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LTC660 датащи(PDF) 8 Page - Linear Technology |
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LTC660 датащи(HTML) 8 Page - Linear Technology |
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8 / 12 page ![]() 8 LTC660 TYPICAL APPLICATIONS N Voltage Doubling Figure 8 shows the LTC660 operating in the voltage doubling mode. The external Schottky (1N5817) diode is for start-up only. The output voltage is 2 • VIN without a load. The diode has no effect on the output voltage. 1 2 3 4 8 7 6 5 BOOST CAP+ GND CAP– LTC660 • F08 C1 150 µF VOUT = 2VIN VIN 2.5V TO 5.5V LTC660 1N5817* V+ OSC LV VOUT C2 150 µF * SCHOTTKY DIODE IS FOR START-UP ONLY + + Figure 8. Voltage Doubler Negative Voltage Converter Figure 7 shows a typical connection which will provide a negative supply from an available positive supply. This circuit operates over full temperature and power supply ranges without the need of any external diodes. The LV pin (Pin 6) is shown grounded, but for V+ ≥ 3V, it may be floated, since LV is internally switched to ground (Pin 3) for V + ≥ 3V. The output voltage (Pin 5) characteristics of the circuit are those of a nearly ideal voltage source in series with a 6.5 Ω resistor. The 6.5 Ω output impedance is composed of two terms: 1) the equivalent switched-capacitor resistance (see Theory of Operation), and 2) a term related to the on- resistance of the MOS switches. At an oscillator frequency of 10kHz and C1 = 150 µF, the first term is: R= 1 f/2 EQUIV OSC () = = C1 1 5 10 150 10 13 36 •• • . – Ω. Notice that the equation for REQUIV is not a capacitive reactance equation (XC = 1/ωC) and does not contain a 2 π term. The exact expression for output impedance is complex, but the dominant effect of the capacitor is clearly shown on the typical curves of output impedance and power effi- ciency versus frequency. For C1 = C2 = 150 µF, the output impedance goes from 6.5 Ω at fOSC = 10kHz to 110Ω at fOSC = 100Hz. As the 1/fC term becomes large compared to the switch on-resistance term, the output resistance is determined by 1/fC only. Ultraprecision Voltage Divider An ultraprecision voltage divider is shown in Figure 9. To achieve the 0.002% accuracy indicated, the load current should be kept below 100nA. However, with a slight loss in accuracy, the load current can be increased. 1 2 3 4 8 7 6 5 BOOST CAP+ GND CAP– C2 150 µF LTC660 • F07 C1 150 µF VOUT = –VIN VIN 1.5V TO 5.5V LTC660 V+ OSC LV VOUT + Figure 7. Voltage Inverter Battery Splitter A common need in many systems is to obtain positive and negative supplies from a single battery or single power supply system. Where current requirements are small, the circuit shown in Figure 10 is a simple solution. It provides symmetrical positive or negative output voltages, both equal to one-half the input voltage. The output voltages are both referenced to Pin 3 (Output Common). Figure 9. Ultraprecision Voltage Divider 8 7 6 5 4 3 2 1 C1 150 µF ± 0.002% V+ 3V TO 11V LTC660 • F09 TMIN ≤ TA ≤ TMAX IL ≤ 100nA C2 150 µF 2 V+ LTC660 + + |
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