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LT1990CS8 Datasheet(PDF) 12 Page - Linear Technology |
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LT1990CS8 Datasheet(HTML) 12 Page - Linear Technology |
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12 / 16 page ![]() LT1990 12 1990f APPLICATIO S I FOR ATIO Primary Features The LT1990 is a complete gain-block solution for high input common mode voltage applications, incorporating a low power precision operational amplifier providing rail- to-rail output swing along with on-chip precision thin-film resistors for high accuracy. The Block Diagram shows the internal architecture of the part. The on-chip resistors form a modified difference amplifier including a reference port for introducing offset or other additive waveforms. With pin-strapping alone either unity gain or gain of 10 is produced with high precision. The resistor network is designed to produce internal common-mode voltage divi- sion of 27 so that a very large input range is available compared to the power supply voltage(s) used by the LT1990 itself. The LT1990 is ideally suited to situations where relatively small signals need to be extracted from high voltage circuits, as is the case in many current monitoring instrumentation applications for example. With the ability to accept a range of input voltages well outside the limits of the local power rails and its greater than 1MΩ input impedances, development of precision low power over-the-top and under-the-bottom instrumentation de- signs is greatly simplified with the LT1990 single chip solution over conventional discrete implementations. Classic Difference Amplifier Used in the basic difference amplifier topology where the gain G is pin-strap configurable to be unity or ten, the following relationship is realized: VO = G • (V+IN – V–IN) + VREF To operate in unity gain, the GAIN1 and GAIN2 pins are left disconnected. For G = 10 operation, the GAIN1 and GAIN2 pins are simply connected together or tied to a common potential such as ground or V–. The input common mode range capability is up to ±250V, governed by the following relationships: For G = 1 and G = 10 where GAIN1 and GAIN2 are only tied together (not grounded,etc): VCM+ ≤ 27 • V+ – 26 • VREF – 23 VCM– ≥ 27 • V– – 26 • VREF + 27 For G = 10 where GAIN1 and GAIN2 are tied to a common potential VGAIN: VCM+ ≤ 27 • V+ – 26 • VREF – 23 – VGAIN VCM– ≥ 27 • V– – 26 • VREF + 27 – VGAIN For split supplies over about ±11V, the full ±250V common mode range is normally available (with VREF a small fraction of the supply). With lower supply voltages, an appropriate selection of VREF can tailor the input common mode range to a specific requirement. As an example, the following low supply voltage scenarios are readily imple- mented with the LT1990: Supply VREF VCM Range +3V 1.25V –5V to 25V (e.g. 12V automotive environment) +5V 1.25V –5V to 80V (e.g. 42V automotive environment) +5V 4.00V –77V to 8V (e.g. telecom environment; use downward signaling) Configuring Other Gains An intermediate gain G ranging between 1 and 10 may be produced by placing an adjustable resistance between the GAIN1 and GAIN2 pins according to the following nominal relationship: RGAIN ≈ (180k/(G – 1)) – 20k While the expression is exact, the value is approximate because the absolute resistance of the internal network could vary on a unit-to-unit basis by as much as ±30% from the nominal figures and the external gain resistance is required to accommodate that deviation. Once ad- justed, however, the gain stability is excellent by virtue of the –30ppm/°C typical temperature coefficient offered by the on-chip thin-film resistor process. Preserving and Enhancing Common Mode Rejection The basic difference amplifier topology of the LT1990 requires that source impedances seen by the input pins +IN and –IN, should be matched to within a few tens of ohms to avoid increasing common mode induced errors beyond the basic production limits of the part. Known source imbalances beyond that level should be compen- sated for by the addition of series resistance to the lower- |
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