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LTC1144CS8 датащи(PDF) 7 Page - Linear Technology |
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LTC1144CS8 датащи(HTML) 7 Page - Linear Technology |
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7 / 8 page ![]() 7 LTC1144 Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen- tation that the interconnection of its circuits as described herein will not infringe on existing patent rights. S APPLICATI TYPICAL Negative Voltage Converter Figure 8 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 output voltage (pin 5) characteristics of the circuit are those of a nearly ideal voltage source in series with a 56 Ω resistor. The 56 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. Figure 9. Voltage Doubler 1 2 3 4 8 7 6 5 + + + + VIN 2V TO 18V VOUT = 2(VIN – 1) 10 µF10µF Vd 1N4148 Vd 1N4148 1144 F09 LTC1144 Ultra-Precision Voltage Divider An ultra-precision voltage divider is shown in Figure 10. To achieve the 0.0002% accuracy indicated, the load current should be kept below 100nA. However, with a slight loss in accuracy, the load current can be increased. At an oscillator frequency of 10kHz and C1 = 10 µF, the first term is: R fC EQUIV OSC = ()× = ×× × = − 1 21 1 510 10 10 20 36 / Ω Notice that the above equation for REQUIV is not a capaci- tive reactance equation (XC = 1/ωC) and does not contain a 2 π term. The exact expression for output impedance is extremely complex, but the dominant effect of the capacitor is clearly shown in Figure 5. For C1 = C2 = 10 µF, the output impedance goes from 56 Ω at fOSC = 10kHz to 250Ω at fOSC = 1kHz. As the 1/(f × C) term becomes large compared to the switch on-resistance term, the output resistance is determined by 1/(f × C) only. Voltage Doubling Figure 9 shows a two-diode capacitive voltage doubler. With a 15V input, the output is 29.45V with no load and 28.18V with a 10mA load. Figure 8. Negative Voltage Converter 1 2 3 4 8 7 6 5 + 10 µF 10 µF V+ 2V TO 18V VOUT = –V + TMIN ≤ TA ≤ TMAX 1144 F08 LTC1144 1 2 3 4 8 7 6 5 + + C2 10 µF C1 10 µF V+ 4V TO 36V 1144 F10 LTC1144 ±0.002% TMIN ≤ TA ≤ TMAX IL ≤ 100nA V+ 2 Figure 10. Ultra-Precision Voltage Divider Battery Splitter A common need in many systems is to obtain (+) and (–) supplies from a single battery or single power supply system. Where current requirements are small, the circuit shown in Figure 11 is a simple solution. It provides symmetrical ± output voltages, both equal to one half the input voltage. The output voltages are both referenced to pin 3 (output common). 1 2 3 4 8 7 6 5 + C2 10 µF C1 10 µF OUTPUT COMMON VB/2 9V –VB/2 –9V 1144 F11 LTC1144 VB 18V + Figure 11. Battery Splitter |
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