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LT6210CS6 датащи(PDF) 13 Page - Linear Technology |
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LT6210CS6 датащи(HTML) 13 Page - Linear Technology |
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13 / 16 page ![]() 13 LT6210/LT6211 62101f Capacitive Loads The LT6210/LT6211 are stable with any capacitive load. Although peaking and overshoot may result in the AC transient response, the amplifier’s compensation decreases bandwidth with increasing output capacitive load to en- sure stability. To maintain a response with minimal peak- ing, the feedback resistor can be increased at the cost of bandwidth as shown in the Typical Performance Charac- teristics. Alternatively, a small resistor (5 Ω to 35Ω) can be put in series with the output to isolate the capacitive load from the amplifier output. This has the advantage that the amplifier bandwidth is only reduced when the capacitive load is present. The disadvantage of this technique is that the gain is a function of the load resistance. Power Supplies The LT6210/LT6211 will operate on single supplies from 3V to 12V and on split supplies from ±1.5V to ±6V. If split supplies of unequal absolute value are used, input offset voltage and inverting input current will shift from the values specified in the Electrical Characteristics table. Input offset voltage will shift 2mV and inverting input current will shift 0.5 µA for each volt of supply mismatch. Slew Rate Unlike a traditional voltage feedback op amp, the slew rate of a current feedback amplifier is not independent of the amplifier gain configuration. In a current feedback ampli- fier, both the input stage and the output stage have slew rate limitations. In the inverting mode, and for gains of 2 or more in the noninverting mode, the signal amplitude between the input pins is small and the overall slew rate is that of the output stage. For gains less than 2 in the noninverting mode, the overall slew rate is limited by the input stage. The input slew rate of the LT6210/LT6211 on ±5V supplies with an RSET resistor of 20k (IS = 6mA) is approximately 600V/ µs and is set by internal currents and capacitances. The output slew rate is additionally con- strained by the value of the feedback resistor and internal capacitance. At a gain of 2 with 887 Ω feedback and gain resistors, ±5Vsuppliesandthesamebiasingasabove,the output slew rate is typically 700V/ µs. Larger feedback resistors, lower supply voltages and lower supply current levels will all reduce slew rate. Input slew rates signifi- cantly exceeding the output slew capability can actually decrease slew performance in a positive gain configura- tion; the cleanest transient response will be obtained from input signals with slew rates slower than 1000V/ µs. Output Swing and Drive The output stage of the LT6210/LT6211 consists of a pair of class-AB biased common emitters that enable the output to swing rail-to-rail. Since the amplifiers can poten- tially deliver output currents well beyond the specified minimum short-circuit current, care should be taken not to short the output of the device indefinitely. Attention must be paid to keep the junction temperature of the IC below the absolute maximum rating of 150 °C if the output is used to drive low impedance loads. See Note 5 for details. Additionally, the output of the amplifier has re- verse-biased ESD diodes connected to each supply. If the output is forced beyond either supply, large currents will flow through these diodes. If the current is limited to 80mA or less, no damage to the part will occur. APPLICATIO S I FOR ATIO TYPICAL APPLICATIO 3V Cable Driver with Active Termination Driving back-terminated cables on single supplies usually results in very limited signal amplitude at the receiving end of the cable. However, positive feedback can be used to reduce the size of the series back termination resistor, thereby decreasing the attenuation between the series and shunt termination resistors while still maintaining con- trolled output impedance from the line-driving amplifier. Figure 3 shows the LT6210 using this “active termination” scheme on a single 3V supply. The amplifier is AC-coupled and in an inverting gain configuration to maximize the input signal range. The gain from VIN to the receiving end of the cable, VOUT, is set to –1. The effective impedance looking into the amplifier circuit from the cable is 50 Ω throughout the usable bandwidth. |
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