ZHCSEP3B February 2016 – February 2016 THS3217
PRODUCTION DATA.
NOTE
Information in the following applications sections is not part of the TI component specification, and TI does not warrant its accuracy or completeness. TI’s customers are responsible for determining suitability of components for their purposes. Customers should validate and test their design implementation to confirm system functionality.
The five example designs presented show a good, but not comprehensive, range of the possible solutions that the THS3217 provides. Numerous more configurations are clearly possible to the creative designer.
For this design example, use the parameters listed in Table 8 as the input parameters.
DESIGN PARAMETER | EXAMPLE VALUE | |||
---|---|---|---|---|
High-frequency, THS3217 channel | 5-VPP, 100-MHz bandwidth | |||
High-voltage, THS3091 channel | 20-VPP, 40-MHz bandwidth |
The THS3217 is well suited for high-speed, low-distortion arbitrary waveform generator (AWG) applications commonly used in laboratory equipment. In this typical application, a high-speed, complementary-current-output DAC is used to drive the D2S. The OPS of the THS3217 easily drives a 100-MHz, 2.5-VPP signal into a matched 50-Ω load. When a larger output signal is required, consider using the THS3091 as the final driver stage.
A passive RLC filter is commonly used on DAC outputs to reduce the high-frequency content in the DAC steps. The filtering between the DAC output and the input to the D2S reduces higher-order DAC harmonics from feeding into the internal OPS path when the external input path is selected. Feedthrough between the internal and external OPS paths increases with increasing frequency; however, the input filter rolls off the DAC harmonics before the harmonics couple to VOUT (pin 10) through the deselected OPS signal path. Figure 96 shows an example of a doubly-terminated differential filter from the DAC to the THS3217 D2S inputs at pins 2 and 3.The DAC is modeled as two, fixed, 10-mA currents and a differential, ac-current source. The 10-mA dc midscale currents set up the average common-mode voltage at the DAC outputs and D2S inputs at 10 mA × 25 Ω = 0.25 VCM. The total voltage swing on the DAC outputs is 0 V to 0.5 V.
Some of the guidelines to consider in this filter design are:
Figure 97 shows the TINA-simulated filter response for the input-stage filter. The low-frequency 34-dBΩ gain is due to the 50-Ω differential resistance at the DAC output terminals. At 400 MHz, this filter is down 16 dB from the 50-Ω level; it is also very flat through 100 MHz.
In the example design of Figure 95, a 100-MHz, third-order Bessel filter is placed between the D2S output and the external OPS input. Another 50-MHz, third-order Bessel filter is placed at the input of a very-high, output-swing THS3091 stage. A double-pole, double-throw (DPDT) relay selects the THS3091 path when the internal OPS path is selected in the THS3217. Figure 95 shows this design. The key operational considerations in this design include:
To design a high-voltage, high-speed pulse generator with minimum overshoot, use the parameters listed in Table 8 as the input parameters.
DESIGN PARAMETER | EXAMPLE VALUE |
---|---|
Power supply | ±7.5 V |
Pulse frequency | 10 MHz |
Pulse output voltage | 10 VPP |
Figure 100 shows an example design using the THS3217 to deliver a 10-VPP maximum voltage from a DAC input, and includes an example external, third-order, interstage Bessel filter. Some of the salient considerations for this design include:
The very-high peak output current and slew rate of the THS3217 OPS make it particularly suitable for driving heavy capacitive loads, such as the piezo elements used in continuous wave (CW) applications that require high-amplitude, sinusoidal-type excitations. The driver is quickly disabled during the receive time when the output TR switch is moved to receive mode. Figure 103 shows an example design using the internal midscale buffer to bias all the stages to midsupply on a single 15-V design. There are many elements to this example that also apply to any single-supply application. The key points here are:
Using a very low series resistor limits the waveform distortion due to the I × R drop at the peak charging point around the sinusoidal zero crossing. The 135 mA through 3.3 Ω causes a 0.45-V peak drop to the load capacitance around zero crossing. The voltage drop across the series output resistor increases the apparent third harmonic distortion at the capacitive load. Figure 45 and Figure 46 show 10-VPP distortion sweeps into various capacitor loads. The results shown in these figures are for the OPS only because the results set the harmonic distortion performance in this example.
An easy way to insert a dc offset into the signal channel (without sacrificing any of the DAC dynamic range) is to apply the desired offset at VMID_IN and use it to bias VREF (pin 14) and VIN+ (pin 9). An example is shown in Figure 104. This example shows a relatively low maximum differential input of 1 VPP on any compliance voltage required by the DAC. Other configuration options include:
Certain applications require the differential DAC output voltage to be level-translated from one common-mode (compliance) level to a differential output at a different common-mode level. The THS3217 performs this function directly using the very flexible blocks provided internally. Figure 105 shows an example of such an application, where the differential gain is always 4 V/V. The differential gain is fine-tuned down by setting the insertion loss in the differential post-filter. The considerations critical to this application include: