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LTC3637 Datasheet(PDF) 13 Page - Linear Technology |
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LTC3637 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 26 page ![]() LTC3637 13 3637fa For more information www.linear.com/LTC3637 APPLICATIONS INFORMATION depends on the price versus size requirements and any radiated field/EMI requirements. New designs for surface mount inductors are available from Würth, Coilcraft, TDK, Toko, and Sumida. CIN and COUT Selection The input capacitor, CIN, is needed to filter the trapezoidal current at the source of the top high side MOSFET. CIN should be sized to provide the energy required to charge the inductor without causing a large decrease in input voltage ( ∆VIN). The relationship between CIN and ∆VIN is given by: CIN > L •IPEAK2 2 • VIN • ∆VIN It is recommended to use a larger value for CIN than calculated by the above equation since capacitance de- creases with applied voltage. In general, a 4.7µF X7R ceramiccapacitorisagoodchoiceforCINinmostLTC3637 applications. To minimize large ripple voltage, a low ESR input capaci- tor sized for the maximum RMS current should be used. RMS current is given by: IRMS =IOUT(MAX) • VOUT VIN • VIN VOUT – 1 This formula has a maximum at VIN = 2VOUT, where IRMS = IOUT/2.Thissimpleworst-caseconditioniscommonlyused for design because even significant deviations do not offer much relief. Note that ripple current ratings from capacitor manufacturers are often based only on 2000 hours of life which makes it advisable to further derate the capacitor, or choose a capacitor rated at a higher temperature than required.Severalcapacitorsmayalsobeparalleledtomeet size or height requirements in the design. The output capacitor, COUT, filters the inductor’s ripple current and stores energy to satisfy the load current when the LTC3637 is in sleep. The output ripple has a lower limit of VOUT/160 due to the 5mV typical hysteresis of the feed- back comparator. The time delay of the comparator adds an additional ripple voltage that is a function of the load current. During this delay time, the LTC3637 continues to switch and supply current to the output. The output ripple can be approximated by: ∆VOUT ≈ IPEAK 2 –ILOAD • 4 • 10–6 COUT + VOUT 160 The output ripple is a maximum at no load and approaches lower limit of VOUT/160 at full load. Choose the output capacitor COUT to limit the output voltage ripple ∆VOUT using the following equation: COUT ≥ IPEAK • 2 •10–6 ∆VOUT – VOUT 160 The value of the output capacitor must be large enough to accept the energy stored in the inductor without a large change in output voltage during a single switching cycle. Setting this voltage step equal to 1% of the output voltage, the output capacitor must be: COUT > 50 •L • IPEAK VOUT 2 Typically, a capacitor that satisfies the voltage ripple requirement is adequate to filter the inductor ripple. To avoid overheating, the output capacitor must also be sized to handle the ripple current generated by the inductor. The worst-case ripple current in the output capacitor is given by IRMS = IPEAK/2. Multiple capacitors placed in parallel may be needed to meet the ESR and RMS current handling requirements. Dry tantalum, special polymer, aluminum electrolytic, and ceramic capacitors are all available in surface mount packages. Special polymer capacitors offer very low ESR but have lower capacitance density than other types. Tantalum capacitors have the highest capacitance density but it is important only to use types that have been surge tested for use in switching power supplies. Aluminum electrolytic capacitors have significantly higher ESR but can be used in cost-sensitive applications provided that consideration is given to ripple current ratings and long- term reliability. Ceramic capacitors have excellent low ESR characteristics but can have high voltage coefficient and audible piezoelectric effects. The high quality factor (Q) |
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