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SS6638G Datasheet(PDF) 16 Page - Silicon Standard Corp. |
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SS6638G Datasheet(HTML) 16 Page - Silicon Standard Corp. |
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16 / 19 page ![]() www.SiliconStandard.com 16 of 19 IPK I IN VEXT ISW IOUT VSW ID t IV ( ) )] V V V V V ( 2 x [1 ) V V (V V V V T 1 fsw SW D OUT SW IN SW D OUT IN D OUT ON − + − + × − + − + = − + − + ≅ SW D OUT IN D OUT ON V V V V V V T 1 where Vsw = switch drop and is proportional to output current. INDUCTOR SELECTION To operate as an efficient energy transfer element, the inductor must fulfill three requirements. First, the inductance must be low enough for the inductor to store adequate energy under the worst-case condition of minimum input voltage and switch ON time. Second, the inductance must also be high enough so the maximum current rating of the SS6638 and inductor are not exceeded at the other worst-case condition of maximum input voltage and ON time. Lastly, the inductor must have sufficiently low DC resistance so excessive power is not lost as heat in the windings. Unfortunately this is inversely related to physical size. Continuous Conduction Mode At the boundary between continuous and discontinuous mode, output current (IOB) is determined by () x 1 T L V 2 1 V V V I ON IN D OUT IN OB − + = where VD is the diode drop, Minimum and maximum input voltage, output voltage and output current must be established before an inductor can be selected. x = (RON+Rs)Ton/L. RON= Switch turn on resistance, Rs= Inductor DC resistance In discontinuous mode operation, at the end of the switch ON time, peak current and energy in the inductor build according to TON = Switch ON time In the discontinuous mode, the switching frequency (Fsw) is + − − + = Ton) L Rs Ron exp( 1 Rs Ron Vin IPK ) x (1 2 T 2 V ) )(I V V 2(L)(V Fsw ON IN OUT IN D OUT + × − + = () − ≅ 2 x 1 T L V ON IN In the continuous mode, the switching frequency is ON IN T L V ≅ (Simple losses equation), where x=(RON+RS)TON/L SS6638G 8/21/2005 Rev.2.3 |
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