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LT3437 Datasheet(PDF) 13 Page - Linear Technology |
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LT3437 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() LT3437 13 3437f APPLICATIO S I FOR ATIO more output current because they reduce peak current seen by the LT3437 switch, which has a 0.5A 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 LT3437 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 0.25A, for instance, a 0.25A inductor may not survive a continuous minimum peak switch current 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 do not 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, 200kHz 3. Decide if the design can tolerate an “open” core geom- etry like a rod or barrel, which has high magnetic field radiation, or whether it needs a closed core like a toroid, to prevent EMI problems. This is a tough decision because the rods or barrels are temptingly cheap and small, and there are no helpful guidelines to calculate when the magnetic field radiation will be a problem. 4. After making an initial choice, consider the secondary things like output voltage ripple, second sourcing, etc. Use the experts in Linear Technology’s applications department if you feel uncertain about the final choice. They have experience with a wide range of inductor types and can tell you about the latest developments in low profile, surface mounting, etc. Table 3. Inductor Selection Criteria VENDOR/ VALUE IDC(MAX) DCR HEIGHT PART NO. ( µH) (mA) (Ohms) (mm) Coiltronics UP1B-101 100 530 1.11 5.0 UP1B-151 150 460 1.61 5.0 UP2B-221 220 380 1.96 5.0 Coilcraft D01605T-473MX 47 450 1.1 1.8 D01605T-104MX 100 300 2.3 1.8 D03308P-154 150 600 0.94 3.0 D03308P-224 220 500 1.6 3.0 Sumida CDRH4D28-470 47 480 0.387 3.0 CDRH4D28-101 100 290 1.02 3.0 CDRH5D28-101 100 420 0.520 3.0 Short-Circuit Considerations The LT3437 is a current mode controller. It uses the VC node voltage as an input to a current comparator which turns off the output switch on a cycle-by-cycle basis as this peak current is reached. The internal clamp on the VC node, nominally 1.5V, then acts as an output switch peak current limit. This action becomes the switch current limit specification. The maximum available output power is then determined by the switch current limit. |
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