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DAC161S997RGHT Datasheet(PDF) 14 Page - Texas Instruments |
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DAC161S997RGHT Datasheet(HTML) 14 Page - Texas Instruments |
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14 / 27 page ![]() LOOP+ LOOP- R1 R2 + - A(s)Gm IDAC IAUX ILOOP ve ILOOP A(s)Gmve ro LOOP+ LOOP- DAC161S997 BASE OUT COMA RX1 CX1 CX2 CX3 CX4 A(s) gm + - IAUX R1 R2 RE Gm IDAC ro DAC161S997 SNAS621 – JUNE 2013 www.ti.com Loop Compliance The maximum V(LOOP+,LOOP-) potential is limited by the choice of step-down regulator, and the external BJT’s Collector Emitter breakdown voltage. For minimum V(LOOP+, LOOP −) potential consider TROUBLEFigure 10. Here, observe that V(LOOP+,LOOP −) ≅ min(VCE) + ILOOPRE + ILOOPR2 = min(VCE) + 0.53V + 0.96V = 3.66V, at ILOOP = 24mA. The voltage drop across internal R2 is specified in ELECTRICAL CHARACTERISTICS. AC Characteristics The approximate frequency dependent characteristics of the loop drive circuit can be analyzed using the circuit in Figure 12: Figure 12. Capacitances Affecting Control Loop Here it is assumed that the internal amplifier dominates the frequency response of the system, and it has a single pole response. The BJT’s response, in the bandwidth of the control loop, is assumed to be frequency independent and is characterized by the transconductance gm and the output resistance ro. As in previous sections IDAC and IAUX represent the filtered output of the ∑Δ modulator and the quiescent current of the companion devices. The circuit in Figure 12 can be further simplified by omitting the on-board capacitances, whose effect will be discussed in Stability, and by combining the amplifier, the external transistor and resistor RE into one Gm block. The resulting circuit is shown in Figure 13. By assuming that the BJT’s output resistance (ro) is large, the loop current ILOOP can be expressed as: (3) Figure 13. AC Analysis Model of a Transmitter 14 Copyright © 2013, Texas Instruments Incorporated Product Folder Links: DAC161S997 |
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