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L6395 Datasheet(PDF) 11 Page - STMicroelectronics

Part # L6395
Description  Industrial drives and fans
PDF  16 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

L6395 Datasheet(HTML) 11 Page - STMicroelectronics

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DocID024048 Rev 2
11/16
L6395
Bootstrap driver
16
7
Bootstrap driver
A bootstrap circuitry is needed to supply the high voltage section. This function is normally
accomplished using a high voltage fast recovery diode (Figure 6). In the L6395 device
a patented integrated structure replaces the external diode. It is implemented using a high
voltage DMOS, driven synchronously with the low-side driver (LVG), with a diode in series,
as shown in Figure 7. An internal charge pump provides the DMOS driving voltage.
CBOOT selection and charging
To select the proper CBOOT value the external MOS can be seen as an equivalent capacitor.
This capacitor CEXT is related to the MOS total gate charge:
Equation 1
The ratio between the capacitors CEXT and CBOOT is proportional to the cyclical voltage
loss.
It must be:
Equation 2
E.g.: if Qgate is 30 nC and Vgate is 10 V, CEXT is 3 nF. With CBOOT = 100 nF the drop is
300 mV.
If HVG needs to be supplied for an extended period, the CBOOT selection has to take into
account also the leakage and quiescent losses.
E.g.: HVG steady state consumption is lower than 220
A, so if HVG TON is 5 ms, CBOOT
must supply 1.1
C to CEXT. This charge on a 1 F capacitor means a voltage drop of 1.1 V.
The internal bootstrap driver offers some important advantages: the external fast recovery
diode can be avoided (it usually has a high leakage current).
This structure can work only if VOUT is close to GND (or lower) and, at the same time, the
LVG is on. The charging time (Tcharge) of the 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) (typical value:
120
). At low switching frequency, this drop can be neglected but, operating at high
switching frequency, it should 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 MOSFET, RDS(on) is the on-resistance
of the bootstrap DMOS and Tcharge is the charging time of the bootstrap capacitor.
CEXT
Qgate
Vgate
---------------
=
CBOOT CEXT
»
Vdrop
Ich e
arg
RDS on

Vdrop
Qgate
Tch e
arg
------------------- RDS on

=
=



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