Inductor operating point. This choice provides
tradeoffs between size, transient response, and effi-
ciency. Choosing higher inductance values results
in lower inductor ripple current, lower peak current,
lower switching losses, and, therefore, higher effi-
ciency at the cost of slower transient response and
larger size. Choosing lower inductance values
results in large ripple currents, smaller size, and
poorer efficiency, but have faster transient response.
Setting the Output Voltage
The MAX1961 has four output voltage presets selected
by SEL. Table 2 shows how each of the preset voltages
are selected. The MAX1962 also has four preset output
voltages, but also is adjustable down to 0.8V. To use the
preset voltages on the MAX1962, FB must be connected
to V
DD
. SEL then selects the output voltage as shown in
Table 2.
Both the MAX1960/MAX1962 feature an adjustable out-
put that can be set down to 0.8V. To set voltages greater
than 0.8V, Connect FB to a resistor-divider from the out-
put (Figures 9 and 11). Use a resistor up to 10k for R2
and select R1 according to the following equation:
where the feedback threshold, V
FB
= 0.8V, and V
OUT
is
the output voltage.
Input Voltage Range
The MAX1960/MAX1961/MAX1962 have an input volt-
age range of 2.35V to 5.5V but cannot operate at both
extremes with one application circuit. The standard
charge-pump doubler application circuit operates with
an input range of 2.7V to 5.5V (Figures 9, 10, and 11).
In order to operate down to 2.35V, the charge pump
must be configured as a tripler. This circuit, however,
limits the maximum input voltage to 3.6V. The schematic
for the tripler charge pump is shown in Figure 2. Note
that the flying capacitor between C+ and C- has been
removed and C+ is not connected.
Inductor Selection
Determine an appropriate inductor value with the fol-
lowing equation:
The inductor current ripple, LIR, is the ratio of peak-to-
peak inductor ripple current to the average continuous
inductor current. An LIR between 20% and 40% pro-
vides a good compromise between efficiency and
economy. Choose a low-loss inductor having the lowest
possible DC resistance. Ferrite core type inductors are
often the best choice for performance. The inductor
saturation current rating must exceed I
PEAK
:
Setting the Current Limit
Lossless Current Limit (MAX1960/MAX1961)
The MAX1960/MAX1961 use the low-side MOSFET’s on-
resistance (R
DS(ON)
) for current sensing. This method of
current limit sets the maximum value of the inductor’s
“valley” current (Figure 3). If the inductor current is higher
than the valley current-limit setting at the end of the
clock period, the controller skips the DH pulse. When
the first current-limit event is detected, the controller initi-
II
LIR
I
PEAK LOAD MAX LOAD MAX
() ()
=+
×
2
RR
V
V
OUT
FB
12 1
-
MAX1960/MAX1961/MAX1962
2.35V to 5.5V, 0.5% Accurate, 1MHz PWM
Step-Down Controllers with Voltage Margining
______________________________________________________________________________________ 13
PRESET OUTPUT VOLTAGE SEL
1.5V GND
1.8V REF
2.5V No connection
3.3V V
DD
Table 2. Preset Voltages—
MAX1961/MAX1962
MAX1960/
MAX1961/
MAX1962
C10
C11
C12
C6
D2
D3 D4 D5
R5
10
C4
1µF
V
CC
C-
C+
V
DD
AV
DD
C10, C11, C12
C6
500kHz
1µF
4.7µF
1MHz
0.47µF
2.2µF
Figure 2. Tripler Charge-Pump Configuration.
MAX1960/MAX1961/MAX1962
ates a 128 clock cycle counter. If the current limit is pre-
sent at the end of this count, the controller remains off
until the input voltage is removed and re-applied, or the
device is re-enabled with CTL1 and CTL2. The 128-cycle
counter is reset when four successive DH pulses are
observed, without activating the current limit.
At maximum load, the low excursion of inductor current,
I
VALLEY(MAX)
, is:
The current-limit threshold (V
CLT
) is set by connecting a
resistor (R
ILIM
) from ILIM to GND. The range for this
resistor is 100k to 400k. Set current-limit threshold as
follows:
V
CLT
= R
ILIM
× 0.714µA
Connecting ILIM to V
DD
sets the threshold to a default
value of 75mV.
To prevent the current limit from falsely triggering, V
CLT
divided by the low-side MOSFET R
DS(ON)
must exceed
the maximum value of I
VALLEY
. The maximum value of
low-side MOSFET R
DS(ON)
should be used:
V
CLT
> R
DS(ON)MAX
x I
VALLEY(MAX)
A limitation of sensing current across MOSFET on-resis-
tance is that the MOSFET on-resistance varies signifi-
cantly from MOSFET to MOSFET and over temperature.
Consequently, this current-sensing method may not be
suitable if a precise current limit is required. If better
accuracy is needed, use the MAX1962 with a current-
sense resistor.
