evectra_main_Blog1_1x1_as

05/07/2013

Proteja IGBTs com Sensores de Corrente Usando Amplificadores com Isolação Óptica

Protect IGBTs By Sensing Current Using Optical Isolation Amplifiers 


Fonte: powerelectronics.  Protect IGBTs By Sensing Current Using Optical Isolation Amplifiers
 [online].  Disponível na Internet via URL:  http://powerelectronics.com/power-management/protect-igbts-sensing-current-using-optical-isolation-amplifiers.  Arquivo capturado em 07.05.2013.

Insulated-gate bipolar transistors (IGBTs) require full protection to avoid damage and failures resulting from conditions such as short circuits, overloads and overvoltages. The protection is key to ensuring safe and stable power-converter operations in applications such as motor drives and solar and wind power generation systems. To detect over-current and overload conditions, isolation amplifiers featuring fast response or fast fault feedback can be used on the output phases and the DC bus.


Fig. 1 . shows a typical block diagram of a power converter in an AC motor drive.It consists of an inverter that converts the DC bus voltage to AC power at a variable frequency to drive the motor. IGBTs are expensive power switches that form the heart of the inverter. These power devices must operate at a high frequency and must be able to withstand high voltages.


Isolation amplifiers (iso-amps), such as the ACPL-C79A (Fig. 2. ), work in conjunction with shunt resistors to provide accurate current measurements in power converters even in the presence of high switching noise. When used with a resistive divider, iso-amps work as precision voltage sensors to monitor the DC bus voltage. The current and voltage information from the iso-amps are collected by the microcontroller, which uses the data to calculate the feedback values and output signals needed to provide effective control and fault management in the power converters.
Fault Protection
In an inverter, the IGBTs are the most costly components and thus it makes sense to provide as much protection as possible to protect them from damage.The iso-amps provide quick sensing of fault conditions and the algorithms the microcontroller executes can prevent the fault conditions from causing the IGBTs to fail. Additionally, the optical isolation in the iso-amps prevents the fault conditions from overloading the microcontroller and causing it to fail.
However, the IGBT protection must be cost-effective -- the market continues to demand sufficient IGBT protection from fault conditions at a cost that does not significantly affect the total cost of the motor drive system. To meet this demand, IGBT gate drivers (such as the ACPL-332J [1]) and current sensors with protection features have been introduced to carry out essential fault detection in addition to their driving and sensing functions. These products provide a cost-effective scheme to implement IGBT protection and eliminate the need for separate detection and feedback components. Refer to References [1, 2] for details of those protection features integrated with gate drivers and how to use those features in IGBT protections. The remainder of this article will focus on some of the fault protection functions that can be implemented with current/voltage sensors as listed in Table 1 .



Over-current conditions in an IGBT can occur due to a phase-to-phase short, a ground short or a shoot through. The shunt + iso-amp current sensing devices on the output phases and DC bus provide fault detection in addition to current measurement. Typical IGBT short-circuit survival times are rated up to 10 ms [3, 4]. To ensure effective protection, this limit should not be exceeded. Within this limit, the fault must be detected, fed back to controller and the shutdown procedure completed within this period. To achieve this requirement, iso-amps use different methods.
For instance, the ACPL-C79A has a fast, 1.6 µs response time for a step input. That allows the iso-amp to capture transients during short-circuit and overload conditions (Fig. 3. ) [5]. The signal propagation delay from input to output at mid point is only 2 ms, while it takes just 2.6 ms for the output signal to catch up with input, reaching 90% of the final levels.

Besides fast response time, the ACPL-C79A provides ±1% gain accuracy, excellent nonlinearity of 0.05% and a signal-to-noise ratio (SNR) of 60 dB. Also available are the ACPL-C79B, which offers a higher-precision gain accuracy of ±0.5%, and the ACPL-C790, which has a ±3% gain tolerance. All devices in the ACPL-C79A family are certified to withstand a 1230 VPEAK working insulation voltage, and can reject high common-mode transient noise of up to 15 kV/ms. These features are delivered in a stretched SO-8 package that has a footprint 30% smaller than the standard DIP-8 package.
Another example is the HCPL-788J, which takes a different approach to achieve fast response in over-current detection (Fig. 4 ) [6, 7]. In addition to the signal output pin, it comes with a Fault pin that toggles quickly from High to Low level to indicate an over-current condition. This iso-amp provides ±3% measurement accuracy.

