG. 4 is a drain-source voltage waveform at different temperatures for the test circuit of the present invention;
the graph shows that the turn-off voltage spike gradually decreases with increasing junction temperature, validating the present invention.
FIG. 5 is a schematic diagram of the turn-off voltage spike and its influencing factors of the present invention;
the graph shows that the increase in junction temperature affects the threshold voltage, the gate-drain capacitance, and the transconductance coefficient, which all affect the turn-off voltage spike drop.
FIG. 6 is a plot of junction temperature versus turn-off voltage spike quantification of the present invention;
example 1
The method of the invention is carried out on SiC MOSFET under the drain-source voltage current level of 700V/300ATesting when the junction temperature is 25-150 ℃, processing data by a linear regression method to obtain the junction temperature TjThe relationship to the off-voltage spike is as follows:
Tj=-9.212ΔVds+3332.76 (4)
the negative linear relationship between the junction temperature and the drain-source voltage displayed after data processing illustrates the effectiveness of the method provided by the invention.
It should be noted that the above-described embodiments are not intended to limit the scope of the present invention, but are to be accorded the widest scope consistent with the principles and novel features disclosed herein, including but not limited to SiC MOSFETs and Si IGBTs.
Those not described in detail in this specification are within the skill of the art.

Claims (4)

1. A double pulse test circuit, comprising: DC power supply UsDouble pulse generator, support capacitor CoHollow inductor L0A silicon carbide MOSFET power cell and a negative voltage source DC,
the silicon carbide MOSFET power cell comprises an upper tube and a lower tube;
the DC power supply UsPositive electrode and supporting capacitor CoIs connected with the DC power supply UsNegative electrode of and supporting capacitor CoIs connected with the other end of the supporting capacitor CoOne end of the capacitor is connected with the drain electrode of the upper tube to support the capacitor CoThe other end of the lower tube is connected with the source electrode of the lower tube;
the hollow inductor L0In parallel with the lower tube;
the double-pulse generator is connected with the grid of the upper tube;
the negative electrode of the negative voltage source DC is connected with the grid electrode of the lower tube, and the positive electrode of the negative voltage source DC is connected with the source electrode of the lower tube.
2. The double-pulse test circuit of claim 1, wherein the equivalent circuit of the top tube is the same as the equivalent circuit of the bottom tube, the equivalent circuit of the top tube comprising: driving deviceDynamic resistor RgGate inductance LgGate-drain capacitor CgdGate source capacitance CgsA drain electrode inductance LdDrain-source capacitance CdsMOSFET and source electrode inductance Ls
The driving resistor RgAnd gate inductance LgIs connected to the gate inductance LgThe other end of the MOSFET is connected with the grid electrode of the MOSFET, and a grid leakage capacitor C is arranged between the grid electrode and the drain electrode of the MOSFETgdA gate-source capacitor C is arranged between the gate and the source of the MOSFETgsA drain-source capacitor C is arranged between the drain electrode and the source electrode of the MOSFETdsThe drain electrode of the MOSFET is also connected with a drain electrode inductor LdThe source electrode of the MOSFET is also connected with a source electrode inductor Ls
3. The double-pulse test circuit of claim 2, wherein the double-pulse generator and the drive resistor RgConnection, drain inductance LdAnd a support capacitor CoIs connected to the source electrode inductance LsConnected to the drain of the lower tube.
4. A junction temperature extraction method for a power semiconductor device, which applies the double-pulse test circuit as claimed in any one of the claims 1 to 3, and is characterized by comprising the following steps:
step 1, building a double-pulse test circuit by using Simplorer simulation software;
before the measurement is started, 5V negative pressure is provided for a grid electrode of the lower tube, and the turn-off of the lower tube is ensured;
sending double pulse signals to the upper tube, observing the current i flowing through the upper tube by an oscilloscopedAnd voltage v across the upper tubedsThe waveform of (a);
step 2, after reading the turn-off voltage peak, analyzing according to a formula (1);
Figure FDA0002926470240000021
wherein igRepresents the drive current, CgsRepresenting gate-source capacitance, vgsRepresenting the gate-source voltage, CgdIndicating gate-drain capacitance, vdsRepresenting the drain-source voltage, VPLIndicating driving negative pressure, RgDenotes the drive resistance, LsRepresents the source inductance, igsIndicating the flow through the gate-source capacitance CgsCurrent of (i)dDenotes the drain current, VDCRepresenting a direct voltage, LloopRepresenting power loop inductance, gfsRepresenting the transconductance coefficient;
the formula of the current transformation rate is derived from the formula (1):
Figure FDA0002926470240000022
wherein, VmWhich is a representation of the voltage of the miller voltage,
the turn-off voltage spike Δ V is derived from equation (2)dsThe formula:
Figure FDA0002926470240000023
wherein ILRepresenting the load current, VthWhich is indicative of the threshold voltage of the transistor,
equation (3) shows that the turn-off voltage spike is subjected to a threshold voltage VthGate-drain capacitor CgdAnd a transconductance coefficient gfsThe influence of (a);
the formula [ Delta ] V is obtained from the formula (3)ds=f(gfs,Cgd,Vth) And f represents a functional relationship,
by analyzing the internal working process of the MOSFET, the following results are obtained: threshold voltage VthTransconductance coefficient gfsHaving a negative temperature coefficient, gate-drain capacitance CgdHaving a positive temperature coefficient, threshold voltage VthTransconductance coefficient gfsReduced sum-gate-drain capacitance CgdBoth increases cause a reduction in the off-voltage spike;
thus, the junction temperature TjThe rise will result in Δ VdsDecrease;
for off peak voltage Δ Vds=f(gfs,Cgd,Vth)=g(Tj) Is transformed to obtain Tj=h(gfs,Cgd,Vth)=k(ΔVds),TjRepresenting a functional relation of g, h and k for the junction temperature of the semiconductor device;
step 3, after the measurement is finished, releasing the support capacitor C to ensure the safety of the working personneloTo the energy of (c).
CN202110134810.6A 2021-02-01 2021-02-01 Junction temperature extraction method of power semiconductor device Active CN113064042B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202110134810.6A CN113064042B (en) 2021-02-01 2021-02-01 Junction temperature extraction method of power semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202110134810.6A CN113064042B (en) 2021-02-01 2021-02-01 Junction temperature extraction method of power semiconductor device

