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LT8607 датащи(PDF) 14 Page - Analog Devices |
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LT8607 датащи(HTML) 14 Page - Analog Devices |
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14 / 24 page ![]() LT8609S 14 Rev. D For more information www.analog.com APPLICATIONS INFORMATION Inductor Selection and Maximum Output Current The LT8609S is designed to minimize solution size by allowing the inductor to be chosen based on the output load requirements of the application. During overload or short circuit conditions the LT8609S safely tolerates oper- ation with a saturated inductor through the use of a high speed peak-current mode architecture. A good first choice for the inductor value is: L = VOUT +VSW(BOT) fSW where fSW is the switching frequency in MHz, VOUT is the output voltage, VSW(BOT) is the bottom switch drop (~0.25V) and L is the inductor value in μH. To avoid overheating and poor efficiency, an inductor must be chosen with an RMS current rating that is greater than the maximum expected output load of the applica- tion. In addition, the saturation current (typically labeled ISAT) rating of the inductor must be higher than the load current plus 1/2 of in inductor ripple current: IL(PEAK) =ILOAD(MAX)+ 1 2 ΔL where ∆IL is the inductor ripple current as calculated sev- eral paragraphs below and ILOAD(MAX) is the maximum output load for a given application. As a quick example, an application requiring 1A output should use an inductor with an RMS rating of greater than 1A and an ISAT of greater than 1.3A. To keep the efficiency high, the series resistance (DCR) should be less than 0.04Ω, and the core material should be intended for high frequency applications. The LT8609S limits the peak switch current in order to protect the switches and the system from overload faults. The top switch current limit (ILIM) is typically 4.75A at low duty cycles and decreases linearly to 4.0A at D = 0.8. The inductor value must then be sufficient to supply the desired maximum output current (IOUT(MAX)), which is a function of the switch current limit (ILIM) and the ripple current: IOUT(MAX) =ILIM – ΔIL 2 The peak-to-peak ripple current in the inductor can be calculated as follows: ΔIL = VOUT L • fSW 1– VOUT VIN(MAX) ⎛ ⎝ ⎜⎜ ⎞ ⎠ ⎟⎟ where fSW is the switching frequency of the LT8609S, and L is the value of the inductor. Therefore, the maximum out- put current that the LT8609S will deliver depends on the minimum switch current limit, the inductor value, and the input and output voltages. The inductor value may have to be increased if the inductor ripple current does not allow sufficient maximum output current (IOUT(MAX)) given the switching frequency, and maximum input voltage used in the desired application. The optimum inductor for a given application may differ from the one indicated by this design guide. A larger value inductor provides a higher maximum load current and reduces the output voltage ripple. For applications requir- ing smaller load currents, the value of the inductor may be lower and the LT8609S may operate with higher ripple current. This allows use of a physically smaller inductor, or one with a lower DCR resulting in higher efficiency. Be aware that low inductance may result in discontinuous mode operation, which further reduces maximum load current. The internal circuitry of the LT8609S is capable of sup- plying IOUT(MAX) up to 3A. Thermal limitations of the LT8609S prevent continuous output of 3A loads due to unsafe operating temperatures. In order to ensure safe operating temperature, the average LT8609S current must be kept below 2A, but will allow transient peaks up to 3A or IOUT(MAX). If high average currents cause unsafe heating of the part, the LT8609S will stop switching and indicate a fault condition to protect the internal circuitry. For more information about maximum output current and discontinuous operation, see Analog Devices Application Note 44. Finally, for duty cycles greater than 50% (VOUT/VIN > 0.5), a minimum inductance is required to avoid sub-harmonic oscillation. See Analog Devices Application Note 19. |
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