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OPA607 Datasheet(PDF) 14 Page - Texas Instruments |
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OPA607 Datasheet(HTML) 14 Page - Texas Instruments |
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14 / 21 page ![]() Time (50 msec/Div) D004 Current waveform 14 OPA607 SBOS981 – OCTOBER 2019 www.ti.com Product Folder Links: OPA607 Submit Documentation Feedback Copyright © 2019, Texas Instruments Incorporated Figure 8. Low-Side Current-Sensing Waveform in a BLDC Motor Control An ADC capturing the data at 500 kSPS puts out a sampled data one time every 2 µs. Because the minimum current pulse duration while running at a 5% duty cycle is 2.5 µs, a 500-kSPS sampling rate ADC is sufficient for this BLDC current-sensing application. The ADS7042 is a low-power, 12-bit, 1-MSPS, SAR ADC. The ADS7042 is operated at 500 kSPS via SCLK at a frequency of 12.5 MHz, which is a standard clock frequency available for SPI communications. For an ADC running at a sampling rate of 500 kSPS on a clock of 12.5 MHz, the bandwidth of the op amp required to drive such an ADC is approximately 2.7 MHz. See the TI precision lab videos on driving SAR ADCs to understand the underlying calculation. The OPA607 has a GBW of 50 MHz. With a gain of 20 V/V, the effective bandwidth available with the OPA607 comes out to approximately 2.5 MHz, making the device the most suitable, cost-optimized amplifier for this application. The RC (240 Ω and 688 pF in Figure 7) charge bucket designed at the input of the SAR ADC is also derived from the calculations provided in the SAR ADC precision lab videos. The fundamental concept behind the design of this charge bucket is to ensure that the acquisition capacitor is charged up to the required final voltage within the acquisition window of the ADC. The ADS7042 samples at 500 kSPS with a 12.5-MHz clock, which translates to a conversion time of 1 µs out of the total time period of 2 µs (1 / 500 kHz). These calculations for different sampling rates and clock frequencies can be found in the ADS7042 data sheet. With the conversion time of 1 µs out of the 2 µs, the OPA607 is left with 1 µs to settle to the required accuracy of 0.1%. Because the full-scale voltage is assumed to be 3 V, an accuracy of 0.1% translates to a maximum allowable error voltage of 3 mV. Thus, the OPA607 must settle to ±3 mV of its final intended value within 1 µs. Figure 9 shows the TINA™ simulation plots for the OPA607 driving the ADS7042. Input voltage (red) is the signal swing across the shunt resistance and the error signal (blue) is representative of the % error in the output of the op amp. As shown at the initial region of the graph in Figure 9, at the time instant (to), the input signal sharply transits from its lowermost point to the uppermost point. This transition can be considered as a short- circuit event or step increase in current resulting from a sudden metal-oxide-semiconductor field-effect transistor (MOSFET) switching. The output (black) waveform tries to follow the high slew rate input signal but is limited by the effective bandwidth of the op amp used. Thus, a higher bandwidth op amp results in the output being able to more closely track the input. The difference between the output and input is represented by the error waveform and the goal of the design is to reduce this error to less than 0.1% within the acquisition window of the ADC. The acquisition window of the ADC is shown in the yellow highlighted regions of Figure 9. Thus the % error signal (blue) must settle down to less than 0.1% before the end of this 1-µs window (within the yellow marked region). As illustrated in Figure 9, the error signal comfortably settles to the final value with an error % of –0.025%, which is well within the required 0.1% accuracy. Thus, the OPA607 settles to 0.1% accuracy within 1 µs with a worst- case, 0-V to 3-V full-scale transient output that is also in a gain configuration of 20 V/V. The OPA607 enables single-sample settling for the ADS7042 running on a 12.5-MHz clock with 500 kSPS, thus making the device a very cost-optimized, single amplifier solution. Figure 10 gives the DC transfer characteristics of the circuit in Figure 7. As per the parameters from Table 2 the current across RSH is varied in both directions and the voltage at the output of the OPA607 is measured. Equation 7 describes the relation between the output of the OPA607 and the ISH current: VO = (20 × ISH × 7 mΩ) + 1.24 V (7) |
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