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LTC3704 Datasheet(PDF) 14 Page - Linear Technology |
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LTC3704 Datasheet(HTML) 14 Page - Linear Technology |
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14 / 28 page ![]() 14 LTC3704 sn3704 3704fs internal ramp compensation (at duty cycles above 50%), and the converter operation will approach voltage mode (ramp compensation reduces the gain of the current loop). If too small an inductor is used, but the converter is still operating in CCM (near critical conduction mode), the internal ramp compensation may be inadequate to prevent subharmonic oscillation. To ensure good current mode gain and avoid subharmonic oscillation, it is recom- mended that the ripple current in the inductor fall in the range of 20% to 40% of the maximum average switch current. For example, if the maximum average switch current is 1A, choose a ∆IL between 0.2A and 0.4A, and a value ‘χ’ between 0.2 and 0.4. Inductor Selection Selecting inductors for a positive-to-negative converter is slightly more complicated than for a single-inductor topol- ogy like a buck or boost. The use of separate, uncoupled inductors can reduce the size of the solution, at the expense of input and output ripple. Using a coupled inductor complicates the design procedure, but can result in significantly lower input and/or output ripple. It will also reduce the number of components that the purchasing department has to keep track of. Regardless of the design goals, however, the inductor selection process is an iterative one. The best recommen- dation is to use the equations as a guideline, and then to build a solution and measure the circuit’s performance. If the measured performance deviates from the design guide- lines, substitute a bigger (or smaller) inductor, as appro- priate, and repeat the measurements. In addition, do your best to minimize layout parasitics, which can have a significant effect on circuit performance. The inductor currents for a positive-to-negative converter are calculated at full load current and minimum input voltage. The peak inductor currents can be significantly higher than the output current, especially with smaller inductors and lighter loads. The following formulae as- sume uncoupled inductors and CCM operation. II D D II L PEAK O MAX MAX MAX L PEAK O MAX 1 2 1 21 1 2 () ( ) () ( ) •• – • =− + =− + χ χ where “ χ” represents the percentage of ripple current. In a positive-to-negative converter, however, the switch cur- rent is the sum of the two inductor currents. Therefore, II D SW PEAK O MAX MAX () ( ) –• • – =+ 1 2 1 1 χ Since the control loop is looking at the switch current, and since the internal slope compensation is acting on this switch current, the ripple current percentage should be between 20% and 40% of the maximum average current at VIN(MIN) and IO(MAX). This corresponds to a value of “χ” in the equations above between 0.20 and 0.40. Expressing this ripple current as a function of the output current results in the following equation for calculating the induc- tor value: LL V If D IN MIN SW MAX 12 == () • • ∆ where: ∆II D SW O MAX MAX = –• • – () χ 1 1 By using a coupled inductor with a 1:1 turns ratio, the value of inductance in the equation above can be replaced by 2L due to mutual inductance. Doing this maintains the same total ripple current and energy storage in the inductor. Substituting 2L yields the following equation for 1:1 coupled inductors: LL V If D IN MIN L MAX 12 2 == () •• • ∆ For the case of uncoupled inductors, choose minimum saturation currents based on the peak currents outlined in APPLICATIO S I FOR ATIO |
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