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TPS61253 Datasheet(PDF) 19 Page - Texas Instruments |
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TPS61253 Datasheet(HTML) 19 Page - Texas Instruments |
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19 / 35 page ![]() ( ) OUT OUT IN MIN OUT I V V C f V V - = D g g g h g g OUT L(DC) OUT IN V 1 I = I V OUT IN IN L(PEAK) OUT I V D V I = + with D 1 2 f L (1 D) V h = - - h g g g g g 19 TPS61253, TPS61254, TPS61256, TPS61258, TPS61259, TPS612592 www.ti.com SLVSAG8F – SEPTEMBER 2011 – REVISED MARCH 2016 Product Folder Links: TPS61253 TPS61254 TPS61256 TPS61258 TPS61259 TPS612592 Submit Documentation Feedback Copyright © 2011–2016, Texas Instruments Incorporated (4) Selecting an inductor with insufficient saturation performance can lead to excessive peak current in the converter. This could eventually harm the device and reduce its reliability. When selecting the inductor, as well as the inductance, parameters of importance are: maximum current rating, series resistance, and operating temperature. The inductor DC current rating should be greater (by some margin) than the maximum input average current, refer to Equation 5 and Current Limit Operation section for more details. (5) The TPS6125x series of step-up converters have been optimized to operate with a effective inductance in the range of 0.7 µH to 2.9 µH and with output capacitors in the range of 10 µF to 47 µF. The internal compensation is optimized for an output filter of L = 1 µH and CO = 10 µF. Larger or smaller inductor values can be used to optimize the performance of the device for specific operating conditions. For more details, see the Checking Loop Stability section. In high-frequency converter applications, the efficiency is essentially affected by the inductor AC resistance (i.e. quality factor) and to a smaller extent by the inductor DCR value. To achieve high efficiency operation, care should be taken in selecting inductors featuring a quality factor above 25 at the switching frequency. Increasing the inductor value produces lower RMS currents, but degrades transient response. For a given physical inductor size, increased inductance usually results in an inductor with lower saturation current. The total losses of the coil 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 The following inductor series from different suppliers have been used with the TPS6125x converters. (1) See Third-Party Products Disclaimer Table 4. List of Inductors MANUFACTURER(1) SERIES DIMENSIONS (in mm) HITACHI METALS KSLI-322512BL1-1R0 3.2 x 2.5 x 1.2 max. height MURATA LQM32PN1R0MG0 3.2 x 2.5 x 1.0 max. height LQM2HPN1R0MG0 2.5 x 2.0 x 1.0 max. height LQM21PN1R5MC0 2.0 x 1.2 x 0.55 max height TOKO DFE322512C-1R0 3.2 x 2.5 x 1.2 max. height MDT2012-CLR1R0AM 2.0 x 1.2 x 0.58 max height 10.2.2.2 Output Capacitor For the output capacitor, it is recommended to use small ceramic capacitors placed as close as possible to the VOUT and GND pins of the IC. If, for any reason, the application requires the use of large capacitors which can not be placed close to the IC, using a smaller ceramic capacitor in parallel to the large one is highly recommended. This small capacitor should be placed as close as possible to the VOUT and GND pins of the IC. To get an estimate of the recommended minimum output capacitance, Equation 6 can be used. (6) Where f is the switching frequency which is 3.5 MHz (typ.) and ΔV is the maximum allowed output ripple. |
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