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AD844AQ Folha de dados(PDF) 7 Page - Analog Devices |
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AD844AQ Folha de dados(HTML) 7 Page - Analog Devices |
7 / 16 page REV. D AD844 –7– Response as an Inverting Amplifier Figure 2 shows the connections for an inverting amplifier. Unlike a conventional amplifier the transient response and the small signal bandwidth are determined primarily by the value of the external feedback resistor, R1, rather than by the ratio of R1/R2 as is customarily the case in an op amp application. This is a direct result of the low impedance at the inverting input. As with conventional op amps, the closed loop gain is –R1/R2. The closed loop transresistance is simply the parallel sum of R1 and Rt. Since R1 will generally be in the range 500 Ω to 2 kΩ and Rt is about 3 M Ω the closed loop transresistance will be only 0.02% to 0.07% lower than R1. This small error will often be less than the resistor tolerance. When R1 is fairly large (above 5 k Ω) but still much less than Rt, the closed loop HF response is dominated by the time constant R1Ct. Under such conditions the AD844 is over-damped and will provide only a fraction of its bandwidth potential. Because of the absence of slew rate limitations under these conditions, the circuit will exhibit a simple single pole response even under large signal conditions. In Figure 2, R3 is used to properly terminate the input if desired. R3 in parallel with R2 gives the terminated resistance. As R1 is lowered, the signal bandwidth increases, but the time constant R1Ct becomes comparable to higher order poles in the closed loop response. Therefore, the closed loop response becomes complex, and the pulse response shows overshoot. When R2 is much larger than the input resistance, RIN, at Pin 2, most of the feedback current in R1 is delivered to this input; but as R2 becomes comparable to RIN, less of the feedback is absorbed at Pin 2, resulting in a more heavily damped response. Conse- quently, for low values of R2 it is possible to lower R1 without causing instability in the closed loop response. Table I lists combinations of R1 and R2 and the resulting frequency response for the circuit of Figure 2. TPC 13 shows the very clean and fast ±10 V pulse response of the AD844. VIN VOUT R3 OPTIONAL R2 R1 AD844 RL CL Figure 2. Inverting Amplifier UNDERSTANDING THE AD844 The AD844 can be used in ways similar to a conventional op amp while providing performance advantages in wideband applications. However, there are important differences in the internal structure which need to be understood in order to optimize the performance of the AD844 op amp. Open Loop Behavior Figure 1 shows a current feedback amplifier reduced to essen- tials. Sources of fixed dc errors such as the inverting node bias current and the offset voltage are excluded from this model and are discussed later. The most important parameter limiting the dc gain is the transresistance, Rt, which is ideally infinite. A finite value of Rt is analogous to the finite open loop voltage gain in a conventional op amp. The current applied to the inverting input node is replicated by the current conveyor so as to flow in resistor Rt. The voltage developed across Rt is buffered by the unity gain voltage follower. Voltage gain is the ratio Rt/ RIN. With typical values of Rt = 3 M Ω and RIN = 50 Ω, the voltage gain is about 60,000. The open loop current gain is another measure of gain and is determined by the beta product of the transistors in the voltage follower stage (see Figure 4); it is typically 40,000. +1 +1 IIN RIN IIN Rt Ct Figure 1. Equivalent Schematic The important parameters defining ac behavior are the trans- capacitance, Ct, and the external feedback resistor (not shown). The time constant formed by these components is analogous to the dominant pole of a conventional op amp, and thus cannot be reduced below a critical value if the closed loop system is to be stable. In practice, Ct is held to as low a value as possible (typically 4.5 pF) so that the feedback resistor can be maximized while maintaining a fast response. The finite RIN also affects the closed loop response in some applications as will be shown. The open loop ac gain is also best understood in terms of the transimpedance rather than as an open loop voltage gain. The open loop pole is formed by Rt in parallel with Ct. Since Ct is typically 4.5 pF, the open loop corner frequency occurs at about 12 kHz. However, this parameter is of little value in determining the closed loop response. |
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