
Application Information
The MIC23158/9 is a high-performance DC/DC step
down regu lator offer ing a sm all solution size. Supporting
two outputs of up to 2A each in a 3mm x 4mm MLF
package. Using the HyperLight Load switching scheme,
the MIC23158/9 is able to maintain high efficiency
throughout the entire load range while providing ultra
fast load transient response. The following sections
provide addit ion al de vice appl icati on inf or mation.
Input Capacitor
A 2.2µF ceramic capacitor or greater should be placed
close to the VIN pin and PGND pin for bypassing. A
Murata GRM188R60J475KE19D, size 0603, 4.7µF
ceramic capacitor is recommended based upon
performance, size and cost. A X5R or X7R temperature
rating is recommended for the input capacitor.
Output Capacitor
The MIC23158/9 is designed for use with a 2.2µF or
greater ceramic output capacitor. Increasing the output
capacitance will lower output ripple and improve load
transient response but could also increase solution size
or cost. A low equivalent series resistance (ESR)
ceramic output capacitor such as the Murata
GRM188R60J475KE19D, size 0603, 4.7µF ceramic
capacitor is recommended based upon performance,
size and cost. Both the X7R or X5R temperature rating
capacitors are recommended.
Inductor Selection
When selecting an inductor, it is important to consider
the following factors:
• Inductance
• Rated current value
• Size requirements
• DC resistance (DCR)
The MIC23158/9 is designed for use with a 0.47µH to
2.2µH inductor. For faster transient response, a 0.47µH
inductor will yield the best result. F or lower o utput rippl e,
a 2.2µH inductor is recommended.
Maximum current ratings of the inductor are generally
given in two methods; permissible DC current, and
saturation current. Permissible DC current can be rated
either for a 40°C temperature rise or a 10% to 20% loss
in inductance. Ensure the inductor selected can handle
the max imum operating c urrent. When saturation cur re nt
is specified, make sure that there is enough margin so
that the peak current does not cause the inductor to
saturate.
Peak current can be calculated in Equation 2:
×
×
−
+
=L
f2 /VV
1
V
II IN
OUT
OUT
OUTPEAK
Eq. 2
As shown by the calculation above, the peak inductor
current is inversely proportional to the switching
frequency and the inductance. The lower the switching
frequenc y or inducta nce, th e higher the peak current. As
input voltage increases, the peak current also increases.
The size of the inductor de pends on the requ irements of
the application. Refer to the typical application circuit
and Bill o f Ma teria ls for details.
Figure 3. Transition between CCM Mode to HLL Mode
DC resistance (DCR) is also important. While DCR is
inversely proportional to size, DCR can represent a
significant efficiency loss. Refer to the “Efficiency
Considerations” subsection.
The transition between continuous conduction mode
(CCM) to HyperLight Load mode is determined by the
inductor ripple current and the load current.
The diagram shows the sig nals f or high-side switch drive
(HSD) for TON control, the Inductor current, and the low-
side switch drive (LSD) for TOFF control.
In HLL mode, the inductor is charged with a fixed TON
pulse on the high side switch. After this, the low side
switch is turned o n a nd c urrent f alls at a rate V OUT/L. The
controller remains in HLL m ode while the induct or falling
current is detec ted to cross approximatel y -5 0m A. When
the LSD (or TOFF) time reaches its minimum and the
inductor falling current is no longer able to reach the
threshold, the part is in CCM mode.