Design of inverter snubber circuit using measured GTO anode current waveform

Publisher:创意梦者Latest update time:2011-11-16 Source: 互联网 Reading articles on mobile phones Scan QR code
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Abstract: The snubber circuit parameter value plays a vital role in the GTO turn-off performance and the working performance of the entire GTO inverter. This paper analyzes the waveforms of the anode current and anode voltage during the GTO turn-off process and proposes a snubber circuit parameter optimization scheme with "comprehensive index" as the objective function. The optimal parameters of the GTO snubber circuit components can be determined according to the specific requirements for the GTO device performance.

Keywords: GTO buffer circuit design anode current

Chinese Library Classification Number: TM464 Document Identification Code: A Article Number: 0219-2713(2000)09-484-03

1 Introduction

The snubber circuit parameter values ​​directly affect the GTO turn-off performance and the working performance of the entire GTO inverter. Therefore, how to reasonably design the snubber circuit parameters when designing a GTO inverter becomes an important issue.

This paper analyzes the waveforms of anode current and anode voltage during the GTO shutdown process, and proposes and proves the argument that the waveform of GTO anode current is independent of the parameters of the buffer circuit, and the reverse recovery process of the buffer diode is independent of the parameters of the buffer circuit. On this basis, a simple and practical buffer circuit parameter optimization design scheme is proposed. The optimal parameters of the GTO buffer circuit components can be determined according to the specific requirements for the performance of the GTO device. When simulating the anode voltage and shutdown power consumption waveform during the GTO shutdown process, the measured anode shutdown current waveform is used to improve the simulation accuracy. The shutdown power consumption waveform is derived based on this. The simulation results are compared with the experimental waveforms, and the error is extremely small. This paper proposes a buffer circuit parameter optimization scheme with "comprehensive indicators" as the objective function.

2 Prerequisites for simulating anode voltage waveform using anode current waveform

The GTO snubber circuit can be equivalent to the circuit shown in Figure 1. If you want to use the measured anode current to simulate the anode voltage, you first need to prove that the following two conditions are true:

(1) The GTO anode current waveform has nothing to do with the buffer circuit parameters;

(2) The reverse recovery process of the snubber diode has nothing to do with the snubber circuit parameters.

2.1GTO anode current waveform has nothing to do with buffer circuit parameters

Figure 2 shows the anode current waveform when the GTO is turned off. The whole process can be divided into three stages: storage period, decline period and tail period.

In the storage period and the falling period, the storage time ts and the falling time tf values ​​only depend on the gate extraction capability and the internal structure of the GTO, and have nothing to do with the parameters of the buffer circuit. The anode current waveforms of these two periods are also independent of the parameters of the buffer circuit.

In the tail period, the tail current is basically

Figure 1 Schematic diagram of GTO buffer circuit

Figure 2 Schematic diagram of GTO anode shutdown current waveform

The above is determined by the anode current waveform and junction temperature during the falling period and has nothing to do with the buffer circuit parameters.

The eight curves in Figure 3 are the anode current and anode voltage waveforms when CS=2, 3, 4, and 5μF. It can be seen that after the buffer circuit parameters change, the anode voltage waveform changes greatly, while the four anode current curves are basically completely overlapped. This experiment verifies the correctness of the above analysis.

Curves (1), (2), (3), and (4) in the figure are the measured anode voltage waveforms after the buffer circuit parameters are changed;

Curves (5), (6), (7), and (8) are the measured anode current waveforms after the buffer circuit parameters are changed.

2.2 The reverse recovery process of the snubber diode is independent of the snubber circuit parameters

The stored charge Qr and the recovery time trr are two important parameters in the reverse recovery process of the snubber diode. When analyzing the GTO turn-off process, Qr and trr can be approximately considered constants. This can be proved by Figure 4. Figure 4 shows the snubber resistor branch current and the snubber diode branch current measured after changing the distributed inductance of the snubber resistor branch. It can be seen that after Lrs changes, irs changes greatly, while ids remains almost unchanged. It can be considered that trr is only related to the characteristics of the snubber diode itself.

Curves (1), (2), and (3) in the figure are the actual measured snubber resistor branch current waveforms before and after Lrs changes.

Curves (4), (5), and (6) are the measured snubber diode branch current waveforms before and after Lrs changes;

Figure 3 Anode current and anode voltage waveforms after buffer circuit parameters are changed

As shown in Figure 5, the reverse recovery characteristic curve of the buffer diode, the current on the buffer diode after t>t5 is approximately considered to be a quadratic curve, which can better illustrate the problem. The curve equation is: (1)(2)

Where trr is the buffer diode recovery time;

t5—time when ids=Ism;

Ido—the current value of the buffer diode when t=t7.

Figure 4 Ids, Irs waveforms after the snubber diode recovers its reverse blocking capability

3 Anode voltage waveform simulation

By using the mathematical model between the GTO anode voltage and anode current and computer simulation using MATLAB language, the simulated waveform of the anode voltage can be obtained from the measured anode current waveform and buffer circuit parameters. The simulated waveform has a very small error compared to the measured waveform. As shown in Figure 6, the curves in the figure are the actual measured anode voltage waveform and the corresponding simulated waveform under the conditions of CS=2μF and 5μF. It can be seen that the simulation accuracy can meet the optimization requirements.

4 Buffer circuit parameter optimization design scheme

4.1 Determination of the objective function

The following specifically discusses the indicators that can be used to determine whether the buffer circuit parameter settings are reasonable.

