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AN3027 数据表(PDF) 9 Page - STMicroelectronics |
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AN3027 数据表(HTML) 9 Page - STMicroelectronics |
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9 / 41 page ![]() AN3027 Designing a TM PFC Doc ID 16134 Rev 4 9/41 3.2 Operating conditions The first step is to define the main parameters of the circuit, using the specifications given in Section 3.1. ● Rated DC output current: Equation 1 ● Maximum input power: Equation 2 ● RMS input current: Equation 3 ● Peak inductor current: Equation 4 As shown in Figure 3, the inductor current is a triangle shape at the switching frequency, and the peak of the triangle is twice its average value. The average value of the inductor current is exactly the peak of the input sine wave current, and therefore it can be easily calculated as its RMS value can be obtained from Equation 3. In order to provide a complete inductor specification for the inductor manufacturer, we must also provide the RMS and the AC current that can be calculated using Equation 5 and Equation 6. ● RMS inductor current: Equation 5 ● AC inductor current: Equation 6 The current flowing in the inductor can be split in two parts, depending on the conduction instant. During the on-time, the current increases from zero up the peak value and circulates into the switch, while during the following off-time the current decreases from its peak down to zero and circulates into the diode. Therefore these two components have a current with a triangular wave, with the same peak value equal to that of the inductor. Thus, it is also possible to calculate the RMS current flowing into the switch and into the diode, needed to calculate the losses of these two elements. out out out V P I = A 25 . 0 V 400 W 100 I out = = η = out in P P W 38 . 106 100 94 W 100 Pin = ⋅ = PF VAC P I min in in ⋅ = A 19 . 1 99 . 0 Vac 90 W 38 . 106 Iin = ⋅ = in pk I 2 2 IL ⋅ ⋅ = A 38 . 3 A 19 . 1 2 2 IL pk = ⋅ ⋅ = in rms I 3 2 IL ⋅ = A 38 . 1 A 19 . 1 3 2 IL rms = ⋅ = 2 in 2 rms ac I IL IL − = () ( ) A 69 . 0 A 19 . 1 38 . 1 IL 2 2 ac = − = |
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