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TPS61240DRVT Datasheet(PDF) 13 Page - Texas Instruments |
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TPS61240DRVT Datasheet(HTML) 13 Page - Texas Instruments |
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13 / 35 page ![]() OUT OUT IN IN L(peak) OUT I V V V D I = + with D = 2 f L (1 D) η V - ´ ´ ´ - ´ ( ) ´ - » D ´ ´ IN OUT IN MIN L OUT V V V L I f V » ´ ´ OUT L_MAX OUT IN V I I η V TPS61240, TPS61241 www.ti.com SLVS806D – APRIL 2009 – REVISED DECEMBER 2015 10.2.2.1 Programming the Output Voltage The output voltage is set by a resistor divider internally. The FB pin is used to sense the output voltage. So to configure the output properly, the FB pin needs to be connected directly to the output. 10.2.2.2 Inductor Selection To make sure that the TPS6124x devices can operate, an inductor must be connected between pin VIN and pin L. A boost converter normally requires two main passive components for storing energy during the conversion. A boost inductor and a storage capacitor at the output are required. To select the boost inductor, it is recommended to keep the possible peak inductor current below the current limit threshold of the power switch in the chosen configuration. The highest peak current through the inductor and the switch depends on the output load, the input (VIN), and the output voltage (VOUT). Estimation of the maximum average inductor current can be done using Equation 2. (2) For example, for an output current of 200 mA at 5.0 V VOUT, at least 540 mA of average current flows through the inductor at a minimum input voltage of 2.3 V. The second parameter for choosing the inductor is the desired current ripple in the inductor. Normally, it is advisable to work with a ripple of less than 20% of the average inductor current. A smaller ripple reduces the magnetic hysteresis losses in the inductor, as well as output voltage ripple and EMI. But in the same way, regulation time at load changes rises. In addition, a larger inductor increases the total system size and cost. With these parameters, it is possible to calculate the value of the minimum inductance by using Equation 3. (3) Parameter f is the switching frequency and ΔIL is the ripple current in the inductor, i.e., 20% x IL. In this example, the desired inductor has the value of 1.7 μH. With this calculated value and the calculated currents, it is possible to choose a suitable inductor. In typical applications a 1.0- μH inductance is recommended. The device has been optimized to operate with inductance values between 1.0 μH and 2.2 μH. It is recommended that inductance values of at least 1.0 μH is used, even if Equation 3 yields something lower. Care has to be taken that load transients and losses in the circuit can lead to higher currents as estimated in Equation 3. Also, the losses in the inductor caused by magnetic hysteresis losses and copper losses are a major parameter for total circuit efficiency. With the chosen inductance value, the peak current for the inductor in steady state operation can be calculated. Equation 4 shows how to calculate the peak current I. (4) This would be the critical value for the current rating for selecting the inductor. It also needs to be taken into account that load transients and error conditions may cause higher inductor currents. Table 3. List of Inductors MANUFACTURER SERIES DIMENSIONS MDT2012-CH1R0AN 2.0 x 1.2 x 1.0 max. height TOKO MDT1608-CH1R0N 1.6 x 0.8 x 0.95 max. height KSLI-201210AG-1R0 2.0 x 1.2 x 1.0 max. height Hitachi Metals KSLI-201610AG-1R0 2.0 x 1.6 x 1.0 max. height muRata LQM21PN1R0MC0 2.0 x 1.2 x 0.55 max. height FDK MIPS2012D1R0-X2 2.0 x 1.2 x 1.0 max. height Copyright © 2009–2015, Texas Instruments Incorporated Submit Documentation Feedback 13 Product Folder Links: TPS61240 TPS61241 |
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