The A5972D is a step down monolithic power
switching regulator with a minimum switch current
limit of 1.8 A so it is able to deliver up to 1.5 A DC
current to the load depending on the application
conditions. The output voltage can be set from
1.235 V to V
The device uses an internal p-channel DMOS
transistor (with a typical R
switching element to minimize the size of the
external components.
An internal oscillator fixes the switching frequency
at 250 kHz. Having a minimum input voltage of
4 V only it fits the automotive applications
requiring the device operation even in cold crank
conditions. Pulse by pulse current limit with the
internal frequency modulation offers an effective
constant current short circuit protection.
Feedback input. Connecting directly to this pin results in an output
5FB
8VCCUnregulated DC input voltage.
voltage of 1.23 V. An external resistive divider is required for higher
output voltages.
4/37Doc ID 13956 Rev 5
A5972DElectrical data
2 Electrical data
2.1 Maximum ratings
Table 2.Absolute maximum ratings
SymbolParameterValueUnit
V
8
V
1
I
1
V
, V
4
P
TOT
T
J
T
STG
Input voltage40V
OUT pin DC voltage
OUT pin peak voltage at Δt = 0.1 μs
Maximum output currentint. limit.
Analog pins4V
5
Power dissipation at T
Operating junction temperature range-40 to 150°C
Storage temperature range-55 to 150°C
2.2 Thermal data
Table 3.Thermal data
SymbolParameterValueUnit
R
thJA
1. Package mounted on evaluation board
Maximum thermal resistance junction-ambient65
-1 to 40
-5 to 40
≤ 70 °C1.2W
A
(1)
V
V
°C/W
Doc ID 13956 Rev 55/37
Electrical characteristicsA5972D
3 Electrical characteristics
TJ = -40 °C to 125 °C, VCC = 12 V, unless otherwise specified.
Table 4.Electrical characteristics
SymbolParameterTest conditionMinTypMaxUnit
V
R
DS(on)
f
CC
I
SW
Operating input
voltage range
Mosfet on resistance0.2500.5Ω
Maximum limiting
L
current
(1)
V
CC
V
CC
Switching frequency212250280kHz
Duty cycle0100%
Dynamic characteristics (see test circuit)
V
ηEfficiencyV
Voltage feedback4.4 V < V
5
= 5 V, V
0
DC characteristics
I
qop
I
Total operating
quiescent current
Quiescent currentDuty cycle = 0; VFB= 1.5 V2.5mA
q
Error amplifier
V
OH
V
High level output
voltage
Low level output
OL
voltage
V
FB
V
FB
436V
= 5 V1.82.53
= 5 V, TJ = 25 °C22.53
< 36 V, 1.1981.2351.272V
CC
= 12 V90%
CC
35mA
= 1 V3.5V
= 1.5 V0.4V
A
V
= 1.9 V;
I
o source
I
o sink
I
Source output current
Sink output current
bSource bias current2.54μA
DC open loop gainR
gmTransconductance
1. With TJ = 85 °C, I
= 2 A, assured by design, characterization and statistical correlation.
lim_min
COMP
V
= 1 V
FB
V
= 1.9 V;
COMP
V
= 1.5 V
FB
L=5065dB
8
I
= -0.1 mA to 0.1 mA;
COMP
V
= 1.9 V
COMP
6/37Doc ID 13956 Rev 5
190300μA
11.5mA
2.3mS
A5972DDatasheet parameters over the temperature range
4 Datasheet parameters over the temperature range
The 100% of the population in the production flow is tested at three different ambient
temperatures (-40 °C; +25 °C, +125 °C) to guarantee the datasheet parameters inside the
junction temperature range (-40 °C; +125 °C).
The device operation is so guaranteed when the junction temperature is inside the (-40 °C;
+150 °C) temperature range. The designer can estimate the silicon temperature increase
respect to the ambient temperature evaluating the internal power losses generated during
the device operation (please refer to the Chapter 2.2).
However the embedded thermal protection disables the switching activity to protect the
device in case the junction temperature reaches the T
temperature.