In the fault feedback design, one issue that the design must deal with is nuisance tripping. Nuisance tripping is a false triggering of the fault detection in the absence of any apparent fault condition that will damage the IGBTs. To avoid false triggering, the HCPL-788J employs a pulse discriminator circuit to effectively blank out the influence of the di/dt and dv/dt glitches. The advantage of this method is that the rejection is independent of amplitude, which means the fault threshold can be set to a much lower level without increasing the risk of nuisance tripping.
In the circuit implementation to achieve the fast fault detection, two comparators in the Fault Detection block are used to detect the negative and positive fault thresholds. The switching threshold is equal to the sigma-delta modulator reference of 256 mV. The outputs of these comparators are connected to blanking filters with a blanking period of 2 ms, and then sent to the Encoder block.
To ensure that the fault status is transmitted across the isolation boundary as quickly as possible, two unique digital coding sequences are used to represent the fault condition, one code for the negative level, one for the positive. When a fault is detected, the normal data transfer through the optical channel is interrupted and the bit stream replaced with the fault code. These two fault codes deviate significantly from the normal coding scheme, so on the detector side, the decoder immediately recognizes the codes as a fault conditions [7].
The time required by the decoder to detect and communicate the fault condition across the isolation boundary is around 1 ms. Adding the anti-aliasing filter delay of 400 ns gives propagation delay of 1.4 ms. The delay between the fault event and the output fault signal is the sum of the propagation delay and the blanking period (2 ms), resulting in an overall fault detection time of 3.4 ms (Fig. 5 ).


The Fault output pin allows fault signal from several devices to be connected together, enabling multiple parts to be wire-ORed together to create a single fault signal (upper right portion of Fig. 6. ) [6]. This signal may then be used to directly disable the PWM inputs through the controller.

Overload Detection
An overload condition refers to a situation where the motor current exceeds the rated current of the drive, but not so far as to put the inverter or motor in immediate danger of failure, e.g. if the motor is mechanically overloaded or a motor stalling situation, as a result of a bearing failure.
Inverters are usually specified with an overload rating in additional to the nominal rating. The time period of the allowable overload rating is dependent on the interval of time before the problem of overheating becomes an issue. A typical overload rating is 150% of nominal load for a period up to one minute.
The ACPL-C79A accepts full scale input range of ±300 mV and the data sheet specifications are based on ±200 mV nominal input range. A designer has the flexibility to choose the overload threshold at either of the two figures, or in between. If the measurement accuracy of the overload current is less stringent compared to that of the normal operating current, which is usually the case, setting the threshold near 300 mV is a good choice as this allows full use of the iso-amp’s dynamic input range. However, setting the threshold at 200 mV ensures measurement accuracy of the overload current. Once the voltage levels are decided, the designer needs to choose appropriate sense resistor value according to corresponding current level.
The HCPL-788J includes an additional feature, the ABSVAL output, which can be used to simplify the overload detection circuit. The ABSVAL circuit rectifies the output signal, providing an output signal proportional to the absolute level of the input signal according to:
This output is also wire OR-able. When three sinusoidal motor phases are combined, the rectified output (ABSVAL) is essentially a DC signal representing the RMS motor current. This DC signal and a threshold comparator can indicate motor overload conditions before damage to the motor or drive occurs (lower right portion of Fig. 6 .).

