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LT3434 Datasheet(PDF) 13 Page - Linear Technology |
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LT3434 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() LT3434 13 3434f APPLICATIO S I FOR ATIO 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 () – = ()( )( ) ()( ) 22 2 CHOOSING THE INDUCTOR For most applications the output inductor will fall in the range of 15µH to 100µH. 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 LT3434 switch, which has a minimum 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 LT3434 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. Table 3. Inductor Selection Criteria VENDOR/ VALUE IDC DCR HEIGHT PART NO. ( µH) (Amps) (Ohms) (mm) Sumida CDRH104R-150 15 3.6 0.050 4 CDRH104R-220 22 2.9 0.073 4 CDRH104R-330 33 2.3 0.093 4 CDRH124-220 22 2.9 0.066 4.5 CDRH124-330 33 2.7 0.097 4.5 CDRH127-330 33 3.0 0.065 8 CDRH127-470 47 2.5 0.100 8 CEI122-220 22 2.3 0.085 3 Coiltronics UP3B-330 33 3 0.069 6.8 UP3B-470 47 2.4 0.108 6.8 UP4B-680 68 4.3 0.120 7.9 Coilcraft DO3316P-153 15 3 0.046 5.2 DO5022p-683 68 3.5 0.130 7.1 |
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