RT8011/A
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DS8011/A-02 March 2011www.richtek.com
Soft Start and Inrush Current
Time (2.5ms/Div)
I
IN
(2A/Div)
V
LX
(5V/Div)
V
IN
= 5V, V
OUT
= 2.5V
I
OUT
= 2A
V
OUT
(2V/Div)
V
IN
(2V/Div)
Soft Start and Inrush Current
Time (2.5ms/Div)
I
IN
(2A/Div)
V
LX
(5V/Div)
V
IN
= 3.3V, V
OUT
= 2.5V
I
OUT
= 2A
V
OUT
(2V/Div)
V
IN
(2V/Div)
Power On & Inductor Current
Time (1ms/Div)
I
LX
(2A/Div)
V
LX
(5V/Div)
V
IN
= 5V, V
OUT
= 2.5V
I
OUT
= 2A
V
OUT
(2V/Div)
V
IN
(2V/Div)
Power On & Inductor Current
Time (1ms/Div)
I
LX
(2A/Div)
V
LX
(5V/Div)
V
IN
= 3.3V, V
OUT
= 2.5V
I
OUT
= 2A
V
OUT
(2V/Div)
V
IN
(2V/Div)
Power Good
Time (1ms/Div)
I
LX
(2A/Div)
V
OUT
(2V/Div)
V
IN
= 3.3V, V
OUT
= 2.5V
I
OUT
= 2A
PGOOD
(2V/Div)
V
IN
(2V/Div)
RT8011/A
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DS8011/A-02 March 2011 www.richtek.com
Application Information
The basic RT8011/A application circuit is shown in Typical
Application Circuit. External component selection is
determined by the maximum load current and begins with
the selection of the inductor value and operating frequency
followed by C
IN
and C
OUT
.
Operating Frequency
Selection of the operating frequency is a tradeoff between
efficiency and component size. High frequency operation
allows the use of smaller inductor and capacitor values.
Operation at lower frequency improves efficiency by
reducing internal gate charge and switching losses but
requires larger inductance and/or capacitance to maintain
low output ripple voltage.
The operating frequency of the RT8011/A is determined
by an external resistor that is connected between the RT
pin and ground. The value of the resistor sets the ramp
current that is used to charge and discharge an internal
timing capacitor within the oscillator. The RT resistor value
can be determined by examining the frequency vs. RT
curve. Although frequencies as high as 4MHz are possible,
the minimum on-time of the RT8011/A imposes a minimum
limit on the operating duty cycle. The minimum on-time
is typically 110ns. Therefore, the minimum duty cycle is
equal to 100 x 110ns x f(Hz).
Inductor Selection
For a given input and output voltage, the inductor value
and operating frequency determine the ripple current. The
ripple current ΔI
L
increases with higher V
IN
and decreases
with higher inductance.
Having a lower ripple current reduces the ESR losses in
the output capacitors and the output voltage ripple. Highest
efficiency operation is achieved at low frequency with small
ripple current. This, however, requires a large inductor. A
reasonable starting point for selecting the ripple current
is ΔI = 0.4(I
MAX
). The largest ripple current occurs at the
highest V
IN
. To guarantee that the ripple current stays
below a specified maximum, the inductor value should be
chosen according to the following equation :
×
=Δ
IN
OUTOUT
L
V
V
1
Lf
V
I
Δ×
=
IN(MAX)
OUT
L(MAX)
OUT
V
V
1
If
V
L
Inductor Core Selection
Once the value for L is known, the type of inductor must
be selected. High efficiency converters generally cannot
afford the core loss found in low cost powdered iron cores,
forcing the use of more expensive ferrite or mollypermalloy
cores. Actual core loss is independent of core size for a
fixed inductor value but it is very dependent on the
inductance selected. As the inductance increases, core
losses decrease. Unfortunately, increased inductance
requires more turns of wire and therefore copper losses
will increase.
Ferrite designs have very low core losses and are preferred
at high switching frequencies, so design goals can
concentrate on copper loss and preventing saturation.
Ferrite core material saturates hard, which means that
inductance collapses abruptly when the peak design
current is exceeded.
