RT8012A
10
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Switching Frequency vs. Temperature
1000
1050
1100
1150
1200
1250
1300
1350
1400
-50 -25 0 25 50 75 100 125
Temperature
Frequency (kHz)
V
IN
= 5V, V
OUT
= 1.2V, I
OUT
= 300mA
(°C)
Switching Frequency vs. Input Voltage
1000
1050
1100
1150
1200
1250
1300
1350
1400
2.5 3 3.5 4 4.5 5 5.5
Input Voltage (V)
Frequency (kHz)
V
OUT
= 1.2V, I
OUT
= 300mA
Regulator 1 Inductor Peak Current vs. Input Voltage
1.3
1.4
1.5
1.6
1.7
1.8
1.9
2.0
2.1
2.2
2.3
4 4.3 4.6 4.9 5.2 5.5
Input Voltage (V)
Inductor Peak Current (A)
V
OUT
= 3.3V
Regulator 2 Inductor Peak Current vs. Input Voltage
2.0
2.1
2.2
2.3
2.4
2.5
2.6
2.7
2.8
2.9
3.0
2.533.544.555.5
Input Voltage (V)
Inductor Peak Current (A)
V
OUT
= 1.2V
Regulator 2 Current Limit vs. Temperature
1.5
1.6
1.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
-50 -25 0 25 50 75 100 125
Temperature
Output Current (A
)
V
IN
= 5V, V
OUT
= 1.2V
(°C)
Regulator 1 Current Limit vs. Temperature
1.0
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
-50 -25 0 25 50 75 100 125
Temperature
Output Current (A
)
V
IN
= 5V, V
OUT
= 3.3V
(°C)
RT8012A
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+
OUT
LOUT
8fC
1
ESR ΔIΔV
Applications Information
The basic RT8012A 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
.
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
L
= 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 :
×
×
=
IN
OUTOUT
L
V
V
1
Lf
V
ΔI
×
Δ×
=
IN(MAX)
OUT
L(MAX)
OUT
V
V
1
If
V
L
1
V
V
V
V
II
OUT
IN
IN
OUT
OUT(MAX)RMS
=
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 :
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 molypermalloy
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 results in an abrupt increase in
inductor ripple current and consequent output voltage ripple.
Do not allow the core to saturate!
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. However, they are
usually more expensive than the similar powered iron
inductors. The choice of which style inductor to use mainly
depends on the price vs size requirements and any radiated
field/EMI requirements.
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 :
RT8012A
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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
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.
Selecting 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 resistive divider allows the FB pin to sense a fraction
of the output voltage as shown in Figure 3.
)
R2
R1
(1VV
REFOUT
+=
Figure 3. Setting the Output Voltage
where V
REF
is the internal reference voltage (0.8V typ.)
For adjustable voltage mode, the output voltage is set by
an external resistive divider according to the following
equation :
Efficiency Considerations
The efficiency of a switching regulator is equal to the output
power divided by the input power times 100%. It is often
useful to analyze individual losses to determine what is
limiting the efficiency and which change would produce
the most improvement. Efficiency can be expressed as :
Efficiency = 100% (L1+ L2+ L3+ ...)
where L1, L2, etc. are the individual losses as a percentage
of input power. Although all dissipative elements in the
circuit produce losses, two main sources usually account
for most of the losses : VIN quiescent current and I
2
R
losses.
The VIN quiescent current loss dominates the efficiency
loss at very low load currents whereas the I
2
R loss
dominates the efficiency loss at medium to high load
currents. In a typical efficiency plot, the efficiency curve
at very low load currents can be misleading since the
actual power lost is of no consequence.
1. The VIN quiescent current appears due to two factors
including the DC bias current as given in the electrical
characteristics and the internal main switch and
synchronous switch gate charge currents. The gate charge
current results from switching the gate capacitance of the
internal power MOSFET switches. Each time the gate is
switched from high to low to high again, a packet of charge
ΔQ moves from V
IN
to ground.
The resulting ΔQ/Δt is the current out of V
IN
that is typically
larger than the DC bias current. In continuous mode,
I
GATECHG
= f(Q
T
+Q
B
)
where Q
T
and Q
B
are the gate charges of the internal top
and bottom switches. Both the DC bias and gate charge
losses are proportional to V
IN
and thus their effects will
be more pronounced at higher supply voltages.
2. I
2
R losses are calculated from the resistances of the
internal switches, R
SW
and external inductor R
L
. In
continuous mode, the average output current flowing
RT8012A
GND
FB
R1
R2
V
OUT

RT8012AGQW

Mfr. #:
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Description:
IC REG BCK ADJ 1A/1.5A DL 16WQFN
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