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LTC1439CG 数据表(PDF) 13 Page - Linear Technology |
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LTC1439CG 数据表(HTML) 13 Page - Linear Technology |
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13 / 32 page ![]() 13 LTC1438/LTC1439 APPLICATIONS INFORMATION Accepting larger values of ∆IL 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 ∆IL = 0.4(IMAX). Remember, the maximum ∆IL occurs at the maximum input voltage. The inductor value also has an effect on low current operation. The transition to low current operation begins when the inductor current reaches zero while the bottom MOSFET is on. Lower inductor values (higher ∆IL) will cause this to occur at higher load currents, which can cause a dip in efficiency in the upper range of low current operation. In Burst Mode operation (TGS1, 2 pins open), lower inductance values will cause the burst frequency to decrease. The Figure 3 graph gives a range of recommended induc- tor values vs operating frequency and VOUT. 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! Molypermalloy (from Magnetics, Inc.) is a very good, low loss core material for toroids, but it is more expensive than ferrite. A reasonable compromise from the same manu- facturer is Kool M µ. Toroids are very space efficient, especially when you can use several layers of wire. Be- cause they generally lack a bobbin, mounting is more difficult. However, designs for surface mount are available which do not increase the height significantly. Power MOSFET and D1 Selection Three external power MOSFETs must be selected for each controller with the LTC1439: a pair of N-channel MOSFETs for the top (main) switch and an N-channel MOSFET for the bottom (synchronous) switch. Only one top MOSFET is required for each LTC1438 controller. To take advantage of the Adaptive Power output stage, two topside MOSFETs must be selected. A large [low RSD(ON)] MOSFET and a small [higher RDS(ON)] MOSFET are re- quired. The large MOSFET is used as the main switch and works in conjunction with the synchronous switch. The smaller MOSFET is only enabled under low load current conditions. The benefit of this is to boost low to midcurrent efficiencies while continuing to operate at constant fre- quency. Also, by using the small MOSFET the circuit will keep switching at a constant frequency down to lower currents and delay skipping cycles. The RDS(ON) recommended for the small MOSFET is around 0.5 Ω. Be careful not to use a MOSFET with an RDS(ON) that is too low; remember, we want to conserve gate charge. (A higher RDS(ON) MOSFET has a smaller gate capacitance and thus requires less current to charge its gate). For all LTC1438 and cost sensitive LTC1439 appli- cations, the small MOSFET is not required. The circuit then begins Burst Mode operation as the load current drops. Inductor Core Selection Once the value for L is known, the type of inductor must be selected. High efficiency converters generally cannot af- ford the core loss found in low cost powdered iron cores, forcing the use of more expensive ferrite, molypermalloy or Kool M µ® 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. Kool M µ is a registered trademark of Magnetics, Inc. OPERATING FREQUENCY (kHz) 0 0 10 20 30 40 60 50 100 150 200 1438 F03 250 300 50 VOUT = 5.0V VOUT = 3.3V VOUT = 2.5V Figure 3. Recommended Inductor Values |
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