All the datasheet parameters can be guaranteed to a maximum junction temperature of
+125 °C to avoid triggering the thermal shutdown protection during the testing phase
because of self heating.
SHTDWN
(+150 °C±10 °C)
Doc ID 13956 Rev 57/37
Functional descriptionA5972D
5 Functional description
The main internal blocks are shown in the device block diagram in Figure 3. They are:
●A voltage monitor circuit which checks the input and the internal voltages.
●A fully integrated sawtooth oscillator with a frequency of 250 kHz ± 15%, including also
the voltage feed forward function and an input/output synchronization pin.
●Two embedded current limitation circuits which control the current that flows through
the power switch. The pulse-by-pulse current limit forces the power switch OFF cycle
by cycle if the current reaches an internal threshold, while the frequency shifter reduces
the switching frequency in order to significantly reduce the duty cycle.
●A transconductance error amplifier.
●A pulse width modulator (PWM) comparator and the relative logic circuitry necessary to
drive the internal power.
●A high side driver for the internal P-MOS switch.
●A circuit to implement the thermal protection function.
Figure 3.Block diagram
5.1 Power supply
The internal regulator circuit (shown in Figure 4) consists of a start-up circuit, an internal
voltage pre-regulator, the Bandgap voltage reference and the Bias block that provides
current to all the blocks. The Starter supplies the start-up currents to the entire device when
the input voltage goes high and the device is enabled (inhibit pin connected to ground). The
pre-regulator block supplies the Bandgap cell with a pre-regulated voltage V
very low supply voltage noise sensitivity.
8/37Doc ID 13956 Rev 5
that has a
REG
A5972DFunctional description
5.2 Voltages monitor
An internal block continuously senses the Vcc, V
their thresholds, the regulator begins operating. There is also a hysteresis on the V
(UVLO).
Figure 4.Internal circuit
5.3 Current protection
The A5972D features two types of current limit protection: pulse-by-pulse and frequency
foldback.
The schematic of the current limitation circuitry for the pulse-by-pulse protection is shown in
Figure 5. The output power PDMOS transistor is split into two parallel PDMOS transistors.
The smallest one includes a resistor in series, R
R
switched off until the next falling edge of the internal clock pulse. Due to this reduction of the
ON time, the output voltage decreases. Since the minimum switch ON time necessary to
sense the current in order to avoid a false overcurrent signal is too short to obtain a
sufficiently low duty cycle at 250 kHz (see Chapter 8.4), the output current in strong
overcurrent or short circuit conditions could be not properly limited. For this reason the
switching frequency is also reduced, thus keeping the inductor current under its maximum
threshold. The frequency shifter (Figure 5) functions based on the feedback voltage. As the
feedback voltage decreases (due to the reduced duty cycle), the switching frequency
decreases also.
and if it reaches the threshold, the mirror becomes unbalanced and the PDMOS is
SENSE
and Vbg. If the voltages go higher than
ref
CC
. The current is sensed through
SENSE
Doc ID 13956 Rev 59/37
Functional descriptionA5972D
Figure 5.Current limitation circuitry
5.4 Error amplifier
The voltage error amplifier is the core of the loop regulation. It is a transconductance
operational amplifier whose non inverting input is connected to the internal voltage
reference (1.235 V), while the inverting input (FB) is connected to the external divider or
directly to the output voltage. The output (COMP) is connected to the external compensation
network. The uncompensated error amplifier has the following characteristics:
The error amplifier output is compared to the oscillator sawtooth to perform PWM control.
5.5 PWM comparator and power stage
This block compares the oscillator sawtooth and the error amplifier output signals to
generate the PWM signal for the driving stage.
The power stage is a highly critical block, as it functions to guarantee a correct turn ON and
turn OFF of the PDMOS. The turn ON of the power element, or more accurately, the rise
time of the current at turn ON, is a very critical parameter. At a first approach, it appears that
the faster the rise time, the lower the turn ON losses.
However, there is a limit introduced by the recovery time of the recirculation diode.