Figure 5 Reverse recovery characteristics of snubber diode

(1) There are several extremely important dynamic parameters in the GTO turn-off process, including peak voltage Up, peak power consumption Pfm, anode voltage rise rate dua/dt, and anode voltage peak UDM. If these dynamic parameters are too high, the GTO will fail, that is, the GTO's tolerance to these dynamic parameters is limited. Assume that the limit values ​​of these dynamic parameters are (Up)m, (Pfm)m, (UDM)m, (dua/dt)m, and (Urm-E)m. It can be seen that the smaller the ratio of the dynamic parameter value to its limit value during the GTO turn-off process, the better the working performance of the GTO device. Since the dynamic parameter value in practical use is closely related to the buffer circuit parameters, it can be said that once the GTO and gate drive circuit are determined, the dynamic parameter value of the GTO when it is turned off will depend on the buffer circuit parameters. Therefore, the ratio of the dynamic parameter value during actual operation to the limit value it can withstand, including Up/(Up)m, UDM/(UDM)m, (dua/dt)/(dua/dt)m, Pfm/(Pfm)m, (Urm-E)m, can be used as an indicator to measure whether the buffer circuit parameter settings are reasonable. The smaller these ratios are, the better the buffer circuit parameter settings are.

(2) The GTO turn-off energy consumption Eoff and the buffer circuit energy consumption Esb during the GTO operation process are important parameters for measuring the working performance of the GTO device. If these parameters are too large, although the GTO may not fail in a short time, it will increase the energy consumption of the entire device, thereby affecting the working stability and reliability of the device. Therefore, we can use the ratio of Eoff, Esb to a specific value (Eoff)m, (Esb)m as an indicator to measure the performance of the GTO device. Because Eoff and Esb are closely related to the buffer circuit parameters, the above two ratios Eoff/(Eoff)m and Esb/(Esb)m can also be used as indicators to measure whether the buffer circuit parameter settings are reasonable. The smaller these two ratios are, the better the buffer circuit parameter settings are.

(3) The turn-on time ton and turn-off time toff of GTO are directly related to the size of the operating frequency limit value of the entire GTO device. The smaller ton and toff are, the higher the operating frequency of the GTO device can be. Its limit value is fmax=1/(ton+toff). Therefore, the values ​​of ton and toff are related to the working performance of the entire device. The ratio of ton+toff to a certain value tm can be used as an indicator to measure the frequency performance of the GTO device. Similarly, the size of ton and toff is closely related to the parameters of the buffer circuit. For example, if the buffer circuit parameters are CS and RS, it is impossible to make the GTO turn-on time lower than 5RSCS. Therefore, (ton+toff)/tm can be used as an indicator to measure whether the buffer circuit parameter settings are reasonable. The smaller this ratio is, the better the buffer circuit parameter settings are. Among them, tm can be defined as the switching time when CS and RS take the upper limit of the optimization space.

(4) Considering that the improvement of the dynamic characteristics of the buffer diode will lead to the deterioration of its power characteristics. The ratio of the stored charge Qr to its specific value Qr/(Qr)m and the ratio of the recovery time trr to a specific value trr/(trr)m can be used as indicators to measure the power characteristics of the GTO device, and are also indicators reflecting the working performance of the GTO device. The smaller the two ratios, the better the buffer circuit parameters. Among them: (Qr)m, (trr)m can be defined as the upper limit of the actual optimization space.

From the above analysis, it can be seen that the objective function J of the snubber circuit optimization can be defined as: where (Up)m, (UDM)m, (dUa/dt)m, (Pfm)m, and (Urm-E)m are the limit values ​​of the dynamic parameters during the GTO turn-off process;

Up, UDM, dua/dt, Pfm are GTO dynamic parameter values ​​under specific conditions;

Figure 6 Comparison of GTO simulation waveform and measured waveform

(Eoff)m, (Esb)m, tm are specific values ​​determined according to actual requirements;

k1, k2, k3, k4 are coefficients determined according to the importance of each indicator. Their values ​​can be determined according to specific requirements, and generally k2>k1>k3>k4.

4.2 Determination of Constraints

The dynamic parameter limit values ​​that the GTO can withstand during the shutdown process can be used as optimization constraints. Specifically, there are the following items:

①Up<(Up)m; ② UDM<(UDM)m; ③ dua/dt<(dua/dt)m; ④ Pfm<(Pfm)m; ⑤ (E- Urm)<(E- Urm)m; ⑥ ton+ toff<1/f, f is the operating frequency of the GTO device.

4.3 Optimization Program Flowchart

As shown in Figure 7, in the block diagram, (Cs)max, (Cs)min, (Rs)max, (Rs)min, (Qr)max, (Qr)min, (trr)max, (trr)min are the upper and lower limits of the optimization space; N1, N2, N3, N4 are step size coefficients.

4.4 Optimization program operation results

Figure 7 Optimization program flowchart

Optimization design purpose: KG-91-2-5GTO is used in a GTO chopper with working parameters of 600A and 1000V. The rated parameters of GTO are 1000A and 2300V. Determine the optimal snubber circuit parameters.

Determination of optimization program parameters:

(1) Determination of the optimization space

CS: from 1μF to 10μF, the step size is set to 1μF, that is, N1=9;

RS: from 1Ω to 21Ω, the step size is set to 5Ω, that is, N2=4;

Qr: from 100μC to 400μC, the step size is set to 100μC, that is, N3=3;

trr: from 1μs to 7μs, the step size is set to 2μs, that is, N4=3;

(2) Determination of objective function

Taking into account the large difference between the actual operating parameters of GTO and its rated parameters, a larger K2 is selected when determining the objective function to highlight the energy consumption index so that the device has lower energy consumption when working under the optimized parameter conditions.

Actual selection:

K1=1; K2=5; K3=2; K4=1.

Program running results:

Minimum value of objective function: Jmin=16.74;

Optimal snubber circuit parameters: CS = 3μF; RS = 6Ω;

Qr=200μC; trr=3μs.

Reference address:Design of inverter snubber circuit using measured GTO anode current waveform

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