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LTC4002 Datasheet(PDF) 17 Page - Linear Technology |
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LTC4002 Datasheet(HTML) 17 Page - Linear Technology |
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17 / 24 page ![]() 17 LTC3783 3783f Boost Converter: Output Diode Selection To maximize efficiency, a fast switching diode with low forward drop and low reverse leakage is desired. The output diode in a boost converter conducts current during the switch off-time. The peak reverse voltage that the diode must withstand is equal to the regulator output voltage. The average forward current in normal operation is equal to the output current, and the peak current is equal to the peak inductor current. II I D D PEAK L PEAK OUT MAX MA () () () • – == + ⎛ ⎝⎜ ⎞ ⎠⎟ 1 21 χ X X The power dissipated by the diode is: PD = IOUT(MAX) • VD and the diode junction temperature is: TJ = TA + PD • θJA The θJA to be used in this equation normally includes the θJC for the device plus the thermal resistance from the board to the ambient temperature in the enclosure. Remember to keep the diode lead lengths short and to observe proper switch-node layout (see Board Layout Checklist) to avoid excessive ringing and increased dissipation. Boost Converter: Output Capacitor Selection Contributions of ESR (equivalent series resistance), ESL (equivalent series inductance) and the bulk capacitance must be considered when choosing the correct compo- nent for a given output ripple voltage. The effects of these three parameters (ESR, ESL and bulk C) on the output voltage ripple waveform are illustrated in Figure 9 for a typical boost converter. The choice of component(s) begins with the maximum acceptable ripple voltage (expressed as a percentage of the output voltage), and how this ripple should be divided between the ESR step and the charging/discharging ∆V. For the purpose of simplicity we will choose 2% for the maximum output ripple, to be divided equally between the ESR step and the charging/discharging ∆V. This percent- age ripple will change, depending on the requirements of the application, and the equations provided below can easily be modified. For a 1% contribution to the total ripple voltage, the ESR of the output capacitor can be determined using the following equation: ESR V I where I COUT OUT IN PEAK IN PEAK < = 001 1 .• : () () ++ ⎛ ⎝⎜ ⎞ ⎠⎟ χ 21 • – () I D OUT MAX MAX For the bulk C component, which also contributes 1% to the total ripple: C I Vf OUT OUT MAX OUT > () .• • 001 For many designs it is possible to choose a single capaci- tor type that satisfies both the ESR and bulk C require- ments for the design. In certain demanding applications, however, the ripple voltage can be improved significantly by connecting two or more types of capacitors in parallel. For example, using a low ESR ceramic capacitor can minimize the ESR setup, while an electrolytic capacitor can be used to supply the required bulk C. Once the output capacitor ESR and bulk capacitance have been determined, the overall ripple voltage waveform should be verified on a dedicated PC board (see Board OPERATIO VOUT (AC) ∆VESR RINGING DUE TO TOTAL INDUCTANCE (BOARD + CAP) ∆VCOUT 3783 F09 Figure 9. Output Ripple Voltage |
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