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ADUC831BCP Datasheet(PDF) 33 Page - Analog Devices |
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ADUC831BCP Datasheet(HTML) 33 Page - Analog Devices |
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33 / 76 page ![]() REV. 0 ADuC831 –33– Using the DAC The on-chip DAC architecture consists of a resistor string DAC followed by an output buffer amplifier, the functional equivalent of which is illustrated in Figure 21. Details of the actual DAC architecture can be found in U.S. Patent Number 5969657 (www.uspto.gov). Features of this architecture include inherent guaranteed monotonicity and excellent differential linearity. OUTPUT BUFFER HIGH Z DISABLE (FROM MCU) DAC0 R R R R R ADuC831 AVDD VREF Figure 21. Resistor String DAC Functional Equivalent As illustrated in Figure 21, the reference source for each DAC is user selectable in software. It can be either AVDD or VREF. In 0-to-AVDD mode, the DAC output transfer function spans from 0 V to the voltage at the AVDD pin. In 0-to-VREF mode, the DAC output transfer function spans from 0 V to the internal VREF, or if an external reference is applied, the voltage at the VREF pin. The DAC output buffer amplifier features a true rail- to-rail output stage implementation. This means that, unloaded, each output is capable of swinging to within less than 100 mV of both AVDD and ground. Moreover, the DAC’s linearity specifi- cation (when driving a 10 k Ω resistive load to ground) is guaranteed through the full transfer function except codes 0 to 100, and, in 0-to-AVDD mode only, codes 3945 to 4095. Linear- ity degradation near ground and VDD is caused by saturation of the output amplifier, and a general representation of its effects (neglecting offset and gain error) is illustrated in Figure 22. The dotted line in Figure 22 indicates the ideal transfer function, and the solid line represents what the transfer function might look like with endpoint nonlinearities due to saturation of the output amplifier. Note that Figure 22 represents a transfer function in 0-to-VDD mode only. In 0-to-VREF mode (with VREF < VDD) the lower nonlinearity would be similar, but the upper portion of the transfer function would follow the “ideal” line right to the end (VREF in this case, not VDD), showing no signs of endpoint linearity errors. VDD VDD –50mV VDD –100mV 100mV 50mV 0mV 000H FFFH Figure 22. Endpoint Nonlinearities Due to Amplifier Saturation The end point nonlinearities conceptually illustrated in Figure 22 get worse as a function of output loading. Most of the ADuC831’s data sheet specifications assume a 10 k Ω resistive load to ground at the DAC output. As the output is forced to source or sink more current, the nonlinear regions at the top or bottom (respectively) of Figure 22 become larger. With larger current demands, this can significantly limit output voltage swing. Figure 23 and Figure 24 illustrate this behavior. It should be noted that the upper trace in each of these figures is only valid for an output range selection of 0-to-AVDD. In 0-to- VREF mode, DAC loading will not cause highside voltage drops as long as the reference voltage remains below the upper trace in the corresponding figure. For example, if AVDD = 3 V and VREF = 2.5 V, the highside voltage will not be affected by loads less than 5 mA. But somewhere around 7 mA the upper curve in Figure 24 drops below 2.5 V (VREF) indicating that at these higher currents the output will not be capable of reaching VREF. SOURCE/SINK CURRENT – mA 5 05 10 15 4 3 2 1 0 DAC LOADED WITH 0000H DAC LOADED WITH 0FFFH Figure 23. Source and Sink Current Capability with VREF = VDD = 5 V |
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