ISL6520AIRZS2698

7
FN9016.6
December 10, 2009
Figure 3 shows the critical power components of the converter.
To minimize the voltage overshoot, the interconnecting wires
indicated by heavy lines should be part of a ground or power
plane in a printed circuit board. The components shown in
Figure 3 should be located as close together as possible.
Please note that the capacitors C
IN
and C
O
may each
represent numerous physical capacitors. Locate the ISL6520A
within 3 inches of the MOSFETs, Q
1
and Q
2
. The circuit traces
for the MOSFETs’ gate and source connections from the
ISL6520A must be sized to handle up to 1A peak current.
Figure 4 shows the circuit traces that require additional
layout consideration. Use single point and ground plane
construction for the circuits shown. Minimize any leakage
current paths on the COMP/OCSET pin and locate the
resistor, R
OSCET
close to the COMP/OCSET pin because
the internal current source is only 20µA. Provide local V
CC
decoupling between VCC and GND pins. Locate the
capacitor, C
BOOT
as close as practical to the BOOT and
PHASE pins. All components used for feedback
compensation should be located as close to the IC a
practical.
Feedback Compensation
Figure 5 highlights the voltage-mode control loop for a
synchronous-rectified buck converter. The output voltage
(V
OUT
) is regulated to the Reference voltage level. The
error amplifier (Error Amp) output (V
E/A
) is compared with
the oscillator (OSC) triangular wave to provide a
pulse-width modulated (PWM) wave with an amplitude of
V
IN
at the PHASE node. The PWM wave is smoothed by the
output filter (L
O
and C
O
).
The modulator transfer function is the small-signal transfer
function of V
OUT
/V
E/A
. This function is dominated by a DC
Gain and the output filter (L
O
and C
O
), with a double pole
break frequency at F
LC
and a zero at F
ESR
. The DC Gain of
the modulator is simply the input voltage (V
IN
) divided by the
peak-to-peak oscillator voltage ΔV
OSC
.
Modulator Break Frequency Equations
The compensation network consists of the error amplifier
(internal to the ISL6520A) and the impedance networks Z
IN
and Z
FB
. The goal of the compensation network is to provide
a closed loop transfer function with the highest 0dB crossing
frequency (f
0dB
) and adequate phase margin. Phase margin
is the difference between the closed loop phase at f
0dB
and
180 degrees. The following equations relate the
compensation network’s poles, zeros and gain to the
components (R
1
, R
2
, R
3
, C
1
, C
2
, and C
3
) in Figure 7. Use
these guidelines for locating the poles and zeros of the
compensation network:
1. Pick Gain (R
2
/R
1
) for desired converter bandwidth.
2. Place 1
ST
Zero Below Filter’s Double Pole (~75% F
LC
).
3. Place 2
ND
Zero at Filter’s Double Pole.
L
O
C
O
LGATE
UGATE
PHASE
Q
1
Q
2
V
IN
V
OUT
RETURN
ISL6520A
C
IN
LOAD
FIGURE 3. PRINTED CIRCUIT BOARD POWER AND
GROUND PLANES OR ISLANDS
FIGURE 4. PRINTED CIRCUIT BOARD SMALL SIGNAL
LAYOUT GUIDELINES
+5V
ISL6520A
COMP/OCSET
GND
VCC
BOOT
D
1
L
O
C
O
V
OUT
LOAD
Q
1
Q
2
PHASE
+V
IN
C
BOOT
C
VCC
R
OCSET
+5V
FIGURE 5. VOLTAGE-MODE BUCK CONVERTER
COMPENSATION DESIGN
V
OUT
REFERENCE
L
O
C
O
ESR
V
IN
ΔV
OSC
ERROR
AMP
PWM
DRIVER
(PARASITIC)
Z
FB
+
-
REFERENCE
R
1
R
3
R
2
C
3
C
2
C
1
COMP
V
OUT
FB
Z
FB
ISL6520A
Z
IN
COMPARATOR
DRIVER
DETAILED COMPENSATION COMPONENTS
PHASE
V
E/A
+
-
+
-
Z
IN
OSC
F
LC
1
2π x L
O
x C
O
-------------------------------------------= F
ESR
1
2π x ESR x C
O
--------------------------------------------=
(EQ. 4)
ISL6520A
8
FN9016.6
December 10, 2009
4. Place 1
ST
Pole at the ESR Zero.
5. Place 2
ND
Pole at Half the Switching Frequency.
6. Check Gain against Error Amplifier’s Open-Loop Gain.
7. Estimate Phase Margin - Repeat if Necessary.
Compensation Break Frequency Equations
Figure 6 shows an asymptotic plot of the DC/DC converter’s
gain vs frequency. The actual Modulator Gain has a high gain
peak due to the high Q factor of the output filter and is not
shown in Figure 6. Using the previously mentioned guidelines
should give a Compensation Gain similar to the curve plotted.
The open loop error amplifier gain bounds the compensation
gain. Check the compensation gain at F
P2
with the
capabilities of the error amplifier. The Closed Loop Gain is
constructed on the graph of Figure 6 by adding the Modulator
Gain (in dB) to the Compensation Gain (in dB). This is
equivalent to multiplying the modulator transfer function to the
compensation transfer function and plotting the gain.
The compensation gain uses external impedance networks
Z
FB
and Z
IN
to provide a stable, high bandwidth (BW) overall
loop. A stable control loop has a gain crossing with
-20dB/decade slope and a phase margin greater than 45
degrees. Include worst case component variations when
determining phase margin.
Component Selection Guidelines
Output Capacitor Selection
An output capacitor is required to filter the output and supply
the load transient current. The filtering requirements are a
function of the switching frequency and the ripple current.
The load transient requirements are a function of the slew
rate (di/dt) and the magnitude of the transient load current.
These requirements are generally met with a mix of
capacitors and careful layout.
Modern components and loads are capable of producing
transient load rates above 1A/ns. High frequency capacitors
initially supply the transient and slow the current load rate
