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LTC1152C 数据表(PDF) 6 Page - Linear Technology |
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LTC1152C 数据表(HTML) 6 Page - Linear Technology |
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6 / 8 page ![]() 6 LTC1152 S APPLICATI I FOR ATIO Rail-to-Rail Operation The LTC1152 is a rail-to-rail input common-mode range, rail-to-rail output swing op amp. Most CMOS op amps, including the entire LTC zero-drift amplifier line, and even a few bipolar op amps, can and do, claim rail-to-rail output swing. One obvious use for such a device is to provide a unity-gain buffer for 0V to 5V signals running from a single 5V power supply. This is not possible with the vast majority of so-called “rail-to-rail” op amps; although the output can swing to both rails, the negative input (which is connected to the output) will exceed the common-mode input range of the device at some point (generally about 1.5V below the positive supply), opening the feedback loop and causing unpredictable and sometimes bizarre behavior. The LTC1152 is an exception to this rule. It features both rail-to-rail output swing and rail-to-rail input common- mode range (CMR); the input CMR actually extends be- yond either rail by about 0.3V. This allows unity-gain buffer circuits to operate with any input signal within the power supply rails; input signal swing is limited only by the output stage swing into the load. Additionally, signals occurring at either rail (power supply current sensing, for example) can be amplified without any special circuitry. Internal Charge Pump The LTC1152 achieves its rail-to-rail input CMR by using a charge pump to generate an internal voltage approxi- mately 2V higher than V+. The input stages of the op amp are run from this higher voltage, making signals at V+ appear to be 2V below the front end’s power supply (Figure 1). The charge pump is contained entirely within the LTC1152; no external components are required. About 100 µVP-P of residual charge pump switching noise will be present on the output of the LTC1152. This feedthrough is at 4.7MHz, higher than the gain-bandwidth of the LTC1152, and will generally not cause any prob- lems. Very sensitive applications can reduce this feedthrough by connecting a capacitor from the CP pin (pin 8) to V+(pin 7); a 0.1 µF capacitor will reduce charge pump feedthrough to negligible levels. The LTC1152 in- cludes an internal diode from pin 8 to pin 7 to prevent external parasitic capacitance from lengthening start-up OUT OUTPUT RAIL TO RAIL INPUT 0.1 µF* *OPTIONAL EXTERNAL CAPACITOR TO REDUCE CHARGE PUMP FEEDTHROUGH VCC + 2V VCC (PIN 7) CP (PIN 8) +IN –IN 1152 F01 INTERNAL CHARGE PUMP Figure 1. LTC1152 Internal Block Diagram time. This diode can stand short-term peak currents of about 50mA, allowing it to quickly charge external capaci- tance to ground or V –. Large capacitors (>1 µF) should not be connected between pin 8 and ground or V – to prevent excessive diode current from flowing at start-up. The LTC1152 can withstand continuous short circuits be- tween pin 8 and V +; however, short circuiting pin 8 to ground or V – will cause large amounts of current to flow through the diode, destroying the LTC1152. Don’t do it. Output Drive The LTC1152 features an enhanced output stage that can sink and source 10mA with a single 5V supply while maintaining rail-to-rail output swing under most loading conditions. The output stage can be modeled as a perfect rail-to-rail voltage source with a resistor in series with it; this open-loop output resistance limits the output swing by creating a resistor divider with the output load. The output resistance drops as total power supply voltage increases, as shown in the typical performance curves. It is typically 140 Ω with a single 5V supply, allowing a 4.4V output swing into a 1k resistor with a single 5V supply. OUT (PIN 6) ≈140Ω AT 5V SUPPLY LTC1152 OUTPUT DRIVER VCC (PIN 7) RLOAD ROUT 1152 F02 Figure 2. LTC1152 Output Resistance Model |
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