This result in an abrupt increase in inductor ripple current
and consequent output voltage ripple.
Do not allow the core to saturate!
The transition from low current operation begins when the
peak inductor current falls below the minimum peak
current. Lower inductor values result in higher ripple current
which causes this to occur at lower load currents. This
causes a dip in efficiency in the upper range of low current
operation.
Figure 5
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
0 100 200 300 400 500 600 700 800 900 100
0
R
RT
(k
)
Frequency (MHz)
R
RT
(kΩ)
1000
RT = 154k for 2MHz
RT = 332k for 1MHz
RT8011/A
12
DS8011/A-02 March 2011www.richtek.com
Figure 6. Setting the Output Voltage
+×=
R2
R1
1VV
REFOUT
RT8011/A
V
FB
GND
V
OUT
R1
R2
Using Ceramic Input and Output Capacitors
Higher values, lower cost ceramic capacitors are now
becoming available in smaller case sizes. Their high ripple
current, high voltage rating and low ESR make them ideal
for switching regulator applications. However, care must
be taken when these capacitors are used at the input and
output. When a ceramic capacitor is used at the input
and the power is supplied by a wall adapter through long
wires, a load step at the output can induce ringing at the
input, V
IN
. At best, this ringing can couple to the output
and be mistaken as loop instability. At worst, a sudden
inrush of current through the long wires can potentially
cause a voltage spike at V
IN
large enough to damage the
part.
Output Voltage Programming
The output voltage is set by an external resistive divider
according to the following equation :
where V
REF
equals to 0.8V typical.
The resistive divider allows the FB pin to sense a fraction
of the output voltage as shown in Figure 6.
C
IN
and C
OUT
Selection
The input capacitance, C
IN
, is needed to filter the
trapezoidal current at the source of the top MOSFET. To
prevent large ripple voltage, a low ESR input capacitor
sized for the maximum RMS current should be used. RMS
current is given by :
This formula has a maximum at V
IN
= 2V
OUT
, where
I
RMS
= I
OUT
/2. This simple worst-case condition is
commonly used for design because even significant
deviations do not offer much relief. Note that ripple current
ratings from capacitor manufacturers are often based on
only 2000 hours of life which makes it advisable to further
derate the capacitor, or choose a capacitor rated at a higher
temperature than required.
Several capacitors may also be paralleled to meet size or
height requirements in the design.
The selection of C
OUT
is determined by the effective series
resistance (ESR) that is required to minimize voltage ripple
and load step transients, as well as the amount of bulk
capacitance that is necessary to ensure that the control
loop is stable. Loop stability can be checked by viewing
the load transient response as described in a later section.
The output ripple, ΔV
OUT
, is determined by :
The output ripple is highest at maximum input voltage
since ΔI
L
increases with input voltage. Multiple capacitors
placed in parallel may be needed to meet the ESR and
RMS current handling requirements. Dry tantalum, special
polymer, aluminum electrolytic and ceramic capacitors are
all available in surface mount packages. Special polymer
capacitors offer very low ESR but have lower capacitance
density than other types. Tantalum capacitors have the
highest capacitance density but it is important to only
1
V
V
V
V
II
OUT
IN
IN
OUT
OUT(MAX)RMS
=
+ΔΔ
OUT
LOUT
8fC
1
ESRIV
use types that have been surge tested for use in switching
power supplies. Aluminum electrolytic capacitors have
significantly higher ESR but can be used in cost-sensitive
applications provided that consideration is given to ripple
current ratings and long term reliability. Ceramic capacitors
have excellent low ESR characteristics but can have a
high voltage coefficient and audible piezoelectric effects.
The high Q of ceramic capacitors with trace inductance
can also lead to significant ringing.
Different core materials and shapes will change the size/
current and price/current relationship of an inductor. Toroid
or shielded pot cores in ferrite or permalloy materials are
small and don't radiate energy but generally cost more
than powdered iron core inductors with similar
characteristics. The choice of which style inductor to use
mainly depends on the price vs. size requirements and
any radiated field/EMI requirements.

RT8011GQW

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Description:
IC REG BUCK ADJUSTABLE 2A 10WDFN
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New from this manufacturer.
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