Current-Sense Resistor (MAX1962)
The MAX1962 uses a current-sense resistor connected
from the inductor to the output with Kelvin sense connec-
tions. The current-sense voltage is measured from CS to
OUT, and has a fixed threshold of 50mV. The MAX1962
current limit is triggered when the peak voltage across
the current-sense resistor, I
PEAK
× R
SENSE
, exceeds
50mV. Once current sense is triggered, the controller
does not turn off, but continues to operate at the current
limit. This method of current sensing is more precise due
to the accuracy of the current-sense resistor. The cost of
this precision is that it requires an extra component and
is slightly less efficient due to the loss in the current-
sense resistance.
Inductor Resistance Current Sense (MAX1962)
Alternately, the inductor resistance can be used to
sense current in place of a current-sense resistor. To
do this, connect a series RC network in parallel with the
inductor (Figure 4). Choose a resistor value less than
40 to avoid offsets due to CS input current. Calculate
the capacitor value from the formula C = 2L / (R
L
× R).
The effective current-sense resistance (R
SENSE
) equals
R
L
. Current-sense accuracy then depends on the accu-
racy of the inductor resistance. Note that the current-
sense signal is delayed due to the RC filter time
constant. Consequently, inductor current may over-
shoot (by as much as 2x) when a fast short occurs.
II
LIR
I
VALLEY MAX LOAD MAX LOAD MAX() () ()
=
×-
2
2.35V to 5.5V, 0.5% Accurate, 1MHz PWM
Step-Down Controllers with Voltage Margining
14 ______________________________________________________________________________________
I
PEAK
I
LOAD
I
VALLEY
INDUCTOR CURRENT
TIME
Figure 3. Inductor Current Waveform
DH
L
R
L
R
R = 33
0.22µH, 2.8mW,
I
LIMIT
= 18A
C
C = 4.7µF
LX
DL
CS
OUT
MAX1962
Figure 4. Using the Inductor Resistance as a Current-Sense
Resistor with the MAX1962
Output Capacitor Selection
The output filter capacitor must have low enough effective
series resistance (ESR) to meet output ripple and load
transient requirements. In addition, the capacitance value
must be high enough to absorb the inductor energy
during load steps.
In applications where the output is subject to large load
transients, low ESR is needed to prevent the output
from dipping too low (V
DIP
) during a load step:
In applications with less severe load steps, maximum
ESR may be governed by what is needed to maintain
acceptable output voltage ripple:
To satisfy both load step and ripple requirements,
select the lowest value from the above two equations.
The capacitor is usually selected by physical size, ESR,
and voltage rating, rather than by capacitance value.
With current tantalum, electrolytic, and polymer capaci-
tor technology, the bulk capacitance will also be suffi-
cient once the ESR requirement is satisfied.
When using low-capacity filter capacitors such as
ceramic, capacitor size is usually determined by the
capacitance needed to prevent voltage undershoot
and overshoot during load transients. The overshoot
voltage (V
SOAR
) is given by:
Generally, once enough capacitance is in place to meet
the overshoot requirement, undershoot at the rising load
edge is no longer a problem.
Input Capacitor Selection
The input capacitor (C
IN
) reduces the current peaks
drawn from the input supply and reduces noise injec-
tion. The source impedance to the input supply largely
determines the value of C
IN
. High source impedance
requires high input capacitance. The input capacitor
must meet the ripple current requirement (I
RMS
)
imposed by the switching currents.
The RMS input ripple current is given by:
For optimal circuit reliability, choose a capacitor that
has less than 10°C temperature rise at the peak ripple
current.
Compensation and Stability
Compensation with Ceramic Output Capacitors
The high switching frequency range of the
MAX1960/MAX1961/MAX1962 allows the use of ceramic
output capacitors. Since the ESR of ceramic capacitors
is very low typically, the frequency of the associated
transfer function zero is higher than the unity-gain
crossover frequency and the zero cannot be used to
compensate for the double pole created by the output
inductor and capacitor. The solution is Type 3 compen-
sation (Figure 5), which takes advantage of local feed-
back to create two zeros and three poles (Figure 6). The
frequency of the poles and zeros are described below:
Unity-gain crossover frequency:
fR C
V
VLC
IN MAX
RAMP
0
00
13
1
2
× ×
××
()
π
f
RC
ZESR
ESR
=
××
1
2
0
π
f
RR C
Z2
1
2233
=
×+×π ()
f
RC
Z1
1
211
=
××π
f
LC
LC
=
×
1
2
00
π
f
R
CC
CC
P3
1
21
12
12
=
××
×
+
π
f
RC
P2
1
223
=
××π
f
P1
0=
II
VVV
V
RMS LOAD
OUT IN OUT
IN
× ()-
V
LI
VC
SOAR
PEAK
OUT OUT
=
×
()
××
2
2
R
V
LIR I
ESR
RIPPLE P P
LOAD MAX
×
()
()
R
V
I
ESR
DIP
LOADSTEP MAX
()
MAX1960/MAX1961/MAX1962
2.35V to 5.5V, 0.5% Accurate, 1MHz PWM
Step-Down Controllers with Voltage Margining
______________________________________________________________________________________ 15

MAX1960EEP+

Mfr. #:
Manufacturer:
Maxim Integrated
Description:
Switching Controllers 1MHz PWM Step-Down
Lifecycle:
New from this manufacturer.
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