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ADP3625 Datasheet(PDF) 14 Page - Analog Devices |
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ADP3625 Datasheet(HTML) 14 Page - Analog Devices |
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14 / 16 page ![]() ADP3623/ADP3624/ADP3625/ADP3633/ADP3634/ADP3635 Rev. A | Page 14 of 16 THERMAL CONSIDERATIONS When designing a power MOSFET gate drive, the maximum power dissipation in the driver must be considered to avoid exceeding maximum junction temperature. Data on package thermal resistance is provided in Table 2 to help the designer in this task. There are several equally important aspects that must be considered. • Gate charge of the power MOSFET being driven • Bias voltage value used to power the driver • Maximum switching frequency of operation • Value of external gate resistance • Maximum ambient (and PCB) temperature • Type of package All of these factors influence and limit the maximum allowable power dissipated in the driver. The gate of a power MOSFET has a nonlinear capacitance characteristic. For this reason, although the input capacitance is usually reported in the MOSFET data sheet as CISS, it is not useful to calculate power losses. The total gate charge necessary to turn on a power MOSFET device is usually reported on the device data sheet under QG. This parameter varies from a few nanocoulombs (nC) to several hundreds of nC, and is specified at a specific VGS value (10 V or 4.5 V). The power necessary to charge and then discharge the gate of a power MOSFET can be calculated as: PGATE = VGS × QG × fSW where: VGS is the bias voltage powering the driver (VDD). QG is the total gate charge. fSW is the maximum switching frequency. The power dissipated for each gate (PGATE) still needs to be multip- lied by the number of drivers (in this case, 1 or 2) being used in each package, and it represents the total power dissipated in charging and discharging the gates of the power MOSFETs. Not all of this power is dissipated in the gate driver because part of it is actually dissipated in the external gate resistor, RG. The larger the external gate resistor is, the smaller the amount of power that is dissipated in the gate driver. In modern switching power applications, the value of the gate resistor is kept at a minimum to increase switching speed and minimize switching losses. In all practical applications where the external resistor is in the order of a few ohms, the contribution of the external resistor can be neglected, and the extra loss is assumed in the driver, providing a good guard band to the power loss calculations. In addition to the gate charge losses, there are also dc bias losses, due to the bias current of the driver. This current is present regardless of the switching. PDC = VDD × IDD The total estimated loss is the sum of PDC and PGATE. PLOSS = PDC + (n × PGATE) where n is the number of gates driven. When the total power loss is calculated, the temperature increase can be calculated as ΔTJ = PLOSS × θJA Design Example For example, consider driving two IRFS4310Z MOSFETs with a VDD of 12 V at a switching frequency of 300 kHz, using an ADP3624 in the SOIC_N_EP package. The maximum PCB temperature considered for this design is 85°C. From the MOSFET data sheet, the total gate charge is QG = 120 nC. PGATE = 12 V × 120 nC × 300 kHz = 432 mW PDC = 12 V × 1.2 mA = 14.4 mW PLOSS = 14.4 mW + (2 × 432 mW) = 878.4 mW From the MOSFET data sheet, the SOIC_N_EP thermal resistance is 59°C/W. ΔTJ = 878.4 mW × 59°C/W = 51.8°C TJ = TA + ΔTJ = 136.8°C ≤ TJMAX This estimated junction temperature does not factor in the power dissipated in the external gate resistor and, therefore, provides a certain guard band. If a lower junction temperature is required by the design, the MINI_SO_EP package can be used, which provides a thermal resistance of 43°C/W, so that the maximum junction temperature is ΔTJ = 878.4 mW × 43°C/W = 37.7°C TJ = TA + ΔTJ = 122.7°C ≤ TJMAX Other options to reduce power dissipation in the driver include reducing the value of the VDD bias voltage, reducing switching fre- quency, and choosing a power MOSFET with smaller gate charge. |
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