MAX1846/MAX1847
High-Efficiency, Current-Mode,
Inverting PWM Controller
______________________________________________________________________________________ 13
2) Higher frequencies allow the use of smaller value
(hence smaller size) inductors and capacitors.
3) Higher frequencies consume more operating
power both to operate the IC and to charge and
discharge the gate at the external FET, which
tends to reduce the efficiency at light loads.
4) Higher frequencies may exhibit lower overall effi-
ciency due to more transition losses in the FET;
however, this shortcoming can often be nullified
by trading some of the inductor and capacitor size
benefits for lower-resistance components.
5) High-duty-cycle applications may require lower
frequencies to accommodate the controller mini-
mum off-time of 0.4µs. Calculate the maximum
oscillator frequency with the following formula:
Remember that V
OUT
is negative when using this formula.
When running at the maximum oscillator frequency
(f
OSCILLATOR
) and maximum duty cycle (D
MAX
), do not
exceed the minimum value of D
MAX
stated in the
Electrical Characteristics
table. For designs that
exceed the D
MAX
and f
OSC(MAX)
, an autotransformer
can reduce the duty cycle and allow higher operating
frequencies.
The oscillator frequency is set by a resistor, RFREQ,
which is connected from FREQ to GND. The relation-
ship between fOSC (in Hz) and RFREQ (in ) is slightly
nonlinear, as illustrated in the Typical Operating
Characteristics. Choose the resistor value from the
graph and check the oscillator frequency using the fol-
lowing formula:
External Synchronization (MAX1847 only)
The SYNC input provides external-clock synchroniza-
tion (if desired). When SYNC is driven with an external
clock, the frequency of the clock directly sets the
MAX1847’s switching frequency. A rising clock edge
on SYNC is interpreted as a synchronization input. If
the sync signal is lost, the internal oscillator takes over
at the end of the last cycle, and the frequency is
returned to the rate set by R
FREQ
. Choose R
FREQ
such
that f
OSC
= 0.9 x f
SYNC
.
Choosing Inductance Value
The inductance value determines the operation of the
current-mode regulator. Except for low-current applica-
tions, most circuits are more efficient and economical
operating in continuous mode, which refers to continu-
ous current in the inductor. In continuous mode there is
a trade-off between efficiency and transient response.
Higher inductance means lower inductor ripple current,
lower peak current, lower switching losses, and, there-
fore, higher efficiency. Lower inductance means higher
inductor ripple current and faster transient response. A
reasonable compromise is to choose the ratio of induc-
tor ripple current to average continuous current at mini-
mum duty cycle to be 0.4. Calculate the inductor ripple
with the following formula:
Then calculate an inductance value:
L = (V
IN(MAX)
/ I
RIPPLE
) x (D
MIN
/ f
OSC
)
Choose the closest standard value. Once again, remem-
ber that V
OUT
is negative when using this formula.
Determining Peak Inductor Current
The peak inductor current required for a particular out-
put is:
I
LPEAK
= I
LDC
+ (I
LPP
/ 2)
where I
LDC
is the average DC inductor current and I
LPP
is the inductor peak-to-peak ripple current. The I
LDC
and I
LPP
terms are determined as follows:
where L is the selected inductance value. The satura-
tion rating of the selected inductor should meet or
exceed the calculated value for I
LPEAK
, although most
coil types can be operated up to 20% over their satura-
tion rating without difficulty. In addition to the saturation
criteria, the inductor should have as low a series resis-
I
I
D
I
VVVxD
Lxf
LDC
LOAD
MAX
LPP
IN MIN SW LIM MAX
OSC
=
()
=
−−
()
()
1
I
IVVVVV
VVV
RIPPLE
LOAD MAX IN MAX SW LIM OUT D
IN MAX SW LIM
=
×× +
()
()
−−
−−
04.
() ()
()
f
RR
OSC
FREQ FREQ
=
×
()
()
××
()
×
()
−−
1
5 21 10 1 92 10 4 86 10
711 19
2
. . .
f
VVV
VVVVV
t
OSC MAX
IN MIN SW LIM
IN MIN SW LIM OUT D
OFF MIN
()
()
()
()
=
+
×
−−
−−
1
MAX1846/MAX1847
High-Efficiency, Current-Mode,
Inverting PWM Controller
14 ______________________________________________________________________________________
tance as possible. For continuous inductor current, the
power loss in the inductor resistance (P
LR
) is approxi-
mated by:
where R
L
is the inductor series resistance.