Overvoltage Detection
The DC bus voltage must also be continuously kept under control. Under certain operating conditions, a motor can act as a generator, delivering a high voltage back into the DC bus through the inverterís power device and/or the recovery diodes. This high voltage is added to the DC bus voltage and forms a very high surge applied to the IGBTs. That surge may exceed the maximum IGBT collect-emitter voltage and cause damage.
The miniature iso-amp (ACPL-C79A) is often used as a voltage sensor in DC bus monitoring applications (Fig. 7. ). A designer needs to scale down the DC bus voltage to fit the input range of the iso-amp by choosing R1 and R2 values according to appropriate ratio.

References
  1. ACPL-332J Data Sheet, Avago Technologies, AV02-0120EN.
  2. Hong Lei Chen and Chun Keong Tee, “Using gate drive Optocouplers in IGBT protections,” EETimes Europe, December 2010, pp. 28-31.
  3. Terje Rogne, “Short-Circuit Capability of IGBT (COMFET) Transistors,” IEEE, 1988.
  4. J. Li, R. Herzer, R. Annacker, B. Koenig, “Modern IGBT/FWD Chip Sets For 1200V Applications,” Semikron Elektronik GmbH, 2007.
  5. ACPL-C79B, ACPL-C79A, ACPL-C790 Precision Miniature Isolation Amplifiers Data Sheet. Avago Technologies, AV02-2460EN.
  6. HCPL-788J Data Sheet, Avago Technologies, AV02-1546EN.
  7. Patrick Sullivan, Denis Kobasevic, “Smart Current Sensor For Motor Drive Control.” PCIM Europe, 1998, Vol.10 no.4, pp. 182-186.
Related Articles

PWM


Pulse-Time Modulation

Pulse-Time Modulation 


Fonte: INTEGRATED PUBLISHING.  Pulse-time modulation [online].  Disponível na Internet via URL:  http://www.tpub.com/neets/book12/49k.htm.  Arquivo capturado em 07.05.2013.

