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3513 数据表(PDF) 13 Page - Linear Technology |
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3513 数据表(HTML) 13 Page - Linear Technology |
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13 / 20 page ![]() LT3513 13 3513fa INDUCTOR SELECTION AND MAXIMUM OUTPUT CURRENT A good first choice for the inductor value is: L VV OUT F = + 1 8 . where VFisthevoltagedropofthecatchdiode(~0.4V)andL is in μH. The inductor’s RMS current rating must be greater than the maximum load current and its saturation current should be at least 30% higher. For highest efficiency, the series resistance (DCR) should be less than 0.1 Ω. Table 1 lists several vendors and types that are suitable. Table 1. Inductor Vendors VENDOR URL PART SERIES TYPE Coilcraft www.coilcraft.com MSS7341 Shielded Murata www.murata.com LQH55D Open TDK www.component.tdk.com SLF7045 SLF10145 Shielded Shielded Toko www.toko.com DC62CB D63CB D75C D75F Shielded Shielded Shielded Open Sumida www.sumida.com CR54 CDRH74 CDRH6D38 CR75 Open Shielded Shielded Open The optimum inductor for a given application may differ from the one indicated by this simple design guide. A larger value inductor provides a higher maximum load current, and reduces the output voltage ripple. If your load is lower than the maximum load current, then you can relax the value of the inductor and operate with higher ripple cur- rent. This allows you to use a physically smaller inductor or one with a lower DCR resulting in higher efficiency. Be aware that the maximum load current depends on input voltage. A graph in the Typical Performance Character- istics section of this data sheet shows the maximum load current as a function of input voltage and inductor value for VOUT = 3.3V. In addition, low inductance may result in discontinuous mode operation, which further reduces maximum load current. For details of maximum output current and discontinuous mode operation, see Linear Technology’s Application Note 44. Finally, for duty cycles greater than 50% (VOUT/VIN > 0.5), a minimum inductance is required to avoid subharmonic oscillations, see Application Note 19. The current in the inductor is a triangle wave with an average value equal to the load current. The peak switch current is equal to the output current plus half the peak-to-peak inductor ripple current. The LT3513 limits its switch cur- rent in order to protect itself and the system from overload faults. Therefore, the maximum output current that the LT3513 will deliver depends on the switch current limit, the inductor value, and the input and output voltages. When the switch is off, the potential across the inductor is the output voltage plus the catch diode drop. This gives the peak-to-peak ripple current in the inductor: ΔI DC V V Lf L OUT F = () + () 1– • where f is the switching frequency of the LT3513 and L is the value of the inductor. The peak inductor and switch current is: II I I SW PK LPK OUT L () == + Δ 2 To maintain output regulation, this peak current must be less than the LT3513’s switch current limit of ILIM. For SW1, ILIM is at least 2A at DC = 0.35, and decreases linearly to 1.5A at DC = 0.75 as shown in the Typical Performance Characteristics section. The maximum output current is a function of the chosen inductor value: II I ADC I OUT MAX LIM LL () –. • – . • – == () ΔΔ 2 25 1 0 57 2 Choosing an inductor value so that the ripple current is small will allow a maximum output current near the switch current limit. One approach to choosing the inductor is to start with the simple rule given above, look at the available inductors and choose one to meet cost or space goals. Then use these equations to check that the LT3513 will be able to deliver the required output current. Note again that these equations assume that the inductor current is continuous. Discontinuous operation occurs when IOUT is less than ΔIL/2. OPERATION |
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