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LTC3859 Datasheet(PDF) 21 Page - Linear Technology |
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LTC3859 Datasheet(HTML) 21 Page - Linear Technology |
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21 / 40 page ![]() LTC3859 21 3859f APPLICATIONS INFORMATION The maximum power loss in R1 is related to duty cycle. For the buck controllers, the maximum power loss will occur in continuous mode at the maximum input voltage: PLOSS R1= (VIN(MAX) − VOUT)• VOUT R1 For the boost controller, the maximum power loss in R1 will occur in continuous mode at VIN = 1/2•VOUT: PLOSS R1= (VOUT(MAX) − VIN)• VIN R1 Ensure that R1 has a power rating higher than this value. If high efficiency is necessary at light loads, consider this power loss when deciding whether to use DCR sensing or sense resistors. Light load power loss can be modestly higher with a DCR network than with a sense resistor, due to the extra switching losses incurred through R1. However, DCR sensing eliminates a sense resistor, reduces conduc- tion losses and provides higher efficiency at heavy loads. Peak efficiency is about the same with either method. Inductor Value Calculation The operating frequency and inductor selection are inter- related in that higher operating frequencies allow the use of smaller inductor and capacitor values. So why would anyone ever choose to operate at lower frequencies with larger components? The answer is efficiency. A higher frequency generally results in lower efficiency because of MOSFET gate charge losses. In addition to this basic trade-off, the effect of inductor value on ripple current and low current operation must also be considered. The inductor value has a direct effect on ripple current. The inductor ripple current ΔIL decreases with higher inductance or frequency. For the buck controllers, ΔIL increases with higher VIN: ΔIL = 1 (f)(L) VOUT 1− VOUT VIN ⎛ ⎝⎜ ⎞ ⎠⎟ For the boost controller, the inductor ripple current ΔIL increases with higher VOUT: ΔIL = 1 (f)(L) VIN 1− VIN VOUT ⎛ ⎝⎜ ⎞ ⎠⎟ Accepting larger values of ΔIL allows the use of low inductances, but results in higher output voltage ripple and greater core losses. A reasonable starting point for setting ripple current is ΔIL = 0.3(IMAX). The maximum ΔIL occurs at the maximum input voltage for the bucks and VIN = 1/2•VOUT for the boost. The inductor value also has secondary effects. The tran- sition to Burst Mode operation begins when the average inductor current required results in a peak current below 25% of the current limit (30% for the boost) determined by RSENSE. Lower inductor values (higher ΔIL) will cause this to occur at lower load currents, which can cause a dip in efficiency in the upper range of low current operation. In Burst Mode operation, lower inductance values will cause the burst frequency to decrease. Inductor Core Selection Once the value for L is known, the type of inductor must be selected. High efficiency converters generally cannot afford the core loss found in low cost powdered iron cores, forcing the use of more expensive ferrite or molypermalloy cores. Actual core loss is independent of core size for a fixed inductor value, but it is very dependent on inductance selected. As inductance increases, core losses go down. Unfortunately, increased inductance requires more turns of wire and therefore copper losses will increase. Ferrite designs have very low core loss and are preferred at high switching frequencies, so design goals can con- centrate on copper loss and preventing saturation. Ferrite core material saturates “hard,” which means that induc- tance collapses abruptly when the peak design current is exceeded. This results in an abrupt increase in inductor ripple current and consequent output voltage ripple. Do not allow the core to saturate! Power MOSFET and Schottky Diode (Optional) Selection Two external power MOSFETs must be selected for each controller in the LTC3859: one N-channel MOSFET for the top switch (main switch for the buck, synchronous for the boost), and one N-channel MOSFET for the bottom switch (main switch for the boost, synchronous for the buck). |
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