SBOS780C March 2016 – June 2021 THS3215
PRODUCTION DATA
The OPS can drive heavy capacitive loads very well, as shown in Figure 6-43 to Figure 6-48. All high-speed amplifiers benefit from the addition of an external series resistor to isolate the load capacitor from the feedback loop. Not using a series isolation resistor often leads to response peaking and possibly oscillation. If frequency response flatness under capacitive load is the design goal, use slightly higher RF values at the lower gains. Target a slightly-higher feedback transimpedance to increase the nominal phase margin before the capacitive load acts to decrease it. Using a higher RF value increases the frequency response flatness across a range of capacitive loads using lower external series resistor values. Although the suggested RF and RG values of Table 8-1 apply when driving a 100 Ω load, if the intended load is capacitive (for example, a passive filter with a shunt capacitor as the first element, another amplifier, or a Piezo element), use the values reported in Table 8-6 as a starting point. The values in Table 8-6 were used to generate Figure 6-43 and Figure 6-44. The results come from a nominal total feedback transimpedance target of 405 Ω (versus 351 Ω used for Table 8-3), and includes the internal 18.5 kΩ resistor in the design. Table 8-6 finds the least error to target gain in the selection of standard resistor values, and limits the minimum RG to 20 Ω. The gains calculated here put 18.5 kΩ in parallel with the reported external standard value RF.
TARGET GAIN (V/V) |
BEST RF (Ω) |
BEST RG (Ω) | CALCULATED GAIN | GAIN ERROR (%) |
|
---|---|---|---|---|---|
(V/V) | (dB) | ||||
1.5 | 487 | 953 | 1.494 | 3.488 | –0..389 |
2 | 432 | 422 | 1.995 | 6 | –0.233 |
2.5 | 402 | 261 | 2.501 | 7.963 | 0.048 |
3 | 332 | 162 | 3.006 | 9.559 | 0.191 |
3.5 | 274 | 107 | 3.515 | 10.917 | 0.416 |
4 | 221 | 73.2 | 3.974 | 11.984 | –0.662 |
4.5 | 165 | 46.4 | 4.513 | 13.090 | 0.295 |
5 | 158 | 39.2 | 4.984 | 13.952 | –0.320 |
5.5 | 165 | 36.5 | 5.467 | 14.755 | –0.602 |
6 | 169 | 33.2 | 6.029 | 15.605 | 0.486 |
6.5 | 169 | 30.1 | 6.547 | 16.321 | 0.729 |
7 | 174 | 28.7 | 6.989 | 16.888 | –0.161 |
7.5 | 174 | 26.7 | 7.437 | 17.429 | –0.833 |
8 | 178 | 24.9 | 8.060 | 18.127 | 0.753 |
8.5 | 178 | 23.2 | 8.578 | 18.668 | 0.915 |
9 | 178 | 22.1 | 8.955 | 19.041 | –0.499 |
9.5 | 182 | 21 | 9.558 | 19.608 | 0.613 |
10 | 187 | 20.5 | 10.006 | 20.005 | 0.056 |
As the capacitive load or amplifier gain increases, the series resistor values can be reduced to hold a flat response (see Figure 6-43). See Figure 6-44 for the measured SSBW shapes for various capacitive loads configured with the suggested series resistor from the output of the OPS and the RF and RG values suggested in Table 8-6 for a gain of 2.5 V/V. This measurement includes a 200 Ω shunt resistor in parallel with the capacitive load as a measurement path.
Figure 6-45 and Figure 6-46 demonstrate the OPS harmonic distortion performance when driving a range of capacitive loads. These figures show suitable performance for large-signal, piezo-driver applications. If voltage swings higher than 12 VPP are required, consider driving the OPS output into a step-up transformer. The high peak-output current for the OPS supports very fast charging edge rates into heavy capacitive loads, as shown in the step response plots (see Figure 6-47 and Figure 6-48). This peak current occurs near the center of the transition time driving a capacitive load. Therefore, the I × R drop to the capacitive load through the series resistor is at a maximum at midtransition, and 0 V at the extremes (low dV/dT points). For even better performance driving heavy capacitive loads, consider using the THS3217, a DAC output amplifier with higher output current and slew rate.