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LT4351CMS датащи(PDF) 15 Page - Linear Technology |
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LT4351CMS датащи(HTML) 15 Page - Linear Technology |
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15 / 20 page ![]() LT4351 15 sn4351 4351fs APPLICATIO S I FOR ATIO The die junction temperature is then computed as: TJ = TA + θJA • PTOTAL where TJ is the die junction temperature, TA is the ambient temperature, θJA is the thermal resistance of the part (120 °C/W) and PTOTAL is ascertained from the above. Therefore, a 0.1W power dissipation causes a 12 degree temperature rise above ambient. Design Example The following demonstrates the calculations involved for setting design components for a 5V system that requires 5A. Two supplies are used to do this. The VIN supply will be deemed in spec when it is within ±5% of nominal. Allow 5% of hysteresis for UV. So, UVFAULT = 4.75V, UVHYST = 0.25V OVFAULT = 5.5 Two separate resistive dividers are used. For the UV divider: R UV I V A k Use k R RV UV V kV VV HYST UVHYST UV FAULT UV 2 025 10 25 24 9 1 2 249 03 475 0 3 == µ = () == . . • – .• . .– . R1 = 1.68k. The closest 1% value is 1.69k Figure 14. Total Power (Typical) Figure 13. PGATE vs VIN (VDD = VIN + 10.7) The OV resistors are set as a straight resistive divider. If the current in the RA, RB divider is 200 µA, then: R R OV V k A B FAULT OV = µ = = = = 0.3V 200 A 1.5k use 1.47k (1%) then R R 25.48k use 25.5k A B – . . –. 1 55 03 11 47 For regulation, the MOSFETs must have: R mV A m DS <= Ω 15 25 15 • . This very low value cannot be accomplished with a single set of MOSFETs so a decision must be made whether to use multiple MOSFETs or to live with an unregulated offset. Since low m Ω RDS(ON) is available, the IR drop using a single FET would still be acceptable. For RDS(ON) = 4m Ω the drop is 2 • 5A • 4mΩ = 40mV. The finished schematic is shown in Figure 15. VIN (V) 0 0.002 0.003 20 4351 F13 0.001 0 5 10 15 0.004 fGATE = 1kHz QG = 50nC VIN (V) 0 0.10 0.12 20 4351 F14 0.08 0.06 5 10 15 0.16 0.14 L = 10 µH L = 4.7 µH VDD = VIN + 10 0.5mA GATE CURRENT |
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