Analog Devices ADuC812 manual Op Amp Model Characteristics, Driving the A/D Converter

Models: ADuC812

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ADuC812

Driving the A/D Converter

The ADC incorporates a successive approximation (SAR) archi- tecture involving a charge-sampled input stage. Figure 7 shows the equivalent circuit of the analog input section. Each ADC conversion is divided into two distinct phases as defined by the position of the switches in Figure 7. During the sampling phase (with SW1 and SW2 in the “track” position) a charge propor- tional to the voltage on the analog input is developed across the input sampling capacitor. During the conversion phase (with both switches in the “hold” position) the capacitor DAC is adjusted via internal SAR logic until the voltage on node A is zero indicating that the sampled charge on the input capacitor is balanced out by the charge being output by the capacitor DAC. The digital value finally contained in the SAR is then latched out as the result of the ADC conversion. Control of the SAR, and timing of acquisition and sampling modes, is handled automatically by built-in ADC control logic. Acquisition and conversion times are also fully configurable under user control.

AIN0

TEMPERATURE

ADuC812

 

SENSOR

 

AIN7

 

 

 

 

200

 

 

 

TRACK

 

 

 

SW1

 

CAPACITOR

 

 

 

 

HOLD

 

DAC

 

2pF

 

 

 

 

 

 

NODE A

 

 

 

SW2

 

 

TRACK

HOLD

COMPARATOR

 

 

 

AGND

 

 

 

Figure 7. Internal ADC Structure

Note that whenever a new input channel is selected, a residual charge from the 2 pF sampling capacitor places a transient on the newly selected input. The signal source must be capable of recovering from this transient before the sampling switches click into “hold” mode. Delays can be inserted in software (between channel selection and conversion request) to account for input stage settling, but a hardware solution will alleviate this burden from the software design task and will ultimately result in a cleaner system implementation. One hardware solution would be to choose a very fast settling op amp to drive each analog input. Such an op amp would need to fully settle from a small signal transient in less than 300 ns in order to guarantee adequate settling under all software configurations. A better solution, recom- mended for use with any amplifier, is shown in Figure 8.

Though at first glance the circuit in Figure 8 may look like a simple antialiasing filter, it actually serves no such purpose since its corner frequency is well above the Nyquist frequency, even at a 200 kHz sample rate. Though the R/C does helps to reject some incoming high-frequency noise, its primary function is to ensure that the transient demands of the ADC input stage are met. It

ADuC812

51

1 AIN0

0.01 F

Figure 8. Buffering Analog Inputs

does so by providing a capacitive bank from which the 2 pF sam- pling capacitor can draw its charge. Since the 0.01 ∝F capacitor in Figure 8 is more than 4096 times the size of the 2 pF sam- pling capacitor, its voltage will not change by more than one count (1/4096) of the 12-bit transfer function when the 2 pF charge from a previous channel is dumped onto it. A larger capacitor can be used if desired, but not a larger resistor (for reasons described below).

The Schottky diodes in Figure 8 may be necessary to limit the voltage applied to the analog input pin as per the data sheet absolute maximum ratings. They are not necessary if the op amp is powered from the same supply as the ADuC812 since in that case the op amp is unable to generate voltages above VDD or below ground. An op amp of some kind is necessary unless the signal source is very low impedance to begin with. DC leakage currents at the ADuC812’s analog inputs can cause measurable dc errors with external source impedances as little as 100 Ω or so. To ensure accurate ADC operation, keep the total source impedance at each analog input less than 61 Ω. The table below illustrates examples of how source impedance can affect dc accuracy.

Source

Error from 1 ∝A

Error from 10 ∝A

Impedance

Leakage Current

Leakage Current

61 Ω

61 ∝V = 0.1 LSB

610 ∝V = 1 LSB

610 Ω

610 ∝V = 1 LSB

6.1 mV = 10 LSB

Although Figure 8 shows the op amp operating at a gain of 1, you can of course configure it for any gain needed. Also, you can just as easily use an instrumentation amplifier in its place to condition differential signals. Use any modern amplifier that is capable of delivering the signal (0 to VREF) with minimal satura- tion. Some single-supply rail-to-rail op amps that are useful for this purpose include, but are certainly not limited to, the ones given in Table VI. Check Analog Devices literature (CD ROM data book, etc.) for details on these and other op amps and instrumentation amps.

Table VI. Some Single-Supply Op Amps

Op Amp Model

Characteristics

 

 

OP181/OP281/OP481

Micropower

OP191/OP291/OP491

I/O Good up to VDD, Low Cost

OP196/OP296/OP496

I/O to VDD, Micropower, Low Cost

OP183/OP283

High Gain-Bandwidth Product

OP162/OP262/OP462

High GBP, Micro Package

AD820/AD822/AD824

FET Input, Low Cost

AD823

FET Input, High GBP

 

 

Keep in mind that the ADC’s transfer function is 0 to VREF, and any signal range lost to amplifier saturation near ground will impact dynamic range. Though the op amps in Table VI are capable of delivering output signals very closely approaching

REV. B

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Analog Devices ADuC812 manual Op Amp Model Characteristics, Driving the A/D Converter, Table VI. Some Single-Supply Op Amps