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LT1007 датащи(PDF) 19 Page - Texas Instruments |
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LT1007 датащи(HTML) 19 Page - Texas Instruments |
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19 / 24 page ![]() LT1007, LT1007A, LT1037, LT1037A LOW-NOISE, HIGH-SPEED, PRECISION OPERATIONAL AMPLIFIERS SLOS017C – D3195, FEBRUARY 1989 – REVISED JANUARY 1993 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 19 APPLICATION INFORMATION Special test precautions are required to measure the typical 60-nV peak-to-peak noise performance of the LT1007 and LT1037: 1. The device should be warmed up for at least five minutes. As the operational amplifier warms up, the offset voltage typically changes 3 µV, due to the chip temperature increasing 10°C to 20°C from the moment the power supplies are turned on. In the 10-second measurement interval, these temperature-induced effects can easily exceed tens of nanovolts. 2. The device must be well shielded from air currents to eliminate thermoelectric effects. In excess of a few nanovolts, thermoelectric effects would invalidate the measurements. 3. Sudden motion in the vicinity of the device can produce a feedthrough effect that increases observed noise. When measuring noise on a large number of units, a noise-voltage density test is recommended. A 10-Hz noise-voltage density measurement will correlate well with a 0.1-Hz to 10-Hz peak-to-peak noise reading since both results are determined by the white noise and the location of the 1/f corner frequency. Figure 40 shows a circuit that measures noise current and presents the formula for calculating noise current. eno 500 k Ω 10 k Ω 500 k Ω 100 Ω In + [vn2 * (130 nV)2]1 2 1M W x 100 Figure 40. Noise Test Circuit The LT1007 and LT1037 achieve low noise, in part, by operating the input stage at 120 µA versus the typical 10 µA for most other operational amplifiers. Voltage noise is directly proportional to the square root of the stage current; therefore, the LT1007 and LT1037 noise current is relatively high. At low frequencies, the low 1/f current-noise corner frequency ( ≈120 Hz) minimizes noise current to some extent. In most practical applications, however, noise current will not limit system performance; this is illustrated in Figure 27, where: total noise = [(noise voltage)2(noise current x RS)2 + (resistor noise)2]1/2 Three regions can be identified as a function of source resistance: (i) RS ≤ 400 Ω Voltage noise dominates in region (i) (ii) RS = 400 Ω to 50 kΩ at 1 kHz Resistor noise dominates in region (ii) RS = 400 Ω to 8 kΩ at 10 kHz (iii) RS > 50 Ω at 1 kHz Current noise dominates in region (iii) RS > 8 kΩ at 10 Hz The LT1007 and LT1037 should not be used in region (iii) where total system noise is at least six times higher than the noise voltage of the operational amplifier (i.e., the low-voltage noise specification is completely wasted). |
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