Suitable for high precision data acquisition system of the AD converter to understand

     Market demand for industrial applications is increasing day by day, data acquisition system is one of the key equipment. They are usually used to detect temperature, flow, liquid level, pressure and other physical quantities, and then convert the analog signals corresponding to these physical quantities into high-resolution digital information, which can be further processed by software. Such systems are increasingly demanding for accuracy and speed. These data acquisition systems consist of amplifier circuits and analog-to-digital converters (ADC), whose performance has a decisive impact on the system.

     However, the overall accuracy is also affected by the ADC's input driver, which is used to buffer and amplify the input signal. In addition, a bias signal must be added or a fully differential signal must be generated to cover the ADC's input voltage range and meet its common-mode voltage requirements, without altering the original signal in the process. Programmable gain instrumentation amplifiers (PGIA) are commonly used as input drivers. In this paper, we propose a combination of input driver and ADC, through which very precise conversion results can be achieved to build a high quality data acquisition system.

     For example, the LTC6373 is a PGIA for high precision data acquisition systems. In addition to a fully differential output, it has high DC accuracy, low noise, low distortion (see Figure 2), and a high bandwidth of 4 MHz with gains of 1/4 to 16. The ADC can be driven directly through it and is therefore suitable for many signal conditioning applications.

The following circuit shows an example of using LTC6373 to drive a precision AD4001 / AD4020 with a 20 bit resolution of 1.8 MSPS

                                                       Figure 1：Example of a circuit that drives a precision ADC

In this circuit, the LTC6373 is DC coupled at the input and output, thus eliminating the need for a transformer to drive the ADC. The gain can be set between 0.25V /V and 16V /V via pins A2/A1/A0. In Figure 1, the LTC6373 uses a differential input-differential output configuration and a ±15 V symmetrical supply voltage. Alternatively, the input can be a single-ended input while the output remains a differential output.

In Figure 1, the output common-mode voltage is set to VREF/2 via the VOCM pin. This enables the output level conversion of LTC6373. Each output of the LTC6373 varies between 0 V and VREF, so there is a differential signal at the ADC input of 2 x VREF amplitude. The RC network between the output of the LTC6373 and the input of the ADC forms a single-pole low-pass filter that reduces the current burr generated when switching capacitors at the ADC input. At the same time, the low pass filter limits the broadband noise.

                      Figure 2：SNR (left) and THD (right) performance of AD4020 driven by LTC6373

Figure 2 shows LTC6373 signal-to-noise ratio (SNR) and total harmonic distortion (THD), in the entire input voltage range (10 v p - p) drive AD4020 SAR ADC (high impedance state model). Satisfactory results can be obtained at a throughput of 1.8 MSPS and a filter resistance of 442 Ω. At 1 MSPS or 0.6 MSPS, the manufacturer recommends an RFILTER of 887 Ω.

The LTC6373 drives most SAR ADCs with differential inputs without the need for an additional ADC driver. However, in some applications, a separate ADC driver can be used between the LTC6373 and the precision ADC to further improve the linearity of the signal chain.