13
FN9055.12
September 30, 2015
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Input Capacitor Selection
Use a mix of input bypass capacitors to control the voltage
overshoot across the MOSFETs. Use small ceramic
capacitors for high frequency decoupling and bulk capacitors
to supply the current needed each time Q
1
turns on. Place the
small ceramic capacitors physically close to the MOSFETs
and between the drain of Q
1
and the source of Q
2
.
The important parameters for the bulk input capacitor are the
voltage rating and the RMS current rating. For reliable
operation, select the bulk capacitor with voltage and current
ratings above the maximum input voltage and largest RMS
current required by the circuit. The capacitor voltage rating
should be at least 1.25 times greater than the maximum
input voltage and a voltage rating of 1.5 times is a
conservative guideline. The RMS current rating requirement
for the input capacitor of a buck regulator is approximately
1/2 the DC load current.
The maximum RMS current required by the regulator may be
closely approximated using Equation 15:
For a through hole design, several electrolytic capacitors may
be needed. For surface mount designs, solid tantalum
capacitors can be used, but caution must be exercised with
regard to the capacitor surge current rating. These capacitors
must be capable of handling the surge-current at power-up.
Some capacitor series available from reputable manufacturers
are surge current tested.
MOSFET Selection/Considerations
The ISL6526, ISL6526A require two N-Channel power
MOSFETs. These should be selected based upon r
DS(ON)
,
gate supply requirements, and thermal management
requirements.
In high-current applications, the MOSFET power dissipation,
package selection and heatsink are the dominant design
factors. The power dissipation includes two loss components;
conduction loss and switching loss. The conduction losses are
the largest component of power dissipation for both the upper
and the lower MOSFETs. These losses are distributed
between the two MOSFETs according to duty factor. The
switching losses seen when sourcing current will be different
from the switching losses seen when sinking current. When
sourcing current, the upper MOSFET realizes most of the
switching losses. The lower switch realizes most of the
switching losses when the converter is sinking current (see
Equations 16 and 17). These equations assume linear
voltage-current transitions and do not adequately model
power loss due the reverse-recovery of the upper and lower
MOSFET’s body diode. The gate-charge losses are
dissipated by the ISL6526, ISL6526A and don't heat the
MOSFETs. However, large gate-charge increases the
switching interval, t
SW
which increases the
MOSFET
switching losses. Ensure that both MOSFETs are within their
maximum junction temperature at high ambient temperature
by calculating the temperature rise according to package
thermal-resistance specifications. A separate heatsink may be
necessary depending upon MOSFET power, package type,
ambient temperature and air flow.
Given the reduced available gate bias voltage (5V), logic-level
or sub-logic-level transistors should be used for both
N-MOSFETs. Caution should be exercised with devices
exhibiting very low V
GS(ON)
characteristics. The shoot-through
protection present aboard the ISL6526, ISL6526A may be
circumvented by these MOSFETs if they have large parasitic
impedances and/or capacitances that would inhibit the gate of
the MOSFET from being discharged below its threshold level
before the complementary MOSFET is turned on.
Bootstrap Component Selection
External bootstrap components, a diode and capacitor, are
required to provide sufficient gate enhancement to the upper
MOSFET. The internal MOSFET gate driver is supplied by the
external bootstrap circuitry, as shown in Figure 7. The boot
capacitor, C
BOOT
, develops a floating supply voltage
referenced to the PHASE pin. This supply is refreshed each
cycle, when D
BOOT
conducts, to a voltage of CPVOUT less the
boot diode drop, V
D
, plus the voltage rise across Q
LOWER
.
I
RMS
MAX
V
OUT
V
IN
--------------
I
OUT
MAX
2
1
12
------
V
IN
V
OUT
Lf
s
-----------------------------
V
OUT
V
IN
--------------


