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LED5000 数据表(PDF) 30 Page - STMicroelectronics |
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LED5000 数据表(HTML) 30 Page - STMicroelectronics |
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30 / 52 page ![]() Application notes - buck conversion LED5000 30/51 Doc ID 023951 Rev 1 Equation 45 where DCRL is the series resistance of the inductor and VFWDIODE is the forward voltage drop across the external rectifying diode. The pulse-by-pulse current limitation is effective to implement constant current protection when: Equation 46 From Equation 44 and Equation 45 we can gather that the implementation of the constant current protection becomes more critical the lower is the VOUT and the higher is 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 forward voltage of the diode) since VOUT is negligible, while during TON the voltage applied the inductor is maximized and it is approximately equal to VIN. In general the worst case scenario is heavy short-circuit at the output with maximum input voltage. The Equation 44 and Equation 45 in overcurrent conditions can be simplified to: Equation 47 considering TON that has been already reduced to its minimum. Equation 48 where TSW=1/fSW considering the nominal fSW. At high input voltage ΔI L TON could be higher than ΔI L TOFF and so the inductor current could escalate. As a consequence, the system typically meets the Equation 46 at a current level higher than the nominal value thanks to the increased voltage drop across stray components. In most 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. The hiccup protection offers an additional protection against heavy short-circuit condition at very high input voltage even considering the spread of the minimum conduction time of the power element. In case the hiccup current level (6.2 A typical) is triggered the switching activity is prevented for 16 msec typ. (see hiccup time in Table 5: Electrical characteristics). Figure 19 shows the operation of the constant current protection when a short-circuit is applied at the output at the maximum input voltage. I L TON Δ V OUT DCR L IV FW DIODE + ⋅ + () – L ---------------------------------------------------------------------------------------- T OFF () = I L TON Δ I L TOFF Δ = I L TON Δ V IN DCR L R DSON HS + () I ⋅ – L --------------------------------------------------------------------------- T ON MIN () V IN L --------- 90ns () ≅ = I L TOFF Δ DCR L I ⋅ V FW DIODE + () – L ------------------------------------------------------------------- T SW 90ns – () DCR L I ⋅ V FW DIODE + () – L ------------------------------------------------------------------- 1.18 μs () ≅ = |
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