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LT1376CS8 Datasheet(PDF) 13 Page - Linear Technology |
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LT1376CS8 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 28 page ![]() 13 LT1375/LT1376 APPLICATIONS INFORMATION discharge surges, such as when the regulator output is dead shorted, do not harm the capacitors. Unlike the input capacitor, RMS ripple current in the output capacitor is normally low enough that ripple cur- rent rating is not an issue. The current waveform is triangular with a typical value of 200mARMS. The formula to calculate this is: Output Capacitor Ripple Current (RMS): I VV V Lf V RIPPLE RMS OUT IN OUT IN ( ) = () − () ()( )( ) 029 . Ceramic Capacitors Higher value, lower cost ceramic capacitors are now becoming available in smaller case sizes. These are tempt- ing for switching regulator use because of their very low ESR. Unfortunately, the ESR is so low that it can cause loop stability problems. Solid tantalum capacitor’s ESR generates a loop “zero” at 5kHz to 50kHz that is instrumen- tal in giving acceptable loop phase margin. Ceramic ca- pacitors remain capacitive to beyond 300kHz and usually resonate with their ESL before ESR becomes effective. They are appropriate for input bypassing because of their high ripple current ratings and tolerance of turn-on surges. For further information on ceramic and other capacitor types please refer to Design Note 95. OUTPUT RIPPLE VOLTAGE Figure 3 shows a typical output ripple voltage waveform for the LT1376. Ripple voltage is determined by the high frequency impedance of the output capacitor, and ripple current through the inductor. Peak-to-peak ripple current through the inductor into the output capacitor is: I VV V VL f P OUT IN OUT IN -P = () − () ()( )( ) For high frequency switchers, the sum of ripple current slew rates may also be relevant and can be calculated from: Σ dI dt V L IN = Peak-to-peak output ripple voltage is the sum of a triwave created by peak-to-peak ripple current times ESR, and a square wave created by parasitic inductance (ESL) and ripple current slew rate. Capacitive reactance is assumed to be small compared to ESR or ESL. V I ESR ESL dI dt RIPPLE = ()( )+() P-P Σ Example: with VIN =10V, VOUT = 5V, L = 10µH, ESR = 0.1Ω, ESL = 10nH: IA dI dt VA mV RIPPLE P-P P-P = () − () () = == = ()( )+ =+ = − − − 510 5 10 10 10 500 10 05 10 10 10 10 05 01 10 10 10 0 05 0 01 60 63 6 6 96 •• . • .. • .. Σ VOUT AT IOUT = 1A VOUT AT IOUT = 50mA INDUCTOR CURRENT AT IOUT = 1A 0.5 µs/DIV 1375/76 F03 Figure 3. LT1376 Ripple Voltage Waveform INDUCTOR CURRENT AT IOUT = 50mA 20mV/DIV 0.5A/DIV CATCH DIODE The suggested catch diode (D1) is a 1N5818 Schottky, or its Motorola equivalent, MBR130. It is rated at 1A average forward current and 30V reverse voltage. Typical forward voltage is 0.42V at 1A. The diode conducts current only during switch off time. Peak reverse voltage is equal to |
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