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LT3435 Datasheet(PDF) 13 Page - Linear Technology |
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LT3435 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() LT3435 13 3435fa To calculate actual peak switch current in continuous mode with a given set of conditions, use: II VV V Lf V SW PK OUT OUT IN OUT IN () – =+ () ()( )( ) 2 If a small inductor is chosen which results in discontinous mode operation over the entire load range, the maximum load current is equal to: I If L V VV V OUT MAX PK IN OUT IN OUT () – = ()( )( ) ()( ) 2 2 2 CHOOSING THE INDUCTOR For most applications the output inductor will fall in the range of 5 µH to 33µH. Lower values are chosen to reduce physical size of the inductor. Higher values allow more output current because they reduce peak current seen by the LT3435 switch, which has a 3A limit. Higher values also reduce output ripple voltage and reduce core loss. When choosing an inductor you might have to consider maximum load current, core and copper losses, allow- able component height, output voltage ripple, EMI, fault current in the inductor, saturation and of course cost. The following procedure is suggested as a way of han- dling these somewhat complicated and conflicting requirements. 1. Choose a value in microhenries such that the maximum load current plus half of the inductor ripple current is less than the minimum peak switch current (IPK). Choosing a small inductor with lighter loads may result in discontinuous mode of operation, but the LT3435 is designed to work well in either mode. Assume that the average inductor current is equal to load current and decide whether or not the inductor must withstand continuous fault conditions. If maxi- mum load current is 1A, for instance, a 1A inductor may not survive a continuous 4A overload condition. For applications with a duty cycle above 50%, the inductor value should be chosen to obtain an inductor ripple current of less than 40% of the peak switch current. 2. Calculate peak inductor current at full load current to ensure that the inductor will not saturate. Peak current can be significantly higher than output current, especially with smaller inductors and lighter loads, so don’t omit this step. Powdered iron cores are forgiving because they saturate softly, whereas ferrite cores saturate abruptly. Other core materials fall somewhere in between. The following formula assumes continuous mode of opera- tion, but it errs only slightly on the high side for discon- tinuous mode, so it can be used for all conditions. II VV V fL V PEAK OUT OUT IN OUT IN =+ () ()( )( ) – 2 VIN = maximum input voltage f = switching frequency, 500kHz Table 3. Inductor Selection Criteria VENDOR/ VALUE IDC(MAX) DCR HEIGHT PART NO. ( µH) (Amps) (Ohms) (mm) Sumida CDRH104R-4R7 4.7 6 0.013 4 CDRH104R-100 10 4.4 0.035 4 CDRH104R-150 15 3.6 0.050 4 CDRH104R-220 22 2.9 0.073 4 CDRH104R-330 33 2.3 0.093 4 CDRH124-4R7 4.7 5.7 0.015 4.5 CDRH124-100 10 4.5 0.026 4.5 CDRH124-220 22 2.9 0.066 4.5 CDRH124R-330 33 2.7 0.097 4.5 CDRH127-330 33 3.0 0.065 8 CEI122-220 22 2.3 0.085 34 Coiltronics UP3B-4R7 4.7 6.5 0.0083 6.8 UP3B-4R7 10 4.3 0.026 6.8 UP3B-330 33 3 0.069 6.8 APPLICATIO S I FOR ATIO |
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