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MIC2159 Datasheet(PDF) 10 Page - Micrel Semiconductor |
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MIC2159 Datasheet(HTML) 10 Page - Micrel Semiconductor |
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10 / 17 page ![]() Micrel MIC2159 October 2006 10 M9999-101206 inductance values are used with higher input voltages. Larger peak-to-peak ripple currents will increase the power dissipation in the inductor and MOSFETs. Larger output ripple currents will also require more output capacitance to smooth out the larger ripple current. Smaller peak-to-peak ripple currents require a larger inductance value and therefore a larger and more expensive inductor. A good compromise between size, loss and cost is to set the inductor ripple current to be equal to 20% of the maximum output current. The inductance value is calculated by the equation below. ( ) (max) (max) (max) 2 . 0 OUT S IN OUT IN OUT I F V V V V L ⋅ ⋅ ⋅ − ⋅ = where: FS = switching frequency, 400 kHz 0.2 = ratio of AC ripple current to DC output current VIN(max) = maximum input voltage The peak-to-peak inductor current (AC ripple current) is: L F V V V V I S IN OUT IN OUT PP . . ) .( (max) (max) − = The peak inductor current is equal to the average output current plus one half of the peak-to-peak inductor ripple current. IPK = IOUT(max)+0.5 x IPP The RMS inductor current is used to calculate the I2R losses in the inductor. 2 (max) (max) 3 1 1 ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ ⋅ + ⋅ = OUT PK OUT INDUCTOR I I I I Maximizing efficiency requires the proper selection of core material and minimizing the winding resistance. The high frequency operation of the MIC2159 requires the use of ferrite materials for all but the most cost sensitive applications. Lower cost iron powder cores may be used but the increase in core loss will reduce the efficiency of the power supply. This is especially noticeable at low output power. The winding resistance decreases efficiency at the higher output current levels. The winding resistance must be minimized although this usually comes at the expense of a larger inductor. The power dissipated in the inductor is equal to the sum of the core and copper losses. At higher output loads, the core losses are usually insignificant and can be ignored. At lower output currents, the core losses can be a significant contributor. Core loss information is usually available from the magnetics vendor. Copper loss in the inductor is calculated by the equation below: WINDING rms INDUCTOR INDUCTOR R I P Cu . 2 ) ( = The resistance of the copper wire, RWINDING, increases with temperature. The value of the winding resistance used should be at the operating temperature. ( ) ( ) C HOT C WINDING hot WINDING o o T T R R 20 ) 20 ( ) ( 0042 . 0 1 − ⋅ + ⋅ = Where: THOT = temperature of wire under full load T20 o C = ambient temperature RWINDING(20oC) = room temperature winding resistance (usually specified by manufacturer) Output Capacitor Selection The output capacitor values are usually determined by the capacitors ESR (equivalent series resistance). Voltage and RMS current capability are two other important factors for selecting the output capacitor. Recommended capacitors are tantalum, low-ESR aluminium electrolytic, and POSCAPS. The output capacitor’s ESR is usually the main cause of output ripple. The output capacitor ESR also affects the overall voltage feedback loop from a stability point of view. See “Feedback Loop Compensation” section for more information. The maximum value of ESR is calculated: PP OUT ESR I V R ∆ ≤ Where: VOUT = peak-to-peak output voltage ripple IPP = peak-to-peak inductor ripple current The total output ripple is a combination of the ESR and output capacitance. The total ripple is calculated below: ()2 2 ) 1 ( ESR PP S OUT PP OUT R I F C D I V ⋅ + ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ ⋅ − ⋅ = ∆ Where: D = duty cycle COUT = output capacitance value fS = switching frequency The voltage rating of the capacitor should be twice the voltage for a tantalum and 20% greater for aluminium electrolytic. The output capacitor RMS current is calculated below: 12 ) ( PP C I I rms OUT = The power dissipated in the output capacitor is: ) ( 2 ) ( ) ( OUT OUT C ESR rms OUT C C DISS R I P ⋅ = |
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