In fact, when the current of the power element is equal to the inductor current, the diode
turns OFF and the drain of the power is able to go high. But during its recovery time, the
10/37Doc ID 13956 Rev 5
A5972DFunctional description
diode can be considered a high value capacitor and this produces a very high peak current,
responsible for numerous problems:
●Spikes on the device supply voltage that cause oscillations (and thus noise) due to the
board parasites.
●Turn ON overcurrent leads to a decrease in the efficiency and system reliability.
●Major EMI problems.
●Shorter freewheeling diode life.
The fall time of the current during turn OFF is also critical, as it produces voltage spikes (due
to the parasites elements of the board) that increase the voltage drop across the PDMOS.
In order to minimize these problems, a new driving circuit topology has been used and the
block diagram is shown in Figure 6. The basic idea is to change the current levels used to
turn the power switch ON and OFF, based on the PDMOS and the gate clamp status.
This circuitry allows the power switch to be turned OFF and ON quickly and addresses the
freewheeling diode recovery time problem. The gate clamp is necessary to ensure that V
of the internal switch does not go higher than V
max. The ON/OFF Control block protects
GS
GS
against any cross conduction between the supply line and ground.
Figure 6.Driving circuitry
5.6 Thermal shutdown
The shutdown block generates a signal that turns OFF the power stage if the temperature of
the chip goes higher than a fixed internal threshold (150±10 °C). The sensing element of the
chip is very close to the PDMOS area, ensuring fast and accurate temperature detection. A
hysteresis of approximately 20 °C keeps the device from turning ON and OFF continuously.
Doc ID 13956 Rev 511/37
Additional features and protectionA5972D
6 Additional features and protection
6.1 Feedback disconnection
If the feedback is disconnected, the duty cycle increases towards the maximum allowed
value, bringing the output voltage close to the input supply. This condition could destroy the
load.
To avoid this hazardous condition, the device is turned OFF if the feedback pin is left
floating.
6.2 Output overvoltage protection
Overvoltage protection, or OVP, is achieved by using an internal comparator connected to
the feedback, which turns OFF the power stage when the OVP threshold is reached. This
threshold is typically 30% higher than the feedback voltage.
When a voltage divider is required to adjust the output voltage (Figure 13), the OVP
intervention will be set at:
Equation 1
Where R
R
is between the feedback pin and ground.
2
is the resistor connected between the output voltage and the feedback pin, and
1
6.3 Zero load
Due to the fact that the internal power is a PDMOS, no boostrap capacitor is required and so
the device works properly even with no load at the output. In this case it works in burst
mode, with a random burst repetition rate.
V
OVP
R1R2+
--------------------
1.3
•V
•=
R
FB
2
12/37Doc ID 13956 Rev 5
A5972DClosing the loop
7 Closing the loop
Figure 7.Block diagram of the loop
Doc ID 13956 Rev 513/37
Closing the loopA5972D
7.1 Error amplifier and compensation network
The output L-C filter of a step-down converter contributes with 180 degrees phase shift in
the control loop. For this reason a compensation network between the COMP pin and
GROUND is added. The simplest compensation network together with the equivalent circuit
of the error amplifier are shown in Figure 8. R
open loop gain. CP does not significantly affect system stability but it is useful to reduce the
noise of the COMP pin.
The transfer function of the error amplifier and its compensation network is:
is the
minimum value. A voltage feed forward is implemented to ensure a constant GPWM. This is
obtained by generating a sawtooth waveform directly proportional to the input voltage V
CC
.
Equation 13
V
OSCMAXVOSCMIN
–KV
•=
CC
Where K is equal to 0.076. Therefore the PWM gain is also equal to:
Equation 14
s()
1
--- -const==
K
G
PWM
This means that even if the input voltage changes, the error amplifier does not change its
value to keep the loop in regulation, thus ensuring a better line regulation and line transient
response.
In summary, the open loop gain can be expressed as:
Equation 15
R
2
--------------------
•A
Gs() G
PWM
s()
R1R2+
s()•ALC•s()=
O
16/37Doc ID 13956 Rev 5
A5972DClosing the loop
Example:
Considering R
F
= 9 Hz
P1
F
= 150 kHz
P2
F
= 1.5 kHz
Z1
If L = 33 µH, C
F
PLC
F
ZESR
Finally R
1
= 4.7 kΩ, CC = 22 nF and CP = 220 pF, the poles and zeroes of A0 are:
C
= 100 µF and ESR = 80mΩ, the poles and zeroes of ALC become:
OUT
= 3.3 kHz
= 19.89 kHz
= 5.6 kΩ and R2 = 3.3 kΩ.
