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OPA690 Datasheet(PDF) 18 Page - Texas Instruments |
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OPA690 Datasheet(HTML) 18 Page - Texas Instruments |
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18 / 27 page ![]() OPA2613 SBOS249D − JUNE 2003− REVISED APRIL 2004 www.ti.com 18 SINGLE-SUPPLY ADSL UPSTREAM DRIVER Figure 6 shows an example of a single-supply ADSL upstream driver. The dual OPA2613 is configured as a differential gain stage to provide signal drive to the primary of the transformer (here, a step-up transformer with a turns ratio of 1:2). The main advantage of this configuration is the cancellation of all even harmonic distortion products. Another important advantage for ADSL is that each amplifier needs only to swing half of the total output required driving the load. R G 308 Ω 1k Ω 1k Ω 1 µF 0.1 µF 0.1 µF RM 12.5 Ω 100 Ω ZLINE AFE 2V PP Max Assumed R F 1k Ω 20 Ω 20 Ω R F 1k Ω 1/2 OPA2613 1/2 OPA2613 +12V 1:n 15VPP I P =150mA IP =150mA RM 12.5 Ω +6.3V Figure 6. Single-Supply ADSL Upstream Driver The analog front-end (AFE) signal is AC-coupled to the driver, and the noninverting input of each amplifier is biased slightly above the mid-supply voltage (+6.3V in this case). In addition to providing the proper biasing to the amplifier, this approach also provides a high-pass filtering with a corner frequency, set here at 1.6kHz. As the upstream signal bandwidth starts at 26kHz, this high-pass filter does not generate any problems and has the advantage of filtering out unwanted lower frequencies. The input signal is amplified with a gain set by the following equation: G D + 1 ) 2 R F R G With RF = 1kΩ and RG = 308Ω, the gain for this differential amplifier is 7.5. This gain boosts the AFE signal, assumed to be a maximum of 2VPP, to a maximum of 15VPP. The two back-termination resistors (12.5 Ω each) added at each input of the transformer make the impedance of the modem match the impedance of the phone line, and also provide a means of detecting the received signal for the receiver. The value of these resistors (RM) is a function of the line impedance and the transformer turns ratio (n), given by the following equation: R M + Z LINE 2n2 LINE DRIVER HEADROOM MODEL The first step in a transformer-coupled, twisted-pair driver design is to compute the peak-to-peak output voltage from the target specifications. This is done using the following equations: P L + 10 log V RMS 2 (1mW) R L With PL power and VRMS voltage at the load, and RL load impedance, this gives the following: V RMS + (1mW) R L 10 P L 10 V P + Crest Factor V RMS + CF V RMS with VP peak voltage at the load and CF Crest Factor. V LPP + 2 CF V RMS with VLPP: peak-to-peak voltage at the load. Consolidating Equations 4 through 7 allows expressing the required peak-to-peak voltage at the load as a function of the crest factor, the load impedance, and the power at the load. Thus, V LPP + 2 CF (1mW) R L 10 P L 10 This VLPP is usually computed for a nominal line impedance and may be taken as a fixed design target. The next step for the driver is to compute the individual amplifier output voltage and currents as a function of VPP on the line and transformer turns ratio. As the turns ratio changes, the minimum allowed supply voltage changes along with it. The peak current in the amplifier output is given by: "I P + 1 2 2 V LPP n 1 4R M With VLPP as defined in Equation 8, and RM as defined in Equation 4 and shown in Figure 7. R M R M V Lpp n V Lpp R L 2V Lpp n V pp = 1:n Figure 7. Driver Peak Output Voltage (3) (4) (5) (6) (7) (8) (9) (10) |
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