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AIC164227XBG Datasheet(PDF) 11 Page - Analog Intergrations Corporation |
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AIC164227XBG Datasheet(HTML) 11 Page - Analog Intergrations Corporation |
11 / 14 page AIC1642 11 I PK IIN V EXT I SW IOUT V SW I D t Continuous Conduction Mode Continuous Conduction Mode At the boundary between continuous and dis- continuous mode, output current (IOB) is deter- mined by ) x 1 ( * T * L V * 2 1 * V V I ON IN OUT IN OB − = where Vd is the diode drop, L T * ) R R ( x ON S ON + = RON= Switch turn on resistance, RS= Inductor DC resistance TON = Switch ON time In the discontinuous mode, the switching fre- quency (Fsw) is Fsw = ) x (1 T V ) (I * ) V V (V * (L) * 2 2 ON 2 IN OUT IN D OUT + × − + In the continuous mode, the switching fre- quency is ( ) − + − + ≅ − + − + − + − + = SW D OUT IN D OUT ON SW D OUT SW IN SW D OUT IN D OUT ON SW V V V V V V T 1 )] V V V V V ( 2 x [1 * ) V V (V V V V T 1 f where Vsw = switch drop and proportion to out- put current. Inductor Selection To operate as an efficient energy transfer ele- ment, the inductor must fulfill three require- ments. First, the inductance must be low enough for the inductor to store adequate en- ergy under the worst case condition of minimum input voltage and switch ON time. Second, the inductance must also be high enough so maxi- mum current rating of AIC1642 and inductor are not exceed at the other worst case condition of maximum input voltage and ON time. Lastly, the inductor must have sufficiently low DC resis- tance so excessive power is not lost as heat in the windings. But unfortunately this is inversely related to physical size. Minimum and maximum input voltage, output voltage and output current must be established in advance and then inductor can be selected. In discontinuous mode operation, at the end of the switch ON time, peak current and energy in the inductor build according to + − − + = ) T * L Rs RON exp( 1 * Rs R V I ON ON IN PK ( ) − ≅ 2 x 1 * T * L V ON IN ON IN T L V ≅ (simple loss equation), where L T * ) R R ( x ON S ON + = |
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