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LT1886CS8 Datasheet(PDF) 11 Page - Linear Technology |
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LT1886CS8 Datasheet(HTML) 11 Page - Linear Technology |
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11 / 16 page ![]() 11 LT1886 APPLICATIO S I FOR ATIO Figures 3 and 4 can be combined as shown in Figure 5. The gain is unity at low frequencies, 1 + RF/RG at mid-band and for stability, a gain of 10 or greater at high frequencies. termination resistor is used, a capacitor to ground at the load can eliminate ringing. Line Driving Back-Termination The standard method of cable or line back-termination is shown in Figure 6. The cable/line is terminated in its characteristic impedance (50 Ω, 75Ω, 100Ω, 135Ω, etc.). A back-termination resistor also equal to to the chararacteristic impedance should be used for maximum pulse fidelity of outgoing signals, and to terminate the line for incoming signals in a full-duplex application. There are three main drawbacks to this approach. First, the power dissipated in the load and back-termination resistors is equal so half of the power delivered by the amplifier is wasted in the termination resistor. Second, the signal is halved so the gain of the amplifer must be doubled to have the same overall gain to the load. The increase in gain increases noise and decreases bandwidth (which can also increase distortion). Third, the output swing of the ampli- fier is doubled which can limit the power it can deliver to the load for a given power supply voltage. RC Vo Vi CC (OPTIONAL) 1886 F03 RF RG = 1 + RF RG Vo Vi < 15MHz 1 2 πRCCC (RC || RG) ≤ RF/9 Output Loading The LT1886 output stage is very wide bandwidth and able to source and sink large currents. Reactive loading, even isolated with a back-termination resistor, can cause ring- ing at frequencies of hundreds of MHz. For this reason, any design should be evaluated over a wide range of output conditions. To reduce the effects of reactive loading, an optional snubber network consisting of a series RC across the load can provide a resistive load at high frequency. Another option is to filter the drive to the load. If a back- Figure 3. Compensation for Noninverting Gains 1886 F04 RF RG Vi VO CC < 15MHz 1 2 πRGCC RG ≤ RF/9 = 1 (LOW FREQUENCIES) (HIGH FREQUENCIES) Vo Vi = 1 + RF RG Figure 4. Alternate Noninverting Compensation RC Vo Vi CC 1886 F05 RF RG CBIG RF RG = 1 AT LOW FREQUENCIES = 1 + AT MEDIUM FREQUENCIES RF (RC || RG) = 1 + AT HIGH FREQUENCIES Vo Vi Figure 5. Combination Compensation 1886 F06 RF RBT CABLE OR LINE WITH CHARACTERISTIC IMPEDANCE RL RG VO Vi RL (1 + RF/RG) = Vo Vi 1 2 RBT = RL An alternate method of back-termination is shown in Figure 7. Positive feedback increases the effective back- termination resistance so RBT can be reduced by a factor of n. To analyze this circuit, first ground the input. As RBT = RL/n, and assuming RP2>>RL we require that: Va = Vo (1 – 1/n) to increase the effective value of RBT by n. Vp = Vo (1 – 1/n)/(1 + RF/RG) Vo = Vp (1 + RP2/RP1) Eliminating Vp, we get the following: (1 + RP2/RP1) = (1 + RF/RG)/(1 – 1/n) Figure 6. Standard Cable/Line Back-Termination |
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