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LED2001PHR 数据表(PDF) 29 Page - STMicroelectronics |
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LED2001PHR 数据表(HTML) 29 Page - STMicroelectronics |
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29 / 42 page ![]() DocID024346 Rev 1 29/42 LED2001 Application information The inductor current ripple during ON and OFF phases can be written as: • ON phase Equation 40 • OFF phase Equation 41 where DCRL is the series resistance of the inductor. The pulse-by-pulse current limitation is effective to implement constant current protection when: Equation 42 From Equation 40 and Equation 41 it can be seen that the implementation of the constant current protection becomes more critical the lower the VOUT and the higher the VIN. In fact, in short-circuit condition the voltage applied to the inductor during the OFF-time becomes equal to the voltage drop across parasitic components (typically the DCR of the inductor and the RDSON of the low-side switch) since VOUT is negligible, while during TON the voltage applied at the inductor is maximized and is approximately equal to VIN. In general, the worst case scenario is heavy short-circuit at the output with maximum input voltage. Equation 40 and Equation 41 in overcurrent conditions can be simplified to: Equation 43 considering TON which has already been reduced to its minimum. Equation 44 where TSW=1/fSW and considering the nominal fSW. At higher input voltage ΔI L TON may be higher than ΔI L TOFF and so the inductor current can escalate. As a consequence, the system typically meets Equation 42 at a current level higher than the nominal value thanks to the increased voltage drop across stray components. In most of the application conditions the pulse-by-pulse current limitation is effective to limit the inductor current. Whenever the current escalates, a second level current protection called “Hiccup mode” is enabled. Hiccup protection offers an additional protection against heavy short-circuit conditions at very high input voltage even considering the spread I L TON Δ V IN V OUT – DCR L R DSON HS + () I ⋅ – L ----------------------------------------------------------------------------------------------- TON () = I L TON Δ V OUT DCR L R DSON LS + () I ⋅ + () – L ---------------------------------------------------------------------------------------- TOFF () = I L TON Δ I L TOFF Δ = I L TON Δ V IN DCR L R DSON HS + () I ⋅ – L ------------------------------------------------------------------------ TON MIN () V IN L --------- 90ns () ≅ = I L TOFF Δ DCR L R DSON LS + () – I ⋅ L -------------------------------------------------------------- TSW 90ns – () DCR L R DSON LS + () – I ⋅ L -------------------------------------------------------------- 1.18 μs () ≅ = |
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