L6386E STMicroelectronics, L6386E Datasheet - Page 8

IC DRIVER HI/LO SIDE HV 14-DIP

L6386E

Manufacturer Part Number
L6386E
Description
IC DRIVER HI/LO SIDE HV 14-DIP
Manufacturer
STMicroelectronics
Type
High Side/Low Sider
Datasheet

Specifications of L6386E

Configuration
High and Low Side, Independent
Input Type
Non-Inverting
Delay Time
110ns
Current - Peak
400mA
Number Of Configurations
1
Number Of Outputs
2
High Side Voltage - Max (bootstrap)
600V
Voltage - Supply
17V
Operating Temperature
-40°C ~ 125°C
Mounting Type
Through Hole
Package / Case
14-DIP (0.300", 7.62mm)
Product
H-Bridge Drivers
Rise Time
50 ns
Fall Time
30 ns
Maximum Power Dissipation
750 mW
Maximum Operating Temperature
+ 125 C
Mounting Style
Through Hole
Bridge Type
Half Bridge
Minimum Operating Temperature
- 45 C
Number Of Drivers
2
For Use With
497-5492 - EVAL BOARD FOR L6384/L6385/L6386
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Other names
497-6215-5

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Bootstrap driver
4
4.1
8/18
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
integrated structure replaces the external diode. It is realized by a high voltage DMOS,
driven synchronously with the low side driver (LVG), with in series a diode, as shown in
Figure 4
diode connected in series to the DMOS has been added to avoid undesirable turn on of it.
C
To choose the proper C
capacitor. This capacitor C
The ratio between the capacitors C
It has to be:
e.g.: if Q
300 mV.
If HVG has to be supplied for a long time, the C
the leakage losses.
e.g.: HVG steady state consumption is lower than 200 μA, so if HVG T
to supply 1 μC to C
The internal bootstrap driver gives great advantages: the external fast recovery diode can
be avoided (it usually has great leakage current).
This structure can work only if V
LVG is on. The charging time (T
fulfilled and it has to be long enough to charge the capacitor.
The bootstrap driver introduces a voltage drop due to the DMOS R
Ω). At low frequency this drop can be neglected. Anyway increasing the frequency it must be
taken in to account.
The following equation is useful to compute the drop on the bootstrap DMOS:
where Q
bootstrap DMOS, and T
BOOT
gate
gate
b. An internal charge pump
selection and charging
is 30 nC and V
is the gate charge of the external power MOS, R
EXT
. This charge on a 1 μF capacitor means a voltage drop of 1 V.
BOOT
charge
V
drop
EXT
gate
value the external MOS can be seen as an equivalent
is the charging time of the bootstrap capacitor.
=
Doc ID 13989 Rev 2
is related to the MOS total gate charge:
is 10 V, C
charge
OUT
I
ch
EXT
arg
is close to GND (or lower) and in the meanwhile the
(Figure 4
) of the C
e
R
and C
C
C
dson
EXT
EXT
BOOT
is 3 nF. With C
BOOT
=
>>>C
BOOT
b) provides the DMOS driving voltage. The
V
Q
-------------- -
V
BOOT
drop
gate
gate
EXT
is proportional to the cyclical voltage loss.
is the time in which both conditions are
(Figure 4
selection has to take into account also
=
------------------ - R
T
Q
ch
gate
BOOT
arg
DSon
e
a). In the L6386E a patented
dson
= 100 nF the drop would be
is the on resistance of the
DSon
ON
(typical value: 125
is 5 ms, C
BOOT
L6386E
has

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