seen by the bulk capacitors. The bulk filter capacitor values
are generally determined by the ESR (Effective Series
Resistance) and voltage rating requirements rather than
actual capacitance requirements.
High frequency decoupling capacitors should be placed as
close to the power pins of the load as physically possible. Be
careful not to add inductance in the circuit board wiring that
could cancel the usefulness of these low inductance
components. Consult with the manufacturer of the load on
specific decoupling requirements.
Use only specialized low-ESR capacitors intended for
switching-regulator applications for the bulk capacitors. The
bulk capacitor’s ESR will determine the output ripple voltage
and the initial voltage drop after a high slew-rate transient. An
aluminum electrolytic capacitor’s ESR value is related to the
case size with lower ESR available in larger case sizes.
However, the Equivalent Series Inductance (ESL) of these
capacitors increases with case size and can reduce the
usefulness of the capacitor to high slew-rate transient loading.
Unfortunately, ESL is not a specified parameter. Work with
your capacitor supplier and measure the capacitor’s
impedance with frequency to select a suitable component. In
most cases, multiple electrolytic capacitors of small case size
perform better than a single large case capacitor.
Output Inductor Selection
The output inductor is selected to meet the output voltage
ripple requirements and minimize the converter’s response
time to the load transient. The inductor value determines the
converter’s ripple current and the ripple voltage is a function
of the ripple current. The ripple voltage and current are
approximated by the following equations:
Increasing the value of inductance reduces the ripple current
and voltage. However, the large inductance values reduce
the converter’s response time to a load transient.
One of the parameters limiting the converter’s response to
a load transient is the time required to change the inductor
current. Given a sufficiently fast control loop design, the
ISL6520A will provide either 0% or 100% duty cycle in
response to a load transient. The response time is the time
required to slew the inductor current from an initial current
value to the transient current level. During this interval the
difference between the inductor current and the transient
current level must be supplied by the output capacitor.
Minimizing the response time can minimize the output
capacitance required.
F
Z1
1
2π x R
2
x C
1
------------------------------------=
F
Z2
1
2π x R
1
R
3
+() x C
3
-------------------------------------------------------=
F
P1
1
2π x R
2
x
C
1
x C
2
C
1
C
2
+
----------------------
⎝⎠
⎜⎟
⎛⎞
---------------------------------------------------------=
F
P2
1
2π x R
3
x C
3
------------------------------------=
(EQ. 5)
100
80
60
40
20
0
-20
-40
-60
F
P1
F
Z2
10M1M100K10K1K10010
OPEN LOOP
ERROR AMP GAIN
F
Z1
F
P2
20LOG
F
LC
F
ESR
COMPENSATION
GAIN (dB)
FREQUENCY (Hz)
GAIN
20LOG
(V
IN
/DV
OSC
)
MODULATOR
GAIN
(R
2
/R
1
)
FIGURE 6. ASYMPTOTIC BODE PLOT OF CONVERTER GAIN
CLOSED LOOP
GAIN
ΔI =
V
IN
- V
OUT
Fs x L
V
OUT
V
IN
ΔV
OUT
= ΔI x ESR
x
(EQ. 6)
ISL6520A
9
FN9016.6
December 10, 2009
The response time to a transient is different for the
application of load and the removal of load. The following
equations give the approximate response time interval for
application and removal of a transient load:
where: I
TRAN
is the transient load current step, t
RISE
is the
response time to the application of load, and t
FALL
is the
response time to the removal of load. The worst case
response time can be either at the application or removal of
load. Be sure to check both of these equations at the
minimum and maximum output levels for the worst case
response time.
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.
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 currentrating. 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 ISL6520A requires 2 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 the
following equations ). 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
ISL6520A 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 ISL6520A may be
circumvented by these MOSFETs if they have large parasitic
impedences and/or capacitances that would inhibit the gate
of the MOSFET from being discharged below it’s threshold
level before the complementary MOSFET is turned on.
Figure 7 shows the upper gate drive (BOOT pin) supplied by a
bootstrap circuit from V
CC
. The boot capacitor, C
BOOT
,
develops a floating supply voltage referenced to the PHASE
pin. The supply is refreshed to a voltage of V
CC
less the boot
diode drop (V
D
) each time the lower MOSFET, Q
2
, turns on.
t
RISE
=
L x I
TRAN
V
IN
- V
OUT
t
FALL
=
L x I
TRAN
V
OUT
(EQ. 7)
P
LOWER
= Io
2
x r
DS(ON)
x (1 - D)
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 Sourcing Current
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
r
DS ON()
× D×
1
2
---
Io V
IN
× t
SW
F
S
××+=
P
UPPER
= Io
2
x r
DS(ON)
x D
(EQ. 8)
+5V
ISL6520A
GND
LGATE
UGATE
PHASE
BOOT
VCC
+5V
NOTE:
NOTE:
V
G-S
V
CC
C
BOOT
D
BOOT
Q1
Q2
+
-
FIGURE 7. UPPER GATE DRIVE BOOTSTRAP
V
G-S
V
CC
-V
D
+ V
D
-
ISL6520A

ISL6520AIRZS2698

Mfr. #:
Manufacturer:
Renesas / Intersil
Description:
Switching Controllers 16LD 4X4QFN SINGLE 5V PWM CONT W/DDRG
Lifecycle:
New from this manufacturer.
Delivery:
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