HIP2122, HIP2123
10
FN7670.0
December 23, 2011
FIGURE 15. PEAK PULL-UP CURRENT vs OUTPUT VOLTAGE FIGURE 16. PEAK PULL-DOWN CURRENT vs OUTPUT VOLTAGE
FIGURE 17. HIP2122 QUIESCENT CURRENT vs VOLTAGE FIGURE 18. HIP2123 QUIESCENT CURRENT vs VOLTAGE
FIGURE 19. BOOTSTRAP DIODE I-V CHARACTERISTICS FIGURE 20. V
HS
VOLTAGE vs V
DD
VOLTAGE
Typical Performance Curves (Continued)
0481012
0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
V
LO
, V
HO
(V)
I
OHL
, I
OHH
(A)
26
0481012
0
1.5
2.0
2.5
3.0
3.5
4.0
4.5
V
LO
, V
HO
(V)
I
OHL
, I
OHH
(A)
26
1.0
0.5
0 5 10 15 20
0
10
20
30
40
50
60
70
80
90
100
110
120
V
DD
, V
HB
(V)
I
DD
, I
HB
(µA)
I
HB
I
DD
0 5 10 15 20
V
DD
, V
HB
(V)
I
DD
, I
HB
(µA)
0
20
40
60
80
100
120
140
160
180
200
220
240
260
280
300
320
I
DD
I
HB
0.3 0.4 0.5 0.6 0.7 0.8
1
.
10
-3
0.01
0.10
1.00
FORWARD VOLTAGE (V)
FORWARD CURRENT (A)
1
.
10
-4
1
.
10
-5
1
.
10
-6
12 13 14 15 16
0
20
40
60
80
100
120
V
HS
TO V
SS
VOLTAGE (V)
V
DD
TO V
SS
VOLTAGE (V)
HIP2122, HIP2123
11
FN7670.0
December 23, 2011
Functional Description
Functional Overview
The HIP2122/23 have independent control inputs, LI and HI, for
each output; LO and HO. When LI is low, LO is low and likewise,
when HI is low, HO is low. The output negative transitions occur
with minimal (and fixed) propagation delays.
The positive transitions of each output are delayed by the
programmed delay as set by RDT. With 80k, the delay is
nominally 25ns. With 8k, the delay is nominally 220ns. Resistors
values less than 8k and greater than 80k are not recommended.
The delay time as a function of R
DT
is approximately
t
DT
(ns) = 2/R
DT
.
Delaying the rising edge but not the falling edge of each output is
the technique that prevents shoot-thru. Please note that there is
no logic that prevents both outputs from being on if both inputs
are on simultaneously.
The enable pin, EN, when low, drives both outputs to a low state.
When the PWM input transitions, it is necessary to insure that
both bridge FETS are not on at the same time to prevent
shoot-through currents (break before make). The programmable
dead time forces both outputs to be off before either of the
bridge FETs is driven on. An 8kΩ resistor connected between R
DT
and V
SS
results in a nominal dead time of 250ns. An 80kΩ
results with a minimum nominal dead time of 50ns. Resistors
values less than 8k and greater than 80k are not recommended.
Dead-time as a function of R
DT
is nominally t
DT
(ns) = 2/R
DT
.
The high-side driver bias is established by the boot capacitor
connected between HB and HS. The charge on the boot capacitor
is provided by the internal boot diode that is connected to V
DD
.
The current path to charge the boot capacitor occurs when the
low-side bridge FET is on. This charge current is limited in
amplitude by the inherent resistance of the boot diode and by the
drain-source voltage of the low-side FET. Assuming that the on
time of the low-side FET is sufficiently long to fully charge the
boot capacitor, the boot voltage will charge very close to V
DD
(less the boot diode drop and the low-side FET on voltage).
When the HI input transitions high, the high-side bridge FET is
driven on after the delay time. Because the HS node is connected
to the source of the high-side FET, the HS node will rise almost to
the level of the bridge voltage (less the conduction voltage across
the bridge FET). Because the boot capacitor voltage is referenced
to the source voltage of the high-side FET, the HB node is V
DD
volts above the HS node and the boot diode is reversed biased.
Because the high-side driver circuit is referenced to the HS node,
the HO output is now approximately VHB + VBRIDGE above
ground.
During the low to high transition of the HS node, the boot
capacitor sources the necessary gate charge to fully enhance the
high-side bridge FET gate. After the gate is fully charged, the boot
capacitor no longer sources the charge to the gate but continues
to provide bias current to the high-side driver. It is clear that the
charge of the boot capacitor must be substantially larger than
the required charge of the high-side FET and high-side driver
otherwise the boot voltage will sag excessively. If the boot
capacitor value is too small for the required maximum of on-time
of the high-side FET, the high-side UV lockout may engage
resulting with an unexpected operation.
Application Information
Selecting the Boot Capacitor Value
The boot capacitor value is chosen not only to supply the internal
bias current of the high-side driver but also, and more
significantly, to provide the gate charge of the driven FET without
causing the boot voltage to sag excessively. In practice, the boot
capacitor should have a total charge that is about 20 times the
gate charge of the driven power FET for approximately a 5% drop
in voltage after the charge has been transferred from the boot
capacitor to the gate capacitance.
