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LT1679CS 数据表(PDF) 13 Page - Linear Technology |
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LT1679CS 数据表(HTML) 13 Page - Linear Technology |
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13 / 16 page ![]() LT1678/LT1679 13 sn16789 16789fs Rail-to-Rail Input The input common mode range for the LT1678/LT1679 can exceed the supplies by at least 100mV. As the common mode voltage approaches the positive rail (+VS – 0.7V), the tail current for the input pair (Q1, Q2) is reduced, which prevents the input pair from saturating (refer to the Simplified Schematic). The voltage drop across the load resistors RC1, RC2 is reduced to less than 200mV, degrading the slew rate, bandwidth, voltage noise, offset voltage and input bias current (the cancella- tion is shut off). When the input common mode range goes below 1.5V above the negative rail, the NPN input pair (Q1, Q2) shuts off and the PNP input pair (Q8, Q9) turns on. The offset voltage, input bias current, voltage noise and bandwidth are also degraded. The graph of Offset Voltage Shift vs Common Mode shows where the knees occur by display- ing the change in offset voltage. The change-over points are temperature dependent; see the graph Common Mode Range vs Temperature. Rail-to-Rail Output The rail-to-rail output swing is achieved by using transis- tor collectors (Q28, Q29 referring to the Simplified Sche- matic) instead of customary class A-B emitter followers for the output stage. The output NPN transistor (Q29) sinks the current necessary to move the output in the negative direc- tion. The change in Q29’s base emitter voltage is reflected directly to the gain node (collectors of Q20 and Q16). For large sinking currents, the delta VBE of Q29 can dominate the gain. Figure 7 shows the change in input voltage for a change in output voltage for different load resistors con- nected between the supplies. The gain is much higher for output voltages above ground (Q28 sources current) since the change in base emitter voltage of Q28 is attenuated by the gain in the PNP portion of the output stage. Therefore, for positive output swings (output sourcing current) there is hardly any change in input voltage for any load resistance. Highest gain and best linearity are achieved when the output is sourcing current, which is the case in single supply op- eration when the load is ground referenced. Figure 8 shows gains for both sinking and sourcing load currents for a worst-case load of 600Ω. –15 –10 –5 0 5 10 15 OUTPUT VOLTAGE (V) INPUT VOLTAGE (50µV/DIV) RL = 10k RL = 600Ω RL = 1k 16789 F07 TA = 25°C VS = ±15V RL CONNECTED TO 0V MEASURED ON TEKTRONIX 577 CURVE TRACER 12 03 5 4 OUTPUT VOLTAGE (V) INPUT VOLTAGE (10µV/DIV) RL TO 5V RL TO 0V 16789 F08 VOLTAGE GAIN SINGLE SUPPLY VS = 5V RL = 600Ω MEASURED ON TEKTRONIX 577 CURVE TRACER Figure 7. Voltage Gain Split Supply Figure 8. Voltage Gain Single Supply APPLICATIO S I FOR ATIO |
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