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OPA820SKGD3 Scheda tecnica(PDF) 17 Page - Texas Instruments |
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OPA820SKGD3 Scheda tecnica(HTML) 17 Page - Texas Instruments |
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17 / 32 page ![]() OPA820 +5V −5V 50Ω V V O I 0.1µF 2.2µF 0.1µF 2.2µF R M 57.6Ω R T 205Ω R F 402Ω 50Ω Source 50Ω Load 0.01µF R G 402Ω OPA820-HT www.ti.com SBOS587 – DECEMBER 2011 Wideband Inverting Operation Operating the OPA820 as an inverting amplifier has several benefits and is particularly useful when a matched 50- Ω source and input impedance is required. Figure 3 shows the inverting gain of −1 circuit used as the basis of the inverting mode typical characteristics. Figure 3. Inverting G = −1 Specifications and Test Circuit In the inverting case, just the feedback resistor appears as part of the total output load in parallel with the actual load. For the 100- Ω load used in the typical characteristics, this gives a total load of 80 Ω in this inverting configuration. The gain resistor is set to get the desired gain (in this case 402 Ω for a gain of −1) while an additional input matching resistor (RM) can be used to set the total input impedance equal to the source if desired. In this case, RM = 57.6 Ω in parallel with the 402-Ω gain setting resistor gives a matched input impedance of 50 Ω. This matching is only needed when the input needs to be matched to a source impedance, as in the characterization testing done using the circuit of Figure 3. The OPA820 offers extremely good DC accuracy as well as low noise and distortion. To take full advantage of that DC precision, the total DC impedance looking out of each of the input nodes must be matched to get bias current cancellation. For the circuit of Figure 32, this requires the 205- Ω resistor shown to ground on the noninverting input. The calculation for this resistor includes a DC-coupled 50- Ω source impedance along with RG and RM. Although this resistor will provide cancellation for the bias current, it must be well decoupled (0.01 μF in Figure 3) to filter the noise contribution of the resistor and the input current noise. As the required RG resistor approaches 50 Ω at higher gains, the bandwidth for the circuit in Figure 3 will far exceed the bandwidth at that same gain magnitude for the noninverting circuit of Figure 2. This occurs due to the lower noise gain for the circuit of Figure 3 when the 50- Ω source impedance is included in the analysis. For instance, at a signal gain of −10 (RG = 50 Ω, RM = open, RF = 499 Ω) the noise gain for the circuit of Figure 3 will be 1 + 499 Ω/(50 Ω + 50 Ω) = 6 as a result of adding the 50-Ω source in the noise gain equation. This gives considerable higher bandwidth than the noninverting gain of +10. Using the 240-MHz gain bandwidth product for the OPA820, an inverting gain of −10 from a 50-Ω source to a 50-Ω RG gives 55-MHz bandwidth, whereas the noninverting gain of +10 gives 30 MHz. Wideband Single-Supply Operation Figure 4 shows the AC-coupled, single 5-V supply, gain of +2 V/V circuit configuration used as a basis for the 5 V only Electrical and Typical Characteristics. The key requirement for single-supply operation is to maintain input and output signal swings within the useable voltage ranges at both the input and the output. The circuit of Figure 4 establishes an input midpoint bias using a simple resistive divider from the 5-V supply (two 806- Ω resistors) to the noninverting input. The input signal is then AC-coupled into this midpoint voltage bias. The input voltage can swing to within 0.9 V of the negative supply and 0.5 V of the positive supply, giving a 3.6VPP input Copyright © 2011, Texas Instruments Incorporated Submit Documentation Feedback 17 Product Folder Link(s): OPA820-HT |
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