Publications (2)

Publication Number Publication Date
CN113064042A true CN113064042A (en) 2021-07-02
CN113064042B CN113064042B (en) 2022-02-08

Family

ID=76558690

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202110134810.6A Active CN113064042B (en) 2021-02-01 2021-02-01 Junction temperature extraction method of power semiconductor device

Country Status (1)

Country Link
CN (1) CN113064042B (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113325292A (en) * 2021-07-09 2021-08-31 华北电力大学 Power semiconductor device gate oxide performance parameter measuring circuit and measuring method thereof
CN115951192A (en) * 2023-03-09 2023-04-11 长沙丹芬瑞电气技术有限公司 Junction temperature detection device, method and medium of power device
CN116466155A (en) * 2023-03-24 2023-07-21 浙江伊控动力系统有限公司 Method for reducing high-temperature voltage stress of SiC module by dividing Bin

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008054098A (en) * 2006-08-25 2008-03-06 Nissan Motor Co Ltd Driving circuit of voltage driving element
CN109444706A (en) * 2018-11-16 2019-03-08 国网江苏省电力有限公司盐城供电分公司 A kind of power electronic devices dynamic switching characteristic test method
CN109557828A (en) * 2018-10-31 2019-04-02 西安理工大学 A kind of SiCMOSFET simulation circuit model parameters precision bearing calibration
US20190376850A1 (en) * 2018-06-07 2019-12-12 General Electric Company Systems and methods for monitoring junction temperature of a semiconductor switch
CN111460748A (en) * 2020-03-24 2020-07-28 北京交通大学 Method for establishing SiC MOSFET short circuit simulation model
CN112001127A (en) * 2020-08-28 2020-11-27 河北工业大学 IGBT junction temperature prediction method

