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APW7089 Datasheet(PDF) 18 Page - Anpec Electronics Coropration |
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APW7089 Datasheet(HTML) 18 Page - Anpec Electronics Coropration |
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18 / 24 page ![]() Copyright © ANPEC Electronics Corp. Rev. A.1 - Jan., 2012 APW7089 www.anpec.com.tw 18 Application Information (Cont.) Output Capacitor Selection (Cont.) (V) C F 8 I V OUT OSC COUT ⋅ ⋅ ∆ = ∆ ........... (4) For the applications using bulk capacitors, the ∆V COUT is much smaller than the V ESR an d c an b e i g n o r e d . Therefore, the AC peak-to-peak output voltage ( ∆V OUT ) is shown as below: (V) ESR I VOUT ⋅ ∆ = ∆ ........... (5) For the applications using ceramic capacitors, the V ESR is much smaller than the ∆V COUT an d c an b e i g no r e d . Therefore, the AC peak-to-peak output voltage ( ∆V OUT ) is close to ∆V COUT . The load transient requirements are the function of the slew rate (di/dt) and the magnitude of the transient load current. These requirements are generally met with a mix of capacitors and careful layout. High frequency capacitors initially supply the transient and slow the current load rate seen by the bulk capacitors. The bulk filter capacitor values are generally determined by the ESR (Effective Series Resistance) and voltage rating require- ments rather than actual capacitance requirements. High frequency decoupling capacitors should be placed as close to the power pins of the load as physically possible. Be careful not to add inductance in the circuit board wiring that could cancel the usefulness of these low inductance components. An aluminum electrolytic capacitor’s ESR value is related to the case size with lower ESR available in larger case sizes. However, the Equiva- lent Series Inductance (ESL) of these capacitors increases with case size and can reduce the usefulness of the ca- pacitor to high slew-rate transient loading. Inductor Value Calculation The operating frequency and inductor selection are interrelated in that higher operating frequencies permit the use of a smaller inductor for the same amount of inductor ripple current. However, this is at the expense of efficiency due to an increase in MOSFET gate charge losses. The equation (2) shows that the inductance value has a direct effect on ripple current. Accepting larger values of ripple current allows the use of low inductances but results in higher output voltage ripple ........... (6) IN(MAX) IN V V = Output Diode Selection The Schottky diode carries load current during the off- time. The average diode current is therefore dependent on the P-channel power MOSFET duty cycle. At high input voltages, the diode conducts most of the time. As V IN ap- proaches V OUT, the diode conducts only a small fraction of the time. The most stressful condition for the diode is when the output is short-circuited. Therefore, it is impor- tant to adequately specify the diode peak current and av- erage power dissipation so as not to exceed the diode ratings. Under normal load conditions, the average current con- ducted by the diode is: OUT D IN OUT IN D I V V V - V I ⋅ + = The APW7089 is equipped with whole protections to re- duce the power dissipation during short-circuit condition. Therefore, the maximum power dissipation of the diode is calculated from the maximum output current as: D(MAX) D DIODE(MAX) I · V P = OUT(MAX) OUT I I = where where Remember to keep lead length short and observe proper grounding to avoid ringing and increased dissipation. and greater core losses. A reasonable starting point for setting ripple current is ∆I ≤ 0.4 ⋅ I OUT(MAX) . Remember, the maximum ripple current occurs at the maximum input voltage. The minimum inductance of the inductor is cal- culated by using the following equation: 1.6 V · L · 380000 ) V - (V · V IN OUT IN OUT ≤ (H) V · 608000 ) V - (V · V L IN OUT IN OUT ≥ |
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