ISL6740EVAL2Z Intersil, ISL6740EVAL2Z Datasheet - Page 18
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ISL6740EVAL2Z
Manufacturer Part Number
ISL6740EVAL2Z
Description
EVALUATION BOARD 2 ISL6740
Manufacturer
Intersil
Datasheet
1.ISL6741IVZ.pdf
(29 pages)
Specifications of ISL6740EVAL2Z
Main Purpose
DC/DC, Step Down
Outputs And Type
1, Non-Isolated
Voltage - Output
12V
Current - Output
8A
Voltage - Input
36 ~ 75V
Regulator Topology
Buck
Board Type
Fully Populated
Utilized Ic / Part
ISL6740
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Power - Output
-
Frequency - Switching
-
MOSFET Selection
The criteria for selection of the primary side half-bridge FETs
and the secondary side synchronous rectifier FETs is largely
based on the current and voltage rating of the device.
However, the FET drain-source capacitance and gate
charge cannot be ignored.
The zero voltage switch (ZVS) transition timing is dependent
on the transformer’s leakage inductance and the
capacitance at the node between the upper FET source and
the lower FET drain. The node capacitance is comprised of
the drain-source capacitance of the FETs and the
transformer parasitic capacitance. The leakage inductance
and capacitance form an LC resonant tank circuit which
determines the duration of the transition. The amount of
energy stored in the LC tank circuit determines the transition
voltage amplitude. If the leakage inductance energy is too
low, ZVS operation is not possible and near or partial ZVS
operation occurs. As the leakage energy increases, the
voltage amplitude increases until it is clamped by the FET
body diode to ground or V
conducts. When the leakage energy exceeds the minimum
required for ZVS operation, the voltage is clamped until the
energy is transferred. This behavior increases the time
window for ZVS operation. This behavior is not without
consequences, however. The transition time and the period
of time during which the voltage is clamped reduces the
effective duty cycle.
The gate charge affects the switching speed of the FETs.
Higher gate charge translates into higher drive requirements
and/or slower switching speeds. The energy required to
drive the gates is dissipated as heat.
The maximum input voltage, V
determines the voltage rating required. With a maximum
input voltage of 53V for this application, and if we allow a
10% adder for transients, a voltage rating of 60V or higher
will suffice.
The RMS current through the each primary side FET can be
determined from Equation 17, substituting 5A of primary
current for I
FETs, rated at 100V and 7.5A (r
selected for the half-bridge switches.
The synchronous rectifier FETs must withstand
approximately one half of the input voltage assuming no
switching transients are present. This suggests a device
capable of withstanding at least 30V is required. Empirical
testing in the circuit revealed switching transients of 20V
were present across the device indicating a rating of at least
60V is required.
The RMS current rating of 7.07A for each SR FET requires a
low r
find in a 60V device. It was decided to use two devices in
parallel to simplify the thermal design. Two Fairchild FDS5670
DS(ON)
OUT
to minimize conduction losses, which is difficult to
. The result is 3.5A RMS. Fairchild FDS3672
IN
, depending on which FET
18
IN
DS(ON)
, plus transient voltage,
= 22mΩ), were
ISL6740, 1SL6741
devices are used in parallel for a total of four SR FETs. The
FDS5670 is rated at 60V and 10A (r
Oscillator Component Selection
The desired operating frequency of 235kHz for the converter
was established in the Design Criteria section. The
oscillator frequency operates at twice the frequency of the
converter because two clock cycles are required for a
complete converter period.
During each oscillator cycle the timing capacitor, C
charged and discharged. Determining the required
discharge time to achieve zero voltage switching (ZVS) is
the critical design goal in selecting the timing components.
The discharge time sets the deadtime between the two
outputs, and is the same as ZVS transition time. Once the
discharge time is determined, the remainder of the period
becomes the charge time.
The ZVS transition duration is determined by the
transformer’s primary leakage inductance, L
Coss, by the transformer’s parasitic winding capacitance,
and by any other parasitic elements on the node. The
parameters may be determined by measurement,
calculation, estimate, or by some combination of these
methods.
Device output capacitance, Coss, is non-linear with applied
voltage. To find the equivalent discrete capacitance, Cfet, a
charge model is used. Using a known current source, the
time required to charge the MOSFET drain to the desired
operating voltage is determined and the equivalent
capacitance is calculated.
Once the estimated transition time is determined, it must be
verified directly in the application. The transformer leakage
inductance was measured at 125nH and the combined
capacitance was estimated at 2000pF. Calculations indicate
a transition period of ~ 25ns. Verification of the performance
yielded a value of T
The remainder of the switching half-period is the charge
time, T
where F
Using Figure 4, the capacitor value appropriate to the
desired oscillator operating frequency of 470kHz can be
selected. A C
t
Cfet
T
zvs
C
=
≈
=
π L
------------------------------------------------------------------- -
--------------- - T
2 F
C
Ichg t •
------------------- -
•
S
, and can be found from
1
is the converter switching frequency.
lk
V
S
•
–
T
(
2C
D
value of 100pF, 220pF, or 330pF is
oss
2
=
D
F
--------------------------------- - 45 10
2 235 10
+
•
closer to 45ns.
C
xfrmr
1
•
)
3
–
S
DS(ON)
•
–
9
=
= 14mΩ).
lk
2.08
, by the FET
T
, must be
July 13, 2007
(EQ. 19)
(EQ. 20)
(EQ. 21)
FN9111.4
μs