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CLC449AMC 数据表(PDF) 5 Page - National Semiconductor (TI) |
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CLC449AMC 数据表(HTML) 5 Page - National Semiconductor (TI) |
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5 / 12 page ![]() 5 http://www.national.com Figure 2: Inverting Gain The normalized gain plots in the Typical Performance Characteristics section show different feedback resistors, Rf, for different gains. These values of Rf are recommended for obtaining the highest bandwidth with minimal peaking. The resistor Rt in Figure 2 provides DC bias for the non- inverting input. For |Av| ≤ 4, calculate the recommended R f as follows: Rf ≅ 295 - |A v| • Ri, where Ri = 45Ω. For |Av| > 4, the minimum recommended feedback resistor is Rf = 100 Ω. Select Rg to set the DC gain: At large gains, Rg becomes small and will load the previous stage. This situation is resolved by driving Rg with a low impedance buffer like the CLC111, or increasing Rf and Rg (see the Bandwidth (Small Signal) sub-section for the tradeoffs). Accurate DC gain is usually limited by the tolerance of the external resistors Rf and Rg. Bandwidth (Small Signal) The CLC449 current-feedback amplifier bandwidth is a function of the feedback resistor (Rf), not of the DC volt- age gain (Av). The bandwidth is approximately proportional to 1/Rf. As a rule, if Rf doubles, the band- width is cut in half. Other AC specifications will also be degraded. Decreasing Rf from the recommended value increases peaking and for very small values of Rf oscillation will occur. With an inverting amplifier design, peaking is sometimes observed. This is often the result of layout parasitics caused by inadequate ground planes or long traces. If this is observed, placing a 50 to 200 Ω resistor between the non-inverting pin and ground will usually reduce the peaking. Bandwidth (Minimum Slew Rate) Slew rate influences the bandwidth for large signal sinusoids. To determine an approximate value of slew rate, necessary to support large sinusoids use the following equation: SR ≅ 5 • f • V peak Vpeak is the peak output sinusoidal voltage, f is the frequency of the sinusoid. The slew rate of the CLC449 in inverting gains is always higher than in non-inverting gains. DC Design (Level Shifting) Figure 3 shows a DC level shifting circuit for inverting gain configurations. Vref produces a DC output level shift of which is independent of the DC output produced by Vin. Figure 3: Level Shifting Circuit DC Design (Single Supply) Figure 4 is a typical single-supply circuit. Resistors R1 and R2 form a voltage divider that sets the non-inverting input DC voltage. This circuit has a DC gain of 1. The coupling capacitor C1 isolates the DC bias point from the previous stage. Both capacitors make a high pass response; the high frequency gain is determined by Rf and Rg. Figure 4: Single Supply Circuit The complete gain equation for the circuit in Figure 4 is: where s = j ω, τ 1 = (R1|| R2) • C1, and τ2 = RgC2. DC Design (DC Offsets) The DC offset model shown in Figure 5 is used to calculate the output offset voltage. The equation for out- put offset voltage is: The current offset terms, IBN and IBI, do not track each other. The specifications are stated in terms of magnitude only. Therefore, the terms Vos, IBN, and IBI may have either positive or negative polarity. Matching the equivalent resistance seen at both input pins does not reduce the output offset voltage. + - CLC449 Rf 0.1 µF 6.8 µF Vo Vin Vcc 0.1 µF 6.8 µF Vee Rg Rt 3 2 4 7 6 + + R R |A | g f v = -V R R ref f ref ⋅ Vin Req2 + - CLC449 Rf Vo Vref Rref Req1 + - CLC449 Rf Vo Vin Vcc Rg R2 R1 Vcc C1 C2 VV I R 1 R R IR oos BN eq1 f eq2 BI f =− + ⋅ ()⋅+ +⋅ () V V s 1s 1s 1 R R 1s o in 1 1 2 f g 2 = + ⋅ +⋅ + + τ τ τ τ |
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