2
+


=
(EQ. 15)
P
LOWER
= Io
2
x r
DS(ON)
x (1 - D)
Losses while Sourcing Current
P
UPPER
Io
2
r
DS ON
D
1
2
---
Io V
IN
t
SW
f
s
+=
(EQ. 16)
Where: D is the duty cycle = V
OUT
/V
IN
,
t
SW
is the combined switch ON and OFF time, and
f
s
is the switching frequency.
Losses while Sinking Current
P
LOWER
Io
2
r
DS ON
1D
1
2
---
Io V
IN
t
SW
f
s
+=
P
UPPER
= Io
2
x r
DS(ON)
x D
(EQ. 17)
ISL6526,
GND
LGATE
UGATE
PHASE
BOOT
V
IN
NOTE:
NOTE:
V
G-S
= V
CC
C
BOOT
D
BOOT
Q
UPPER
Q
LOWER
+
-
FIGURE 7. UPPER GATE DRIVE BOOTSTRAP
V
G-S
= V
CC
-V
D
+
V
D
-
CPVOUT
ISL6526A
ISL6526, ISL6526A
14
FN9055.12
September 30, 2015
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Just after the PWM switching cycle begins and the charge
transfer from the bootstrap capacitor to the gate capacitance
is complete, the voltage on the bootstrap capacitor is at its
lowest point during the switching cycle. The charge lost on
the bootstrap capacitor will be equal to the charge
transferred to the equivalent gate-source capacitance of the
upper MOSFET as shown in Equation 18:
where Q
GATE
is the maximum total gate charge of the upper
MOSFET, C
BOOT
is the bootstrap capacitance, V
BOOT1
is
the bootstrap voltage immediately before turn-on, and
V
BOOT2
is the bootstrap voltage immediately after turn-on.
The bootstrap capacitor begins its refresh cycle when the gate
drive begins to turn-off the upper MOSFET. A refresh cycle
ends when the upper MOSFET is turned on again, which
varies depending on the switching frequency and duty cycle.
The minimum bootstrap capacitance can be calculated by
rearranging the previous equation and solving for C
BOOT
.
Typical gate charge values for MOSFETs considered in
these types of applications range from 20 to 100nC. Since
the voltage drop across Q
LOWER
is negligible, V
BOOT1
is
simply V
CPVOUT
- V
D
. A Schottky diode is recommended to
minimize the voltage drop across the bootstrap capacitor
during the on-time of the upper MOSFET. Initial calculations
with V
BOOT2
no less than 4V will quickly help narrow the
bootstrap capacitor range.
For example, consider an upper MOSFET is chosen with a
maximum gate charge, Q
g
, of 100nC. Limiting the voltage
drop across the bootstrap capacitor to 1V results in a value
of no less than 0.1µF. The tolerance of the ceramic capacitor
should also be considered when selecting the final bootstrap
capacitance value.
A fast recovery diode is recommended when selecting a
bootstrap diode to reduce the impact of reverse recovery
charge loss. Otherwise, the recovery charge, Q
RR
, would
have to be added to the gate charge of the MOSFET and
taken into consideration when calculating the minimum
bootstrap capacitance.
ISL6526, ISL6526A DC/DC Converter
Application Circuit
Figure 8 shows an application circuit of a DC/DC Converter.
Detailed information on the circuit, including a complete Bill
of Materials and circuit board description, can be found in
Application Note AN1021:
http://www.intersil.com/data/an/an1021.pdf.
Q
GATE
C
BOOT
V
BOOT1
V
BOOT2
=
(EQ. 18)
C
BOOT
Q
GATE
V
BOOT1
V
BOOT2
-----------------------------------------------------
=
(EQ. 19)
ISL6526, ISL6526A
15
FN9055.12
September 30, 2015
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Component Selection Notes:
C
3,
C
8,
C
9
- Each 150µF, Panasonic EEF-UE0J151R or Equivalent.
D1 - 30mA Schottky Diode, MA732 or Equivalent
L
1
- 1µH Inductor, Panasonic P/N ETQ-P6F1ROSFA or Equivalent.
Q
1
- Fairchild MOSFET; ITF86110DK8.
2.5V @ 5A
FBCOMP
UGATE
PHASE
BOOT
GND
LGATE
ISL6526, ISL6526A
R
3
R
5
C
10
C
11
R
2
L
1
D
1
C
7
C
1
C
4
C
6
C
8, 9
OCSET
CPVOUT
C
3
R
1
Q
1
CT1
CT2
CPGND
VCC
3.3V
C
5
C
2
C
12
R
4
GND
U
1
GND
14
1
2
3
4
5
8
6
7
9
10
11
12
13
TP
1
TP
3
ENABLE
9.76k
6.49k
2.26k
124
0.1µF
1000pF
10µF
0.22µF
1µF
0.1µF
33pF
5600pF
8200pF
1.07k
CERAMIC
ENABLE
FIGURE 8. 3.3V TO 2.5V 5A DC/DC CONVERTER
CAP
ISL6526, ISL6526A

ISL6526ACBZ

Mfr. #:
Manufacturer:
Renesas / Intersil
Description:
Switching Controllers 600KHZ SNG PWM W/CHA RGE PUMP 14LD NSOIC
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
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