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OPA843 Datasheet(PDF) 12 Page - Texas Instruments |
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OPA843 Datasheet(HTML) 12 Page - Texas Instruments |
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12 / 32 page ![]() OPA2846 SBOS274C −JUNE 2003 − REVISED AUGUST 2008 www.ti.com 12 APPLICATIONS INFORMATION WIDEBAND, NONINVERTING OPERATION The OPA2846 provides a unique combination of features—low input voltage noise along with a very low distortion output stage—to give one of the highest dynamic range dual op amps available. Its very high Gain Bandwidth Product (GBP) can be used either to deliver high signal bandwidths at high gains, or to deliver very low distortion signals at moderate frequencies and lower gains. To achieve the full performance of the OPA2846, careful attention to printed circuit board (PCB) layout and component selection is required, as discussed in the remaining sections of this data sheet. Figure 1 shows the noninverting gain of +10 circuit used as the basis of the Electrical Characteristics and most of the Typical Characteristics. Most of the curves were charac- terized using signal sources with 50 Ω driving impedance, and with measurement equipment presenting a 50 Ω load impedance. In Figure 1, the 50 Ω shunt resistor at the VI terminal matches the source impedance of the test generator, while the 50 Ω series resistor at the VO terminal provides a matching resistor for the measurement equip- ment load. Generally, data sheet voltage swing specifica- tions are at the output pin (VO in Figure 1), while output power (dBm) specifications are at the matched 50 Ω load. The total 100 Ω load at the output, combined with the 503Ω total feedback network load, presents the OPA2846 with an effective output load of 83 Ω for the circuit of Figure 1. 1/2 O PA 2 846 +5V −5V −V S +V S 50 Ω V O V I 50 Ω 0.1 µF 6.8 µF 6.8 µF R G 50 Ω R F 453 Ω 50 Ω Source 50 Ω Load 0.1 µF Figure 1. Noninverting, G = +10 Specification and Test Circuit Voltage-feedback op amps, unlike current-feedback designs, can use a wide range of resistor values to set their gains. The circuit of Figure 1, and the specifications at other gains, uses the constraint that RG should always be set to 50 Ω and RF adjusted to get the desired gain. Observing this guideline will ensure that the thermal noise contribution of the feedback network is insignificant compared to the 1.2nV/ √Hz input voltage noise for the op amp itself. WIDEBAND, INVERTING GAIN OPERATION Operating the OPA2846 as an inverting amplifier has several benefits and is particularly appropriate when a matched input impedance is required. Figure 2 shows the inverting gain circuit used as the basis of the inverting mode Typical Characteristics. 1/2 O P A 2846 +5V −5V +V S −V S 91 Ω 50 Ω V O V I 6.8 µF 0.1 µF 6.8 µF 0.1 µF 0.1 µF R F 1k Ω R G 50 Ω 50 Ω Source 50 Ω Load Figure 2. Inverting, G = −20 Characterization Circuit Driving this circuit from a 50 Ω source, and constraining the gain resistor (RG) to equal 50Ω, will give both a signal bandwidth and noise advantage. RG acts as both the input termination resistor and the gain setting resistor for the circuit. Although the signal gain (VO/VI) for the circuit of Figure 2 is double that for Figure 1, the noise gains are in fact equal when the 50 Ω source resistor is included. This has the interesting effect of doubling the equivalent GBP of the amplifier. This can be seen in comparing the G = +10 and G = −20 small-signal frequency response curves. Both show approximately 250MHz bandwidth, but the inverting configuration of Figure 2 gives 6dB higher signal gain. If the signal source is actually the low impedance output of another amplifier, RG should be increased to the minimum load resistance value allowed for that amplifier and RF should be adjusted to achieve the desired gain. For stable operation of the OPA2846, it is critical that this driving amplifier show a very low output impedance at frequencies beyond the expected closed-loop bandwidth for the OPA2846. |
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