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SLVSAC4 Datenblatt(PDF) 12 Page - Texas Instruments |
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SLVSAC4 Datenblatt(HTML) 12 Page - Texas Instruments |
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12 / 27 page ![]() L L max out max I I I 2 D = + L Vout 1 Vin I Vout L ƒ - D = ´ ´ c 1 = = 50kHz 2 (1 H 10 F) f p ´ ´ ´ TLV62065 SLVSAC4B – NOVEMBER 2010 – REVISED DECEMBER 2015 www.ti.com Typical Application (continued) 8.2.2.2 Output Filter Design (Inductor and Output Capacitor) The internal compensation network of TLV62065 is optimized for a LC output filter with a corner frequency of: The device operates with nominal inductors of 1.0 µH to 1.2 µH and with 10 µF to 22 µF small X5R and X7R ceramic capacitors. Please refer to the lists of inductors and capacitors. The device is optimized for a 1-µH inductor and 10-µF output capacitor. 8.2.2.2.1 Inductor Selection The inductor value has a direct effect on the ripple current. The selected inductor has to be rated for its DC resistance and saturation current. The inductor ripple current ( ΔIL) decreases with higher inductance and increases with higher VI or VO. Equation 5 calculates the maximum inductor current in PWM mode under static load conditions. The saturation current of the inductor should be rated higher than the maximum inductor current as calculated with Equation 6. This is recommended because during heavy load transient the inductor current rises above the calculated value. (5) where • f = Switching frequency (3 MHz typical) • L = Inductor value • ΔIL = Peak-to-peak inductor ripple current • ILmax = Maximum inductor current (6) A more conservative approach is to select the inductor current rating just for the switch current limit ILIMF of the converter. The total losses of the coil have a strong impact on the efficiency of the DC–DC conversion and consist of both the losses in the DC resistance R(DC) and the following frequency-dependent components: • The losses in the core material (magnetic hysteresis loss, especially at high switching frequencies) • Additional losses in the conductor from the skin effect (current displacement at high frequencies) • Magnetic field losses of the neighboring windings (proximity effect) • Radiation losses Table 1. List of Inductors DIMENSIONS [mm3] INDUCTANCE μH INDUCTOR TYPE SUPPLIER 3.2 x 2.5 x 1.0 max 1.0 LQM32PN (MLCC) Murata 3.7 x 4 x 1.8 max 1.0 LQH44 (wire wound) Murata 4.0 x 4.0 x 2.6 max 1.2 NRG4026T (wire wound) Taiyo Yuden 3.5 x 3.7 x 1.8 max 1.2 DE3518 (wire wound) TOKO 12 Submit Documentation Feedback Copyright © 2010–2015, Texas Instruments Incorporated Product Folder Links: TLV62065 |
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