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AN2785 Datasheet(PDF) 10 Page - STMicroelectronics

Part # AN2785
Description  L6393 half bridge gate driver
PDF  51 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN2785 Datasheet(HTML) 10 Page - STMicroelectronics

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Bootstrap driver
AN2785
10/51
Doc ID 14785 Rev 1
5
Bootstrap driver
A bootstrap circuitry is needed to supply the high voltage section. This function is normally
accomplished by a high-voltage fast recovery diode (Figure 6 a). In the L6393 a patented
integrated structure replaces the external diode. It is realized with a high-voltage DMOS
driven synchronously with the low-side driver (LVG), with a diode in series, as shown in the b
part of Figure 6 on page 11. An internal charge pump (Figure 6 b) provides the DMOS
driving voltage.
5.1
CBOOT selection and charging
To choose the proper CBOOT value the external MOS can be seen as an equivalent
capacitor. This capacitor CEXT is related to the total gate charge of the MOS.
Equation 1
The ratio between the capacitors CEXT and CBOOT is proportional to the cyclical voltage
loss. It must be:
Equation 2
CBOOT >> CEXT
For example, if Qgate is 30 nC and Vgate is 10 V, CEXT is 3 nF. With CBOOT = 100 nF, the
drop would be 300 mV.
If HVG has to be supplied for a long time, the CBOOT selection must also take into account
the leakage and quiescent losses.
For example, since the HVG steady state consumption is lower than 200 µA, if HVG TON is
5 ms then CBOOT has to supply 1 µC to CEXT. This charge on a 1 µF capacitor means a
voltage drop of 1 V.
The internal bootstrap driver gives a great advantage: the external fast-recovery high-
voltage diode can be avoided (it usually has great leakage current). This structure works if
VOUT is close to GND (or lower) while LVG is on. The charging time (Tcharge) of CBOOT is the
time in which both conditions are fulfilled and it has to be long enough to charge the
capacitor.
The bootstrap driver introduces a voltage drop due to the DMOS RDS(on). At a low frequency
operation this drop can be neglected, but if the frequency is increased the drop must be
taken into account.
The following equation is useful to compute the drop on the bootstrap DMOS.
Equation 3
where Qgate is the gate charge of the external power MOS, RDS(on) is the ON resistance of
the bootstrap DMOS and TCHARGE is the charging time of the bootstrap capacitor.
GATE
GATE
EXT
V
Q
C
=
DSON
CHARGE
GATE
DROP
DSON
CHARGE
DROP
R
T
Q
V
R
I
V
⋅
=
→
⋅
=



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