Once the peak inductor current is calculated, the cur-
rent sense resistor, R
CS
, is determined by:
R
CS
= 85mV / I
LPEAK
For high peak inductor currents (>1A), Kelvin-sensing
connections should be used to connect CS and PGND
to R
CS
. Connect PGND and GND together at the
ground side of R
CS
. A lowpass filter between R
CS
and
CS may be required to prevent switching noise from
tripping the current-sense comparator at heavy loads.
Connect a 100 resistor between CS and the high side
of R
CS
, and connect a 1000pF capacitor between CS
and GND.
Checking Slope-Compensation Stability
In a current-mode regulator, the cycle-by-cycle stability
is dependent on slope compensation to prevent sub-
harmonic oscillation at duty cycles greater than 50%.
For the MAX1846/MAX1847, the internal slope compen-
sation is optimized for a minimum inductor value (L
MIN
)
with respect to duty cycle. For duty cycles greater then
50%, check stability by calculating LMIN using the fol-
lowing equation:
where V
IN(MIN)
is the minimum expected input voltage,
M
s
is the Slope Compensation Ramp (41 mV/µs) and
D
MAX
is the maximum expected duty cycle. If L
MIN
is
larger than L, increase the value of L to the next stan-
dard value that is larger than L
MIN
to ensure slope
compensation stability.
Choosing the Inductor Core
Choosing the most cost-effective inductor usually
requires optimizing the field and flux with size. With
higher output voltages the inductor may require many
turns, and this can drive the cost up. Choosing an
inductor value at L
MIN
can provide a good solution if
discontinuous inductor current can be tolerated.
Powdered iron cores can provide the most economical
solution but are larger in size than ferrite.
Power MOSFET Selection
The MAX1846/MAX1847 drive a wide variety of P-chan-
nel power MOSFETs (PFETs). The best performance,
especially with input voltages below 5V, is achieved
with low-threshold PFETs that specify on-resistance
with a gate-to-source voltage (V
GS
) of 2.7V or less.
When selecting a PFET, key parameters include:
Total gate charge (Q
G
)
Reverse transfer capacitance (C
RSS
)
On-resistance (R
DS(ON)
)
Maximum drain-to-source voltage (V
DS(MAX)
)
Minimum threshold voltage (V
TH(MIN)
)
At high-switching rates, dynamic characteristics (para-
meters 1 and 2 above) that predict switching losses
may have more impact on efficiency than R
DS(ON
),
which predicts DC losses. Q
G
includes all capacitance
associated with charging the gate. In addition, this
parameter helps predict the current needed to drive the
gate at the selected operating frequency. The power
MOSFET in an inverting converter must have a high
enough voltage rating to handle the input voltage plus
the magnitude of the output voltage and any spikes
induced by leakage inductance and ringing.
An RC snubber circuit across the drain to ground might
be required to reduce the peak ringing and noise.
Choose R
DS(ON)(MAX)
specified at V
GS
< V
IN(MIN)
to be
one to two times R
CS
. Verify that V
IN(MAX)
< V
GS(MAX)
and V
DS(MAX)
> V
IN(MAX)
- V
OUT
+ V
D
. Choose the rise-
and fall-times (t
R
, t
F
) to be less than 50ns.
