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LT1956IGN データシート(PDF) 26 Page - Linear Technology |
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LT1956IGN データシート(HTML) 26 Page - Linear Technology |
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26 / 28 page ![]() 26 LT1956/LT1956-5 1956f PACKAGE DESCRIPTIO Minimum inductor continuous mode: L VV fV V I I VV V MIN IN OUT IN OUT P OUT OUT F IN = ++ + ()( ) ()( ) – () 21 For a 12V to –12V converter using the LT1956 with peak switch current of 1.5A and a catch diode of 0.63V: IA CONT > ++ + = () ( . ) ()( . ) . 12 1 5 4 1212 1212 0 63 0 370 22 For a load current of 0.25A, this says that discontinuous mode can be used and the minimum inductor needed is found from: LH MIN == µ 212 0 25 500 10 1 5 53 32 ()( . ) (• )( . ) . In practice, the inductor should be increased by about 30% over the calculated minimum to handle losses and variations in value. This suggests a minimum inductor of 7 µH for this application. Ripple Current in the Input and Output Capacitors Positive-to-negative converters have high ripple current in the input capacitor. For long capacitor lifetime, the RMS value of this current must be less than the high frequency ripple current rating of the capacitor. The following formula will give an approximate value for RMS ripple current. This formula assumes continuous mode and large inductor value. Small inductors will give some- what higher ripple current, especially in discontinuous mode. The exact formulas are very complex and appear in Application Note 44, pages 29 and 30. For our pur- poses here I have simply added a fudge factor (ff). The value for ff is about 1.2 for higher load currents and L ≥15µH. It increases to about 2.0 for smaller inductors at lower load currents. Capacitor I ff I V V RMS OUT OUT IN = ()( ) ff = 1.2 to 2.0 The output capacitor ripple current for the positive-to- negative converter is similar to that for a typical buck regulator—it is a triangular waveform with peak-to-peak value equal to the peak-to-peak triangular waveform of the inductor. The low output ripple design in Figure 14 places the input capacitor between VIN and the regulated negative output. This placement of the input capacitor significantly reduces the size required for the output capacitor (versus placing the input capacitor between VIN and ground). The peak-to-peak ripple current in both the inductor and output capacitor (assuming continuous mode) is: IP-P P-P = == + ++ = DC V fL DC Duty Cycle VV VV V I RMS I IN OUT F OUT IN F COUT • • () 12 The output ripple voltage for this configuration is as low as the typical buck regulator based predominantly on the inductor’s triangular peak-to-peak ripple current and the ESR of the chosen capacitor (see Output Ripple Voltage in Applications Information). Diode Current Average diode current is equal to load current. Peak diode current will be considerably higher. Peak diode current: Continuous Mode I VV V VV Lf V V Discontinuous Mode IV Lf OUT IN OUT IN IN OUT IN OUT OUT OUT = + + + = () ( )( ) ()( )( ) ()( ) ()( ) 2 2 Keep in mind that during start-up and output overloads, average diode current may be much higher than with normal loads. Care should be used if diodes rated less than 1A are used, especially if continuous overload conditions must be tolerated. |
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