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LM5111-1M Datasheet(PDF) 9 Page - Texas Instruments |
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LM5111-1M Datasheet(HTML) 9 Page - Texas Instruments |
9 / 19 page VHIGH Q2 VGATE RG Q1 VTRIG CIN LM5111 www.ti.com SNVS300F – JULY 2004 – REVISED MAY 2011 Thermal Performance INTRODUCTION The primary goal of thermal management is to maintain the integrated circuit (IC) junction temperature (TJ) below a specified maximum operating temperature to ensure reliability. It is essential to estimate the maximum TJ of IC components in worst case operating conditions. The junction temperature is estimated based on the power dissipated in the IC and the junction to ambient thermal resistance θJA for the IC package in the application board and environment. The θJA is not a given constant for the package and depends on the printed circuit board design and the operating environment. DRIVE POWER REQUIREMENT CALCULATIONS IN LM5111 The LM5111 dual low side MOSFET driver is capable of sourcing/sinking 3A/5A peak currents for short intervals to drive a MOSFET without exceeding package power dissipation limits. High peak currents are required to switch the MOSFET gate very quickly for operation at high frequencies. The schematic above shows a conceptual diagram of the LM5111 output and MOSFET load. Q1 and Q2 are the switches within the gate driver. RG is the gate resistance of the external MOSFET, and CIN is the equivalent gate capacitance of the MOSFET. The gate resistance Rg is usually very small and losses in it can be neglected. The equivalent gate capacitance is a difficult parameter to measure since it is the combination of CGS (gate to source capacitance) and CGD (gate to drain capacitance). Both of these MOSFET capacitances are not constants and vary with the gate and drain voltage. The better way of quantifying gate capacitance is the total gate charge QG in coloumbs. QG combines the charge required by CGS and CGD for a given gate drive voltage VGATE. Assuming negligible gate resistance, the total power dissipated in the MOSFET driver due to gate charge is approximated by PDRIVER = VGATE x QG x FSW where • FSW = switching frequency of the MOSFET (1) For example, consider the MOSFET MTD6N15 whose gate charge specified as 30 nC for VGATE = 12V. The power dissipation in the driver due to charging and discharging of MOSFET gate capacitances at switching frequency of 300 kHz and VGATE of 12V is equal to PDRIVER = 12V x 30 nC x 300 kHz = 0.108W. (2) If both channels of the LM5111 are operating at equal frequency with equivalent loads, the total losses will be twice as this value which is 0.216W. In addition to the above gate charge power dissipation, - transient power is dissipated in the driver during output transitions. When either output of the LM5111 changes state, current will flow from VCC to VEE for a very brief interval of time through the output totem-pole N and P channel MOSFETs. The final component of power dissipation in the driver is the power associated with the quiescent bias current consumed by the driver input stage and Under-voltage lockout sections. Copyright © 2004–2011, Texas Instruments Incorporated Submit Documentation Feedback 9 Product Folder Links: LM5111 |
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