The following parameters are required to calculate the value of
the boot capacitor for a specific amount of voltage droop. In this
example, the values used are arbitrary. They should be changed
to comply with the actual application.
The following equations calculate the total charge required for
the Period. This equation assumes that all of the parameters are
constant during the period duration. The error is insignificant if
the ripple is small.
V
DD
= 10V V
DD
can be any value between 7 and 14VDC
V
HB
= V
DD
- 0.6V = V
HO
High side driver bias voltage (V
DD
- boot diode
voltage) referenced to V
HS
Period = 1ms This is the longest expected switching period
I
HB
= 100µA Worst case high side driver current when
xHO = high
(this value is specified for V
DD
= 12V but the
error is not significant)
R
GS
= 100kΩ Gate-source resistor
(usually not needed)
Ripple = 5% Desired ripple voltage on the boot capacitor
(larger ripple is not recommended)
I
gate_leak
= 100nA From the FET vendor’s datasheet
Qgate80V = 64nC From Figure 21
FIGURE 21. TYPICAL GATE CHARGE OF A POWER FET
12
10
8
6
4
2
0
10 20 30 40 50 60 70 80
QG TOTAL GATE CHARGE (nC)
VGS, GATE-TO-SOURCE VOLTAGE (V)
0
V
DS
= 80V
V
DS
= 50V
V
DS
= 20V
I
D
= 33A
HIP2122, HIP2123
12
FN7670.0
December 23, 2011
Q
c
= Q
gate80V
+ Period x (I
HB
+ V
HO
/R
GS
+ I
gate_leak
)
C
boot
= Q
c
/(Ripple * VDD)
C
boot
= 0.52µF
If the gate to source resistor is removed (R
GS
is usually not
needed or recommended), then:
C
boot
= 0.33µF
Typical Application Circuit
Figure 23 is an example of how the HIP2122/23 can be
configured for a half bridge power supply application.
Depending on the application, the switching speed of the bridge
FETs can be reduced by adding series connected resistors
between the xHO outputs and the FET gates. Gate-Source
resistors are recommended on the low Side FETs to prevent
unexpected turn-on of the bridge should the bridge voltage be
applied before VDD. Gate-source resistors on the high side FETs
are not usually required if low-side gate-source resistors are
used. If relatively small gate-source resistors are used on the
high-side FETs, be aware that they will load the boot capacitor,
which will then require a larger value for the boot capacitor.
Transients on HS Node
An important operating condition that is frequently overlooked by
designers is the negative transient on the xHS pins that occurs
when the high side bridge FET turns off. The Absolute Maximum
transient allowed on the xHS pin is -6V but it is wise to minimize
the amplitude to lower levels. This transient is the result of the
parasitic inductance of the low-side drain-source conductor on
the PCB. Even the parasitic inductance of the low-side FET
contributes to this transient.
When the high-side bridge FET turns off (see Figure 22), because
of the inductive characteristics of the load, the current that was
flowing in the high-side FET (blue) must rapidly commutate to
flow through the low side FET (red). The amplitude of the
negative transient impressed on the xHS node is (di/dt x L) where
L is the total parasitic inductance of the low-side FET drain-
source path and di/dt is the rate at which the high-side FET is
turned off. With the increasing power levels of power supplies
and motor, clamping this transient become more and more
significant for the proper operation of the HIP2122/23.
There are several ways of reducing the amplitude of this
transient. If the bridge FETs are turned off more slowly to reduce
di/dt, the amplitude will be reduced but at the expense of more
switching losses in the FETs. Careful PCB design will also reduce
the value of the parasitic inductance. However, these two
solutions by themselves may not be sufficient. Figure 22
illustrates a simple method for clamping the negative transient.
A fast PN junction, 1A diode is connected between xHS and VSS
as shown. It is important that this diode be placed as close as
possible to the xHS and VSS pins to minimize the parasitic
inductance of this current path. Because this clamping diode is
essentially in parallel with the body diode of the low side FET, a
small value resistor is necessary to limit current when the body
diode of the low side bridge FET is conducting during the dead
time.
Please note that a similar transient with a positive polarity occurs
when the low-side FET turns off. This is less frequently a problem
because xHS node is floating up toward the bridge bias voltage.
The Absolute Max voltage rating for the xHS node does need to
be observed when the positive transient occurs.
VSS
HS
LO
HO
INDUCTIVE
LOAD
+
-
+
-
FIGURE 22. PARASITIC INDUCTANCE CAUSES TRANSIENTS ON HS
NODE
ISL78420
HI
DRIVER
LO
DRIVER
LOGIC
HO
LO
HS
PWM
EN
RDT
VSS
VDD HB
8-15V
100V MAX
PWM
CONTROLLER
FIGURE 23. TYPICAL HALF BRIDGE APPLICATION

HIP2123FRTAZ-T

Mfr. #:
Manufacturer:
Renesas / Intersil
Description:
Gate Drivers 100V 2A PEAK HALF BRDG DRV W/DELAY TMR
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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