Output Capacitor Selection
The output capacitor (C
OUT
) does all the filtering in an
inverting converter. The output ripple is created by the
variations in the charge stored in the output capacitor
with each pulse and the voltage drop across the
capacitor’s equivalent series resistance (ESR) caused
by the current into and out of the capacitor. There are
two properties of the output capacitor that affect ripple
voltage: the capacitance value, and the capacitor’s
ESR. The output ripple due to the output capacitor’s
value is given by:
V
RIPPLE-C
= (I
LOAD
D
MAX
T
OSC
) / C
OUT
The output ripple due to the output capacitor’s ESR is
given by:
V
RIPPLE-R
= I
LPP
R
ESR
These two ripple voltages are additive and the total out-
put ripple is:
V
RIPPLE-T
= V
RIPPLE-C
+ V
RIPPLE-R
LVxRM
xxD D
MIN IN MIN CS S
MAX MAX
=
()
()()
−−
()
/
/211
PRx
I
ID
LR L
LOAD
MAX
~
2
MAX1846/MAX1847
High-Efficiency, Current-Mode,
Inverting PWM Controller
______________________________________________________________________________________ 15
The ESR-induced ripple usually dominates this last
equation, so typically output capacitor selection is
based mostly upon the capacitor’s ESR, voltage rating,
and ripple current rating. Use the following formula to
determine the maximum ESR for a desired output ripple
voltage (V
RIPPLE-D
):
R
ESR
= V
RIPPLE-D
/ I
L
PP
Select a capacitor with ESR rating less than R
ESR
. The
value of this capacitor is highly dependent on dielectric
type, package size, and voltage rating. In general, when
choosing a capacitor, it is recommended to use low-ESR
capacitor types such as ceramic, organic, or tantalum
capacitors. Ensure that the selected capacitor has suffi-
cient margin to safely handle the maximum RMS ripple
current.
For continuous inductor current the maximum RMS ripple
current in the output filter capacitor is:
Choosing Compensation Components
The MAX1846/MAX1847 are externally loop-compen-
sated devices. This feature provides flexibility in
designs to accommodate a variety of applications.
Proper compensation of the control loop is important to
prevent excessive output ripple and poor efficiency
caused by instability. The goal of compensation is to
cancel unwanted poles and zeros in the DC-DC con-
verter’s transfer function created by the power-switch-
ing and filter elements. More precisely, the objective of
compensation is to ensure stability by ensuring that the
DC-DC converter’s phase shift is less than 180° by a
safe margin, at the frequency where the loop gain falls
below unity. One method for ensuring adequate phase
margin is to introduce corresponding zeros and poles
in the feedback network to approximate a single-pole
response with a -20dB/decade slope all the way to
unity-gain crossover.
Calculating Poles and Zeros
The MAX1846/MAX1847 current-mode architecture
takes the double pole caused by the inductor and out-
put capacitor and shifts one of these poles to a much
higher frequency to make loop compensation easier.
To compensate these devices, we must know the cen-
ter frequencies of the right-half plane zero (z
RHP
) and
the higher frequency pole (p
OUT2
). Calculate the z
RHP
frequency with the following formula:
The calculations for p
OUT2
are very complex. For most
applications where V
OUT
does not exceed -48V (in a
negative sense), the p
OUT2
will not be lower than 1/8th
of the oscillator frequency and is generally at a higher
frequency than z
RHP
. Therefore:
p
OUT2
0.125
f
OSC
A pole is created by the output capacitor and the load
resistance. This pole must also be compensated and
its center frequency is given by the formula:
p
OUT1
= 1 / (2π
R
LOAD
C
OUT
)
Finally, there is a zero introduced by the ESR of the out-
put capacitor. This zero is determined from the follow-
ing equation:
z
ESR
= 1 / (2π
C
OUT
R
ESR
)
Calculating the Required Pole Frequency
To ensure stability of the MAX1846/MAX1847, the gain
of the error amplifier must roll-off the total loop gain to 1
before Z
RHP
or P
OUT2
occurs. First, calculate the DC
open-loop gain, A
DC
:
where:
A
CS
is the current sense amplifier gain = 3.3
B is the feedback-divider attenuation factor =
G
M
is the error-amplifier transconductance =
400 µA/V
R
O
is the error-amplifier output resistance = 3 M
R
CS
is the selected current-sense resistor
Determining the Compensation Component Values
Select a unity-gain crossover frequency (f
CROS
), which
is lower than z
RHP
and p
OUT2
and higher than p
OUT1
.
Using f
CROS
, calculate the compensation resistor
(R
COMP
).
R
fxR
AxP f
COMP
CROS O
DC OUT CROS
=
1
R
RR
2
12+
A
BxG R D R
AxR
DC
M O MAX LOAD
CS CS
xx
=
()1
Z
DxV VxR
xV L
RHP
MAX IN MIN OUT LOAD
OUT
=
−−
()
()
×
()
1
2
2
()
π
I
I
ID
xD D
RMS
LOAD
MAX
MAX MAX
=
2

MAX1846EUB+

Mfr. #:
Manufacturer:
Maxim Integrated
Description:
Switching Controllers Current-Mode Invert PWM Controller
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