lm5113sdx National Semiconductor Corporation, lm5113sdx Datasheet - Page 6

• Manufacturer Part Number: lm5113sdx
• Description: 5a, 100v Half-bridge Gate Driver For Enhancement Mode Gan Fets
• Manufacturer: National Semiconductor Corporation

www.national.com
Detailed Operating Description
The LM5113 is designed to drive both the high-side and the
low-side enhancement mode Gallium Nitride FETs in a syn-
chronous buck or a half-bridge configuration. The outputs of
the LM5113 are independently controlled with TTL input
thresholds. The inputs of the LM5113 can withstand voltages
up to 14V regardless of the VDD voltage, and can be directly
connected to the outputs of PWM controllers.
The high side driver uses the floating bootstrap capacitor volt-
age to drive the high-side FET. As shown in
bootstrap capacitor is recharged through an internal boot-
strap diode each cycle when the HS pin is pulled below the
VDD voltage. For inductive load applications the HS node will
fall to a negative potential, clamped by the low side FET.
Due to the intrinsic feature of enhancement mode GaN FETs
the source-to-drain voltage, when the gate is pulled low, is
usually higher than a diode forward voltage drop. This can
lead to an excessive bootstrap voltage that can damage the
high-side GaN FET. The LM5113 solves this problem with an
internal clamping circuit that prevents the bootstrap voltage
from exceeding 5V.
The output pull-down and pull-up resistance of LM5113 is op-
timized for enhancement mode GaN FETs to achieve high
frequency, efficient operation. The 0.5Ω pull-down resistance
provides a robust low impedance turn-off path necessary to
eliminate undesired turn-on induced by high dv/dt or high di/
dt. The 2Ω pull-up resistance helps reduce the ringing and
over-shoot of the switch node voltage. The split outputs of the
LM5113 offer flexibility to adjust the turn-on and turn-off speed
by independently adding additional impedance in either the
turn-on path and/or the turn-off path.
The LM5113 has an Under-voltage Lockout (UVLO) on both
the VDD and bootstrap supplies. When the VDD voltage is
below the threshold voltage of 4V, both the HI and LI inputs
are ignored, to prevent the GaN FETs from being partially
turned on. Also if there is sufficient VDD voltage, the UVLO
will actively pull the LOL and HOL low. When the HB to HS
bootstrap voltage is below the UVLO threshold of 3.3V, only
HOL is pulled low. Both UVLO threshold voltages have
200mV of hysteresis to avoid chattering.
Bypass Capacitor
The VDD bypass capacitor provides the gate charge for the
low-side and high-side transistors and to absorb the reverse
recovery charge of the bootstrap diode. The required bypass
capacitance can be calculated as follows:
Q
transistors respectively. Q
the bootstrap diode, which is typically around 4nC. ΔV is the
maximum allowable voltage drop across the bypass capaci-
gH
and Q
gL
are gate charge of the high-side and low-side
rr
is the reverse recovery charge of
Figure
1, the
6
tor. A 0.1uF or larger value, good quality, ceramic capacitor
is recommended. The bypass capacitor should be placed as
close to the pins of the IC as possible to minimize the parasitic
inductance.
Bootstrap Capacitor
The bootstrap capacitor provides the gate charge for the high-
side switch, dc bias power for HB under-voltage lockout cir-
cuit, and the reverse recovery charge of the bootstrap diode.
The required bypass capacitance can be calculated as fol-
lows:
I
maximum on-time period of the high-side transistor. A good
quality, ceramic capacitor should be used for the bootstrap
capacitor. It is recommended to place the bootstrap capacitor
as close to the HB and HS pins as possible.
Power Dissipation
The power consumption of the driver is an important measure
that determines the maximum achievable operating frequen-
cy of the driver. It should be kept below the maximum power
dissipation limit of the package at the operating temperature.
The total power dissipation of the LM5113 is the sum of the
gate driver losses and the bootstrap diode power loss.
The gate driver losses are incurred by charge and discharge
of the capacitive load. It can be approximated as
C
tive loads respectively. It can also be calculated with the total
input gate charge of the high-side and the low-side transistors
as
The bootstrap diode power loss is the sum of the forward bias
power loss that occurs while charging the bootstrap capacitor
and the reverse bias power loss that occurs during reverse
recovery. Since each of these events happens once per cycle,
the diode power loss is proportional to the operating frequen-
cy. Larger capacitive loads require more energy to recharge
the bootstrap capacitor resulting in more losses. Higher input
voltages (V
recovery losses.
HB
LoadH
is the quiescent current of the high-side driver. t
and C
IN
) to the half bridge also result in higher reverse
LoadL
are the high-side and the low-side capaci-
on
is the