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STLD20D Fiches technique(PDF) 14 Page - STMicroelectronics |
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STLD20D Fiches technique(HTML) 14 Page - STMicroelectronics |
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14 / 31 page ![]() Components selection STLD20D 14/31 7 Components selection 7.1 L, Boost inductor selection To get a good trade-off thickness/efficiency, an attention must be given on the inductor choice. ● The inductance value must be selected to remain in the discontinuous conduction mode. ● Its saturation current (Isat) must be equal or higher than the programmed current (ILIM). ● An attention must be taken on the dynamic inductor parameters. Actually, some power losses can occur in the boost inductor when it works at several hundred KHz and can reduce the efficiency. 7.1.1 Calculation of the inductor value The inductor must be dimensioned so that the STLD20D stays running in discontinuous conduction mode operation in the worst operation condition (VIN = VIN_min= 2.8V). The limit between continuous and discontinuous mode is called critical mode and characterized by an uninterrupted current through the inductor (see figure 18). The formula [1] gives the maximum typical value of the inductor for a discontinuous mode operation in the worst case condition (critical mode). Figure 19 shows the typical L value versus the voltage across the LED branch N.VLED. Note that this curve includes the STLD20D and inductance dispersions (20%). N.VLED = 4x4V = 16V and ILOAD = 20mA Figure 18. 3 different conduction modes IL Continuous Discontinuous Critical t L typ η V 2 in min () NVLED V in min () – V FB I LED R LDS ⋅ ++ ⋅ () ⋅ 2.4 I LED NV LED F max NV LED I LED R LDS ⋅ + ⋅ () ⋅⋅ ⋅ ⋅ ⋅ -------------------------------------------------------------------------------------------------------------------------------------------------------------- 1 [] ≤ |
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