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AD823ARZ-R7 Datasheet(PDF) 13 Page - Analog Devices |
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AD823ARZ-R7 Datasheet(HTML) 13 Page - Analog Devices |
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13 / 20 page ![]() AD823 Rev. B | Page 13 of 20 THEORY OF OPERATION The AD823 is fabricated on the Analog Devices, Inc. proprietary complementary bipolar (CB) process that enables the construction of PNP and NPN transistors with similar fT’s in the 600 MHz to 800 MHz region. In addition, the process also features N-Channel JFETs that are used in the input stage of the AD823. These process features allow the construction of high frequency, low distortion op amps with picoamp input currents. This design uses a differential output input stage to maximize bandwidth and headroom (see Figure 36). The smaller signal swings required on the S1P/S1N outputs reduce the effect of the nonlinear currents due to junction capacitances and improve the distortion performance. With this design, harmonic distortion of better than −91 dB @ 20 kHz into 600 Ω with VOUT = 4 V p-p on a single 5 V supply is achieved. The complementary common emitter design of the output stage provides excellent load drive without the need for emitter followers, thereby improving the output range of the device considerably with respect to conventional op amps. The AD823 can drive 20 mA with the outputs within 0.6 V of the supply rails. The AD823 also offers outstanding precision for a high speed op amp. Input offset voltages of 1 mV maximum and offset drift of 2 μV/°C are achieved through the use of the Analog Devices advanced thin film trimming techniques. A nested integrator topology is used in the AD823 (see Figure 37). The output stage can be modeled as an ideal op amp with a single-pole response and a unity-gain frequency set by transconductance gm2 and Capacitor C2. R1 is the output impedance of the input stage; gm is the input transconductance. C1 and C5 provide Miller compensation for the overall op amp. The unity-gain frequency occurs at gm/C5. Solving the node equations for this circuit yields () [] () ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ + ⎥⎦ ⎤ ⎢⎣ ⎡ × + + = 1 2 1 1 2 1 1 0 2 C g s A C sR A Vi V m OUT where: A0 = gmgm2 R2R1 (open-loop gain of op amp) A2 = gm2 R2 (open-loop gain of output stage). The first pole in the denominator is the dominant pole of the amplifier and occurs at ~18 Hz. This equals the input stage output impedance R1 multiplied by the Miller-multiplied value of C1. The second pole occurs at the unity-gain bandwidth of the output stage, which is 23 MHz. This type of architecture allows more open-loop gain and output drive to be obtained than a standard 2-stage architecture would allow. VCC VINP VINN VEE R42 R37 J1 J6 I1 C6 R33 I2 R43 I3 Q56 S1P Q72 Q61 Q46 I5 VBE +0.3V S1N Q53 Q35 Q48 VCC Q21 Q62 Q60 Q54 R44 R28 Q52 I4 Q59 A = 1 VB C1 Q17 A = 19 VOUT C2 Q18 Q49 Q55 Q43 I6 Q44 A = 1 Q57 A = 19 Q58 V1 Figure 36. Simplified Schematic |
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