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LT1792IN8 Datasheet(PDF) 8 Page - Linear Technology |
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LT1792IN8 Datasheet(HTML) 8 Page - Linear Technology |
8 / 12 page 8 LT1792 S APPLICATI I FOR ATIO best bipolar op amps, with higher current noise, will eventually lose out to the LT1792 when transducer imped- ance increases. The low voltage noise of the LT1792 allows it to surpass most single JFET op amps available. For the best performance versus area available anywhere, the LT1792 is offered in the SO-8 surface mount package with no degradation in performance. The low voltage and current noise offered by the LT1792 makes it useful in a wide range of applications, especially where high impedance, capacitive transducers are used such as hydrophones, precision accelerometers and photo diodes. The total output noise in such a system is the gain times the RMS sum of the op amp input referred voltage noise, the thermal noise of the transducer, and the op amp bias current noise times the transducer impedance. Figure 2 shows total input voltage noise versus source resistance. In a low source resistance (<5k) application the op amp voltage noise will dominate the total noise. This means the LT1792 will beat out any JFET op amp, only the lowest noise bipolar op amps have the edge at low source resistances. As the source resistance in- creases from 5k to 50k, the LT1792 will match the best bipolar op amps for noise performance, since the thermal noise of the transducer (4kTR) begins to dominate the total noise. A further increase in source resistance, above 50k, is where the op amp’s current noise component (2qIB RTRANS) will eventually dominate the total noise. At these high source resistances, the LT1792 will out perform the lowest noise bipolar op amp due to the inherently low Figure 3. Noninverting and Inverting Gain Configurations R2 OUTPUT RB CB R1 CS RS CB ≅ CS RB = RS RS > R1 OR R2 TRANSDUCER OUTPUT CF CB RB CB = CFCS RB = RFRS RF CS RS TRANSDUCER 1792 F03 Q = CV; = I = C dQ dt dV dt SOURCE RESISTANCE ( Ω) 100 1 10 1k 1k 100M 1792 F02 100k 100 10M 10k 1M RESISTOR NOISE ONLY Vn = AV √Vn 2 (OP AMP) + 4kTR + 2qIB • R 2 + – CS RS VO CS RS LT1007 LT1792 LT1007* LT1792* SOURCE RESISTANCE = 2RS = R * PLUS RESISTOR † PLUS RESISTOR 1000pF CAPACITOR LT1792 † LT1007 † Figure 2. Comparison of LT1792 and LT1007 Total Output 1kHz Voltage Noise Versus Source Resistance current noise of FET input op amps. Clearly, the LT1792 will extend the range of high impedance transducers that can be used for high signal-to-noise ratios. This makes the LT1792 the best choice for high impedance, capacitive transducers. The high input impedance JFET front end makes the LT1792 suitable in applications where very high charge sensitivity is required. Figure 3 illustrates the LT1792 in its inverting and noninverting modes of operation. A charge amplifier is shown in the inverting mode example; here the gain depends on the principal of charge conservation at |
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