The ST1S10 is a step-down DC-DC converter with an optimized inhibit function for powering
high-voltage LCD applications and low-voltage digital core HDD applications. Generally, it
replaces the high current linear solution when high power dissipation is a problem. It
provides up to 3 A over an input voltage range of 2.5 V to 18 V and synchronous rectification
saves the external Schottky diode. A high internal switching frequency (0.9 MHz) allows it to
use tiny surface-mount components, as well as the resistor divider, to set the output voltage
value. Only an inductor and 3 capacitors are required. The current PWM mode architecture
and stable operation with low E.S.R SMD ceramic capacitors results in low, predictable
output ripple. To maximize the power conversion efficiency in light load, the regulator can
work in burst mode automatically. The device can operate in PWM mode at a fixed
frequency or synchronized to an external frequency. It switches at a frequency of 900 kHz
when SYNC is connected to ground or a fixed voltage (less than 5.5 V) and synchronizes
the switching frequency between 400 kHz to 1.2 MHz from the external clock that is applied
to SYNC. A thermal shutdown circuit is integrated and activates at 150 °C. Cycle-by-cycle
current limitation provides protection against shorted outputs. The on-chip 260 µs power-on
reset ensures the proper operation when switching on the power supply. The quiescent
current is less than 6 µA in the inhibit state. The device is available in MLP4x4 and SO-8
ePad packages.
input capacitor reduces the current peaks drawn from the input power
IN_SW
for the power supply input voltage where the
IN_SW
to supply the ST1S10 internal circuitry and
IN_A
supply and reduces switching noise in the IC. High power supply source impedance requires
larger input capacitance.
For the V
input capacitor the RMS current rating is a critical parameter that must be
IN_SW
higher than the RMS input current. The maximum RMS input current can be calculated
using the following equation:
Equation 1
2
2D
I
RMSIO
⋅
D
-------------- -–
η
where η is the expected system efficiency, D is the duty cycle and I
2
D
------ -+⋅=
η
the output DC current.
O
This function reaches its maximum value at D = 0.5 and the equivalent RMS current is equal
to IO divided by 2 (considering η= 1).
The maximum and minimum duty cycles are:
Equation 2
V
+
outVF
D
MAX
-----------------------------------=
V
–
inMINVSW
Equation 3
V
+
D
MIN
outVF
-------------------------------------=
V
–
inMAXVSW
where V
internal PDMOS. Considering the range D
I
RMS
A minimum value of 4.7 µF for the V
is the voltage drop across the internal NMOS and VSW the voltage drop across the
F
MIN
to D
following through the input capacitor.
and a 0.1 µF ceramic capacitor for the V
IN_SW
suitable in most application conditions. A 10 µF or higher ceramic capacitor for the V
and a 1 µF (V
) are advisable in case of higher power supply source impedance or where
IN_A
it is needed to have long wires between the power supply source and the V
above suggested higher input capacitors values are also advisable in case of high output
capacitive load which can impact the switching peak current drawn from the input capacitor
during the startup transient.
It is also advisable to use ceramic capacitors with a voltage rating in the range of 1.5 times
the maximum input voltage. The input capacitors should be located as close as possible to
the V
IN
pins.
Different capacitors can be considered:
●Electrolytic capacitors. These are the most commonly used because they are the least
expensive and are available with a wide range of RMS current ratings. The only
4/20Doc ID 13883 Rev 3
it is possible to determine the max
MAX
pins. The
IN
IN_A
IN_SW
are
AN2620Application information component selection
drawback is that, considering a requested ripple current rating, they are physically
larger than other capacitors.
●Ceramic capacitors. If available for the requested value and voltage rating, these
capacitors usually have a higher RMS current rating for a given physical dimension
(due to the very low ESR). The drawback is the quite high cost.
●Tantalum capacitor. Very good tantalum capacitors are becoming available, with very
low ESR and small size. The only problem is that they occasionally can burn if
subjected to very high current during the charge. So, it is better to avoid this type of
capacitor for the input filter of the device. In fact, they can be subjected to high surge
current when connected to the power supply.
1.2 Output capacitor
The output capacitor is very important in satisfying the output voltage ripple requirement.
Using a small inductor value to reduce the size of the choke is useful, but increases the
current ripple. So, to reduce the output voltage ripple, a low ESR capacitor is required.
The most important parameters for the output capacitor are the capacitance, the ESR and
the voltage rating.
The capacitance and the ESR affect the control loop stability, the output ripple voltage, and
transient response of the regulator. The ripple due to the capacitance can be calculated by
the following formula:
Equation 4
0.125 ΔISW⋅
-------------------------------- -=
F
SCout
⋅
where F
V
ripple C()
is the PWM switching frequency and ΔISW is the inductor peak-to-peak switching
S
current that can be calculated as:
Equation 5
VinV
–()
ΔI
SW
------------------------------
out
F
S
D⋅=
L⋅
where D is the duty cycle while the ripple due to the ESR is given by:
Equation 6
V
ripple ESR()ISw
ΔESR⋅=
Use the above equations to define capacitor selection range, but final values should be
verified by testing an evaluation circuit.
Lower ESR ceramic capacitors are usually advisable to reduce the output ripple voltage.
Capacitors with higher voltage ratings have lower ESR values, providing lower output ripple
voltage.
Also the capacitor ESL value impacts the output ripple voltage, but ceramic capacitors
usually have very low ESL, making ripple voltages due to the ESL negligible. In order to
reduce ripple voltages due to a parasitic inductive effect, keep the output capacitor
connection paths as short as possible.
Doc ID 13883 Rev 35/20
Application information component selectionAN2620
The ST1S10 has been designed to have the best performances with ceramic capacitors. In
typical application conditions a minimum value of 22 µF ceramic capacitor is suggested on
the output, but higher values are suitable considering that the control loop has been
designed to properly work with a natural output LC frequency given by a 3.3 µH inductor and
22 µF output capacitor in the typical application (V
=12 V, V
in
out
=5 V).
It is advisable to use ceramic capacitors with a voltage rating in the range of 1.5 times the
maximum output voltage.
1.3 Inductor
The inductor value is very important because it fixes the ripple current flowing through the
output capacitor. The ripple current is usually fixed at 20-40% of I
I
= 3 A. The inductor value is approximately obtained by the following formula:
Omax
Equation 7
–
V
inVout
L
-------------------------
T
⋅=
IΔ
on
, that is 0.6-1.2 A with
Omax
where, T
For example, with V
is the ON time of the internal switch, given by D · T.
on
= 3.3 V, Vin = 5 V and ΔIO = 0.45 A, the inductor value is about
out
2.8 µH. The peak current thought the inductor is given by:
Equation 8
IΔ
I
I
PKIO
---- -+=
2
≥
SATIPK
It can be seen that if the inductor value decreases, the peak current (that has to be lower
than the current limit of the device) increases. So, for fixed the peak current, a higher value
of the inductor allows a higher value for the output current.
The ST1S10 is designed to have maximum performance with a 3.3 µH inductor value at
900 kHz.
The peak inductor current must be designed in order to not exceed the switching current
limit.
6/20Doc ID 13883 Rev 3
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