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MIC2199 Datasheet(PDF) 11 Page - Micrel Semiconductor |
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MIC2199 Datasheet(HTML) 11 Page - Micrel Semiconductor |
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11 / 15 page ![]() November 2004 11 MIC2199 MIC2199 Micrel reduction in efficiency. The average current required to drive the high-side MOSFET is: IQ f G[high-side](avg) G S =× where: I G[high-side](avg) = average high-side MOSFET gate current Q G = total gate charge for the high-side MOSFET taken from manufacturer’s data sheet with V GS = 5V. f s = 300kHz The low-side MOSFET is turned on and off at V DS = 0 because the freewheeling diode is conducting during this time. The switching losses for the low-side MOSFET is usually negligible. Also, the gate drive current for the low-side MOSFET is more accurately calculated using C ISS at VDS = 0 instead of gate charge. For the low-side MOSFET: IC V f G[low-side](avg) ISS GS S =× × Since the current from the gate drive comes from the input voltage, the power dissipated in the MIC2199 due to gate drive is: PV I I GATEDRIVE IN G[high-side](avg) G[low-side](avg) =+ () A convenient figure of merit for switching MOSFETs is the on- resistance times the total gate charge (R DS(on) × QG). Lower numbers translate into higher efficiency. Low gate-charge logic-level MOSFETs are a good choice for use with the MIC2199. Power dissipation in the MIC2199 package limits the maximum gate drive current. Parameters that are important to MOSFET switch selection are: • Voltage rating • On-resistance • Total gate charge The voltage rating of the MOSFETs are essentially equal to the input voltage. A safety factor of 20% should be added to the V DS(max) of the MOSFETs to account for voltage spikes due to circuit parasitics. The power dissipated in the switching transistor is the sum of the conduction losses during the on-time (P CONDUCTION) and the switching losses that occur during the period of time when the MOSFETs turn on and off (P AC). PP P SW CONDUCTION AC =+ where: PI R CONDUCTION SW(rms) SW 2 =× PP P AC AC(off) AC(on) =+ R SW = on-resistance of the MOSFET switch. Making the assumption the turn-on and turnoff transition times are equal, the transition time can be approximated by: t CV C V I T ISS GS OSS IN G = ×+ × where: C ISS and COSS are measured at VDS = 0. I G = gate drive current (1A for the MIC2199) The total high-side MOSFET switching loss is: P(V V ) I t f AC IN D PK T S =+ × × × where: t T = switching transition time (typically 20ns to 50ns) V D = freewheeling diode drop, typically 0.5V. f S it the switching frequency, nominally 300kHz The low-side MOSFET switching losses are negligible and can be ignored for these calculations. RMS Current and MOSFET Power Dissipation Calculation Under normal operation, the high-side MOSFETs RMS cur- rent is greatest when V IN is low (maximum duty cycle). The low-side MOSFETs RMS current is greatest when V IN is high (minimum duty cycle). However, the maximum stress the MOSFETs see occurs during short circuit conditions, where the output current is equal to I OVERCURRENT(max). (See the “Sense Resistor” section). The calculations below are for normal operation. To calculate the stress under short circuit conditions, substitute I OVERCURRENT(max) for IOUT(max). Use the formula below to calculate D under short circuit condi- tions. D 0.063 1.8 10 V SHORTCIRCUIT 3 IN = − ×× − The RMS value of the high-side switch current is: ID I I 12 SW(high side)(rms) OUT(max) 2 PP 2 − =× + ⎛ ⎝ ⎜ ⎞ ⎠ ⎟ I1 D I I 12 SW(low side)(rms) OUT(max) 2 PP 2 − = − () + ⎛ ⎝ ⎜ ⎞ ⎠ ⎟ where: D = duty cycle of the converter D V V OUT IN = × η η = efficiency of the converter. Converter efficiency depends on component parameters, which have not yet been selected. For design purposes, an efficiency of 90% can be used for V IN less than 10V and 85% can be used for V IN greater than 10V. The efficiency can be more accurately calculated once the design is complete. If the assumed efficiency is grossly inaccurate, a second iteration through the design procedure can be made. |
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