The external gate-driver resistors,
RG(ON) and RG(OFF) are used to:
- Limit ringing caused by parasitic inductances and
capacitances
- Limit ringing caused by high voltage or high current switching
dv/dt, di/dt, and body-diode reverse recovery
- Fine-tune gate drive strength, specifically peak sink and
source current to optimize the switching loss
- Reduce electromagnetic interference (EMI)
The output stage has a pull-up structure
consisting of a P-channel MOSFET and an N-channel MOSFET in parallel. The combined
typical peak source current is 10 A for UCC5350L-Q1. Use Equation 1 to estimate the peak source current. Recommend using at least 5Ω gate resistor
for additional robustness for DWL package due to wide body adding additional
inductance.
Equation 1.
where
- RON is the external turn-on
resistance, which is 2.2 Ω in this
example.
- RGFET_Int is the power transistor internal gate resistance, found in
the power transistor data sheet. We will
assume 1.8Ω for our example.
- IOH is the typical peak
source current which is the minimum value between 10 A, the gate-driver peak source
current, and the calculated value based on the gate-drive loop resistance.
In this example, the peak source current is
approximately 3.36 A as calculated in Equation 2.
Equation 2.
Similarly, use Equation 3 to calculate the peak sink current.
Equation 3.
where
- ROFF is the external turn-off
resistance, which is 2.2 Ω in this
example.
- IOL is the typical peak sink
current which is the minimum value between 10
A, the gate-driver peak sink current, and the calculated value based on
the gate-drive loop resistance.
In this example, the peak sink current is the
minimum value between Equation 4 and 10 A.
Equation 4.
Note: The estimated peak current is also
influenced by PCB layout and load capacitance. Parasitic inductance in the
gate-driver loop can slow down the peak gate-drive current and introduce
overshoot and undershoot. Therefore, TI strongly recommends that the gate-driver
loop should be minimized. Conversely, the peak source and sink current is
dominated by loop parasitics when the load capacitance (CISS) of the
power transistor is very small (typically less than 1 nF) because the rising and
falling time is too small and close to the parasitic ringing period.