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OP2177ARM Datasheet(PDF) 12 Page - Analog Devices |
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OP2177ARM Datasheet(HTML) 12 Page - Analog Devices |
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12 / 20 page ![]() REV. B OP1177/OP2177/OP4177 –12– Figure 6 is a scope photograph of the output of the OP1177 in response to a 400 mV pulse. The load capacitance is 2 nF. The circuit is configured in positive unity gain, the worst-case condition for stability. Placing an R-C network, as shown in Figure 8, parallel to the load capacitance CL will allow the amplifier to drive higher values of CL without causing oscillation or excessive overshoot. There is no ringing and overshoot is reduced from 27% to 5% using the snubber network. Optimum values for RS and CS are tabulated in Table I for several capacitive loads up to 200 nF. Values for other capacitive loads can be determined experimentally. Table I. Optimum Values for Capacitive Loads CL (nF) RS ( )CS 10 20 0.33 µF 50 30 6.8 nF 200 200 0.47 µF 0 0 0 00 0 0000 0 000 0 0 0 0 0 0 GND VSY = 5V RL = 10k CL = 2nF TIME – 10 s/DIV Figure 6. Capacitive Load Drive without Snubber 0 0 0 00 0 0000 0 000 0 0 0 0 0 0 GND VSY = 5V RL = 10k RS = 200 CL = 2nF CS = 0.47 F TIME – 10 s/DIV Figure 7. Capacitive Load Drive with Snubber RS V+ V 1 4 2 3 7 OP1177 CS CL 400mV + VOUT Figure 8. Snubber Network Configuration CAUTION: The snubber technique cannot recover the loss of bandwidth induced by large capacitive loads. Stray Input Capacitance Compensation The effective input capacitance in an op amp circuit, Ct, con- sists of three components. These are: the internal differential capacitance between the input terminals, the internal common mode capacitance of each input to ground, and the external capacitance including parasitic capacitance. In the circuit of Figure 9, the closed-loop gain increases as the signal frequency increases. The transfer function of the circuit is: 1 2 1 11 ++ () R R sC R t indicating a zero at: s RR RR C RR C t t = + = () 21 21 1 2 π 1// 2 Depending on the value of R1 and R2, the cutoff frequency of the closed-loop gain may be well below the crossover frequency. In this case, the phase margin, Φm, can be severely degraded resulting in excessive ringing or even oscillation. A simple way to overcome this problem is to insert a capacitor in the feedback path as shown in Figure 10. The resulting pole can be positioned to adjust the phase margin. Setting Cf = (R1/R2)Ct, achieves a phase margin of 90°. VOUT R2 V+ V 1 4 2 3 OP1177 R1 Ct V1 7 + – Figure 9. Stray Input Capacitance VOUT R2 V+ V 1 4 2 3 OP1177 R1 Ct V1 7 Cf + – Figure 10. Compensation Using Feedback Capacitor |
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