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PM6675 bảng dữ liệu(PDF) 34 Page - STMicroelectronics |
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PM6675 bảng dữ liệu(HTML) 34 Page - STMicroelectronics |
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34 / 47 page ![]() Obsolete Product(s) - Obsolete Product(s) Obsolete Product(s) - Obsolete Product(s) Application information PM6675 34/47 7.1.1 Inductor selection Once the switching frequency has been defined, the inductance value depends on the desired inductor ripple current. Low inductance value means great ripple current that brings poor efficiency and great output noise. On the other hand a great current ripple is desirable for fast transient response when a load step is applied. High inductance brings to good efficiency but the transient response is critical, especially if VINmin - VOUT is little. Moreover a minimum output ripple voltage is necessary to assure system stability and jitter-free operations (see Section 7.1.3: Output capacitor selection on page 36 ). The product of the output capacitor's ESR multiplied by the inductor ripple current must be taken in consideration. A good trade-off between the transient response time, the efficiency, the cost and the size is choosing the inductance value in order to maintain the inductor ripple current between 20% and 50% (usually 40%) of the maximum output current. The maximum inductor ripple current, ∆I L,MAX , occurs at the maximum input voltage. Given these considerations, the inductance value can be calculated using the following expression: Equation 30 where fSW is the switching frequency, VIN is the input voltage, VOUT is the output voltage and ∆I L is the inductor ripple current. Once the inductor value is determined, the inductor ripple current is then recalculated: Equation 31 The next step is the calculation of the maximum r.m.s. inductor current: Equation 32 The inductor must have an r.m.s. current greater than IL,RMS in order to assure thermal stability. Then the calculation of the maximum inductor peak current follows: Equation 33 IL,PEAK is important when choosing the inductor, in term of its saturation current. IN OUT L OUT IN V V I fsw V V L ⋅ ∆ ⋅ − = MAX , IN OUT OUT MAX , IN MAX , L V V L fsw V V I ⋅ ⋅ − = ∆ 12 ) I ( ) I ( I 2 MAX , L 2 MAX , LOAD RMS , L ∆ + = 2 I I I MAX , L MAX , LOAD PEAK , L ∆ + = |
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