Pulse-Time Modulation
In pulse-modulated systems, as in an analog system, the intelligence may be impressed on the carrier by varying any of its characteristics. In the preceding paragraphs the method of modulating a pulse train by varying its amplitude was discussed. Time characteristics of pulses may also be modulated with intelligence information. Two time characteristics may be affected: (1) the time duration of the pulses, referred to as PULSE-DURATION MODULATION (pdm) or PULSE-WIDTH MODULATION (pwm); and (2) the time of occurrence of the pulses, referred to as PULSE-POSITION MODULATION (ppm), and a special type of PULSE-TIME MODULATION (ptm) referred to as PULSE-FREQUENCY MODULATION (pfm). Figure 2-43 shows these types of ptm in views (C),(D), and (E). Views (A) and (B) show the modulating signal and timing, respectively.
Figure 2-43A. - Pulse-time modulation (ptm). MODULATION
Figure 2-43B. - Pulse-time modulation (ptm). TIMING
Figure 2-43C. - Pulse-time modulation (ptm). PDM
Figure 2-43D. - Pulse-time modulation (ptm). PPM
Figure 2-43E. - Pulse-time modulation (ptm). PFM
PULSE-DURATION MODULATION. - Pdm and pwm are designations for a single type of modulation. The width of each pulse in a train is made proportional to the instantaneous value of the modulating signal at the instant of the pulse. Either the leading edges, the trailing edges, or both edges of the pulses may be modulated to produce the variation in pulse width. Pdm can be obtained in a number of ways, one of which is illustrated in views (A) through (D) in figure 2-44. A circuit to produce pdm is shown in figure 2-45. Adding the modulating signal [figure 2-44, view (A)] to a repetitive sawtooth [view (B)] will result in the waveform shown in view (C). This waveform is then applied to a circuit which changes state when the input signal exceeds a specific threshold level. This action produces pulses with widths that are determined by the length of time that the input waveform exceeds the threshold level. The resulting waveform is shown in view (D).
Figure 2-44A. - Pulse-duration modulation (pdm). MODULATING SIGNAL
Figure 2-44B. - Pulse-duration modulation (pdm). REPETITIVE SAWTOOTH PULSES
Figure 2-44C. - Pulse-duration modulation (pdm). MODULATING SIGNAL AND SAWTOOTH ADDED
Figure 2-44D. - Pulse-duration modulation (pdm). WIDTH MODULATED PULSES FROM CIRCUIT OF FIGURE 2-45
Figure 2-45. - Circuit for producing pdm.
In the circuit of figure 2-45, a series of sawtooth pulses, occurring at the sampling rate, is applied to a one-shot multivibrator. The multivibrator has the signal voltage Essuperimposed on the bias voltage Ein. Each pulse triggers a cycle of multivibrator operation which terminates after a time interval and varies linearly with the voltage Es. The pulse of plate voltage produced by the multivibrator will have a leading edge at T1. The leading edge will vary in position with the signal voltage, while the trailing edge at T2 is fixed by the termination of the sawtooth pulse. The length of the output pulse is thus duration or width modulated. If the sawtooth has an instantaneous buildup and a sloping trailing edge, then the leading edge (T1) is fixed and the trailing edge (T2) varies. If the sawtooth generator produces a slope on both leading and trailing edges, both T1 and T2 are variable in position, but the result is still pdm. Pdm is often used because it is of a constant amplitude and is, therefore, less susceptible to noise. When compared with ppm, pdm has the disadvantage of a varying pulse, width and, therefore, of varying power content. This means that the transmitter must be powerful enough to handle the maximum-width pulses, although the average power transmitted is much less than peak power.On the other hand, pdm will still work if the synchronization between the transmitter and receiver fails; in ppm it will not, as will be seen in the next section.
PULSE-POSITION MODULATION. - The amplitude and width of the pulse is kept constant in the system. The position of each pulse, in relation to the position of a recurrent reference pulse, is varied by each instantaneous sampled value of the modulating wave. Ppm has the advantage of requiring constant transmitter power since the pulses are of constant amplitude and duration. It is widely used but has the disadvantage of depending on transmitter-receiver synchronization.
Ppm can be generated in several ways, but we will discuss one of the simplest.Figure 2-46 shows three waveforms associated with developing ppm from pdm.The pdm pulse train is applied to a differentiating circuit. (Differentiation was presented in NEETS, Module 9,
Introduction to Wave-Generation and Wave-Shaping Circuits.) This provides positive- and negative-polarity pulses that correspond to the leading and trailing edges of the pdm pulses. Considering pdm and its generation, you can see that each pulse has a leading and trailing edge. In this case the position of the leading edge is fixed, whereas the trailing edge is not, as shown in view (A) of figure 2-46. The resultant pulses after the differentiation are shown in view (B). The negative pulses are position-modulated in accordance with the modulating waveform. Both the negative and positive pulse are then applied to a rectification circuit. This application eliminates the positive, non-modulated pulses and develops a ppm pulse train, as shown in view (C).
Figure 2-46. - Pulse-position modulation (ppm).
PULSE-FREQUENCY MODULATION. - Pfm is a method of pulse modulation in which the modulating wave is used to frequency modulate a pulse-generating circuit. For example, the pulse rate may be 8,000 pulses per second (pps) when the signal voltage is 0. The pulse rate may step up to 9,000 pps for maximum positive signal voltage, and down to 7,000 pps for maximum negative signal voltage. Figure 2-47, views (A), (B), and (C) show three typical waveforms for pfm. This method of modulation is not used extensively because of complicated pfm generation methods. It requires a stable oscillator that is frequency modulated to drive a pulse generator. Since the other forms of ptm are easier to achieve, they are commonly used.
Figure 2-47A. - Pulse-frequency modulation (pfm). MODULATION
Figure 2-47B. - Pulse-frequency modulation (pfm). TIMING
Figure 2-47C. - Pulse-frequency modulation (pfm). PFM
Q.23 What characteristics of a pulse can be changed in pulse-time modulation?
Q.24 Which edges of the pulse can be modulated in pulse-duration modulation?
Q.25 What is the main disadvantage of pulse-position modulation?
Q.26 What is pulse-frequency modulation?