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008054098A (en) * 2006-08-25 2008-03-06 Nissan Motor Co Ltd Driving circuit of voltage driving element
US20190376850A1 (en) * 2018-06-07 2019-12-12 General Electric Company Systems and methods for monitoring junction temperature of a semiconductor switch
CN109557828A (en) * 2018-10-31 2019-04-02 西安理工大学 A kind of SiCMOSFET simulation circuit model parameters precision bearing calibration
CN109444706A (en) * 2018-11-16 2019-03-08 国网江苏省电力有限公司盐城供电分公司 A kind of power electronic devices dynamic switching characteristic test method
CN111460748A (en) * 2020-03-24 2020-07-28 北京交通大学 Method for establishing SiC MOSFET short circuit simulation model
CN112001127A (en) * 2020-08-28 2020-11-27 河北工业大学 IGBT junction temperature prediction method

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
DAN ZHENG等: "Monitoring of SiC MOSFET Junction Temperature with On-state Voltage at High Currents", 《CHINESE JOURNAL OF ELECTRICAL ENGINEERING》 *
HUI LI等: "Analysis of Voltage Variation in Silicon Carbide MOSFETs during Turn-On and Turn-Off", 《ENERGIES》 *
任磊等: "电力电子电路中功率晶体管结温在线测量技术研究现状", 《电工技术学报》 *

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113325292A (en) * 2021-07-09 2021-08-31 华北电力大学 Power semiconductor device gate oxide performance parameter measuring circuit and measuring method thereof
CN115951192A (en) * 2023-03-09 2023-04-11 长沙丹芬瑞电气技术有限公司 Junction temperature detection device, method and medium of power device
CN116466155A (en) * 2023-03-24 2023-07-21 浙江伊控动力系统有限公司 Method for reducing high-temperature voltage stress of SiC module by dividing Bin
CN116466155B (en) * 2023-03-24 2024-05-07 浙江伊控动力系统有限公司 Method for reducing high-temperature voltage stress of SiC module by dividing Bin

Also Published As

Publication number Publication date
CN113064042B (en) 2022-02-08

Similar Documents

Publication Publication Date Title
CN113064042B (en) Junction temperature extraction method of power semiconductor device
US10605854B2 (en) Method for estimating power system health
Pu et al. In situ degradation monitoring of SiC MOSFET based on switching transient measurement
US9683898B2 (en) Method and apparatus for determining an actual junction temperature of an IGBT device
Pu et al. A practical on-board SiC MOSFET condition monitoring technique for aging detection
Jiang et al. Online junction temperature measurement for SiC MOSFET based on dynamic threshold voltage extraction
CN106771951A (en) Electronic power switch device junction temperature on-Line Monitor Device, detection circuit and method of testing
CN105510793B (en) A kind of self-calibrating method of current transformer IGBT power module junction temperature measurement
CN110658435B (en) IGBT junction temperature monitoring device and method
Zhang et al. Online junction temperature monitoring using turn-off delay time for silicon carbide power devices
Pu et al. SiC MOSFET aging detection based on Miller plateau voltage sensing
Qiao et al. Online junction temperature monitoring for SiC MOSFETs using turn-on delay time
Brandelero et al. Online junction temperature measurements for power cycling power modules with high switching frequencies
Gonzalez et al. Bias temperature instability and condition monitoring in SiC power MOSFETs
CN206362890U (en) Electronic power switch device junction temperature on-Line Monitor Device, detection circuit
CN114839499A (en) Power device junction temperature on-line monitoring system based on dynamic threshold voltage
Zheng et al. Monitoring of SiC MOSFET junction temperature with on-state voltage at high currents
Rizzo et al. Intrusiveness of power device condition monitoring methods: Introducing figures of merit for condition monitoring
Liu et al. Online junction temperature extraction and aging detection of IGBT via Miller plateau width
Wang et al. Condition monitoring of SiC MOSFETs based on gate-leakage current estimation
Sharma et al. A robust approach for characterization of junction temperature of SiC power devices via quasi-threshold voltage as temperature sensitive electrical parameter
Pu et al. On-board SiC MOSFET degradation monitoring through readily available inverter current/voltage sensors
CN113376497A (en) Online monitoring method suitable for junction and aging information of power semiconductor device
Shi et al. A current sensorless IGBT junction temperature extraction method via parasitic parameters between power collector and auxiliary collector
CN116106714A (en) Real-time online junction temperature extraction circuit capable of adjusting turn-on delay time

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant