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OPA690 Datasheet(PDF) 17 Page - Texas Instruments |
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OPA690 Datasheet(HTML) 17 Page - Texas Instruments |
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17 / 35 page ![]() OPA2613 SBOS249H − JUNE 2003 − REVISED AUGUST 2008 www.ti.com 17 1/2 OPA2613 +5V +V S VS /2 806 Ω 100 Ω VO V I 57.6 Ω 806 Ω RF 402 Ω RG 402 Ω 0.1 µF 0.1 µF 6.8 µF + 0.1 µF Figure 3. AC-Coupled, G = +2, Single-Supply, Specification and Test Circuit The last configuration used as the basis of the +5V Electrical and Typical Characteristics is shown in Figure 4. Design considerations for this inverting, bipolar supply configuration are covered either in single-supply configuration (as shown in Figure 3) or in the Inverting Amplifier Operation section. 1/2 OPA2613 +5V V S /2 806 Ω V I 100 Ω V O 806 Ω R F 402 Ω R M 57.6 Ω 6.8 µF + 0.1 µF 0.1 µF 0.1 µF R G 402 Ω Figure 4. AC-Coupled, G = −1, Single-Supply, Specification and Test Circuit DIFFERENTIAL INTERFACE APPLICATIONS Dual op amps are particularly suitable to differential input to differential output applications. Typically, these fall into either Analog-to-Digital Converter (ADC) input interface or line driver applications. Two basic approaches to differential I/O are noninverting or inverting configurations. Since the output is differential, the signal polarity is somewhat meaningless—the noninverting and inverting terminology applies here to where the input is brought into the OPA2613. Each has its advantages and disadvan- tages. Figure 5 shows a basic starting point for noninverting input differential I/O applications. R F 402 Ω R F 402 Ω 1/2 OP A2613 +V CC Power−Supply decoupling not shown. −V CC R G 268 Ω V O 1/2 OP A2613 V I Figure 5. Noninverting Differential I/O Amplifier This approach provides for a source termination impedance that is independent of the signal gain. For instance, simple differential filters may be included in the signal path right up to the noninverting inputs without interacting with the gain setting. The differential signal gain for the circuit of Figure 5 is: A D + 1 ) 2 R F R G Since the OPA2613 is a voltage-feedback (VFB) amplifier, its bandwidth is principally controlled by the noise gain. The equivalent noise gain for Figure 5 is: 1 ) 2 402 W 268 W + 4V V Various combinations of single-supply or AC-coupled gain can also be delivered using the basic circuit of Figure 5. Common-mode bias voltages on the two noninverting inputs pass on to the output with a gain of 1 since an equal DC voltage at each inverting node creates no current through RG. This circuit does show a common-mode gain of 1 from input to output. The source connection should either remove this common-mode signal if undesired (using an input transformer can provide this function), or the common-mode voltage at the inputs can be used to set the output common-mode bias. If the low common-mode rejection of this circuit is a problem, the output interface may also be used to reject that common-mode. For instance, most modern differential input ADCs reject common-mode signals very well, while a line driver application through a transformer will also remove the common-mode signal through to the line. (1) (2) |
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