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MAX4193C/D датащи(PDF) 6 Page - Maxim Integrated Products |
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MAX4193C/D датащи(HTML) 6 Page - Maxim Integrated Products |
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6 / 14 page ![]() External Components Resistors Since the LBR and VFB input bias currents are specified as 10nA (max), the current in the dividers R1/R2 and R3/R4 (Figure 1) may be as low as 1µA without signifi- cantly affecting accuracy. Normally R2 and R4 are between 10k Ω and 1MΩ, which sets the current in the voltage-dividers in the 1.3µA to 130µA range. R1 and R3 can then be calculated as follows: where VOUT is the desired output voltage and VLB is the desired low-battery warning threshold. If the IC (shutdown) input is pulled up through a resistor rather than connected directly to +VS, the current through the pullup resistor should be a minimum of 4µA with IC at the input-high threshold of 1.3V: Inductor Value The available output current from a DC-DC voltage boost converter is a function of the input voltage, exter- nal inductor value, output voltage, and the operating frequency. The inductor must 1) have the correct inductance, 2) be able to handle the required peak currents, and 3) have acceptable series resistance and core losses. If the inductance is too high, the MAX630 will not be able to deliver the desired output power, even with the LX out- put on for every oscillator cycle. The available output power can be increased by either decreasing the inductance or the frequency. Reducing the frequency increases the on-period of the LX output, thereby increasing the peak inductor current. The available out- put power is increased since it is proportional to the square of the peak inductor current (IPK). where POUT includes the power dissipated in the catch diode (D1) as well as that in the load. If the inductance is too low, the current at LX may exceed the maximum rating. The minimum allowed inductor value is expressed by: where IMAX ≈ 525mA (peak LX current) and tON is the on-time of the LX output. The most common MAX630 circuit is a boost-mode converter (Figure 1). When the N-channel output device is on, the current linearly rises since: At the end of the on-time (14µs for 40kHz, 55% duty- cycle oscillator) the current is: The energy in the coil is: At maximum load, this cycle is repeated 40,000 times per second, and the power transferred through the coil is 40,000 x 5.25 = 210mW. Since the coil only supplies the voltage above the input voltage, at 15V, the DC-DC converter can supply 210mW / (15V - 5V) = 21mA. The coil provides 210mW and the battery directly supplies another 105mW, for a total of 315mW of output power. If the load draws less than 21mA, the MAX630 turns on its output only often enough to keep the output voltage at a constant 15V. Reducing the inductor value increases the available output current: lower L increases the peak current, thereby increasing the available power. The external inductor required by the MAX630 is readily obtained from a variety of suppliers (Table 1). Standard coils are suitable for most applications. Types of Inductors Molded Inductors These are cylindrically wound coils that look similar to 1W resistors. They have the advantages of low cost and ease of handling, but have higher resistance, higher losses, and lower power handling capability than other types. ImA pk VT L Vx s H ON == μ μ = 514 470 150 di dt V L = LMIN VT I IN ON MAX = L VT f P ce P LI f and I IN ON OUT OUT pk pk VT L IN ON = = = () sin : : 2 2 2 2 R VV A IC S ≤ +− μ 13 4 . 10 2 1 1 2 131 131 10 4 1 3 4 131 131 ΩΩ ΩΩ ≤≤ = − ≤≤ = − . . . . RM R R x VV RM R R x VV OUT LB CMOS Micropower Step-Up Switching Regulator 6 _______________________________________________________________________________________ EJ LIpk = =μ 2 2 525 . |
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