The gain and phase bode diagrams are plotted respectively inFigure 9 and Figure 10.
Figure 9.Module plot
Figure 10. Phase plot
The cut-off frequency and the phase margin are:
Equation 16
FC33K Hz=
Doc ID 13956 Rev 517/37
Phase margin = 46°
Application informationA5972D
8 Application information
8.1 Component selection
●Input capacitor
The input capacitor must be able to support the maximum input operating voltage and the
maximum RMS input current.
Since step-down converters draw current from the input in pulses, the input current is
squared and the height of each pulse is equal to the output current. The input capacitor has
to absorb all this switching current, which can be up to the load current divided by two (worst
case, with duty cycle of 50%). For this reason, the quality of these capacitors has to be very
high to minimize the power dissipation generated by the internal ESR, thereby improving
system reliability and efficiency. The critical parameter is usually the RMS current rating,
which must be higher than the RMS input current. The maximum RMS input current (flowing
through the input capacitor) is:
Equation 17
2
I
RMSIO
D
2D
•
--------------- -–
η
2
D
------ -+•=
2
η
Where η is the expected system efficiency, D is the duty cycle and I
is the output DC
O
current. This function reaches its maximum value at D = 0.5 and the equivalent RMS current
is equal to I
divided by 2 (considering η = 1). The maximum and minimum duty cycles are:
O
Equation 18
V
+
D
MAX
OUTVF
------------------------------------ -=
V
–
INMINVSW
and
Equation 19
V
+
OUTVF
MIN
--------------------------------------=
V
–
INMAXVSW
D
18/37Doc ID 13956 Rev 5
A5972DApplication information
Where VF is the freewheeling diode forward voltage and VSW the voltage drop across the
internal PDMOS. Considering the range D
MIN
to D
, it is possible to determine the max
MAX
IRMS going through the input capacitor. Capacitors that can be considered are:
Electrolytic capacitors:
These are widely used due to their low price and their availability in a wide range of
RMS current ratings.
The only drawback is that, considering ripple current rating requirements, they are
physically larger than other capacitors.
Ceramic capacitors:
If available for the required value and voltage rating, these capacitors usually have a
higher RMS current rating for a given physical dimension (due to very low ESR).
The drawback is the considerably high cost.
Tantalum capacitors:
Very good, small tantalum capacitors with very low ESR are becoming more available.
However, they can occasionally burn if subjected to very high current during charge.
Therefore, it is better to avoid this type of capacitor for the input filter of the device. They
can, however, be subjected to high surge current when connected to the power supply.
Table 6.List of ceramic capacitors for the A5972D
ManufacturerSeriesCapacitor value (µ) Rated voltage (V)
TAIYO YUDENUMK325BJ106MM-T1050
MURATAGRM42-2 X7R 475K 504.750
●Output capacitor
The output capacitor is very important to meet the output voltage ripple requirement.
Using a small inductor value is useful to reduce the size of the choke but it increases the
current ripple. So, to reduce the output voltage ripple, a low ESR capacitor is required.
Nevertheless, the ESR of the output capacitor introduces a zero in the open loop gain,
which helps to increase the phase margin of the system. If the zero goes to a very high
frequency, its effect is negligible. For this reason, ceramic capacitors and very low ESR
capacitors in general should be avoided.
Tantalum and electrolytic capacitors are usually a good choice for this purpose. A list of
some tantalum capacitor manufacturers is provided in Table 7.: Output capacitor selection.
Doc ID 13956 Rev 519/37
Application informationA5972D
Table 7.Output capacitor selection
ManufacturerSeriesCap value (µF)Rated voltage (V)ESR (mΩ)
Sanyo POSCAP
AVXTPS100 to 4704 to 3550 to 200
KEMETT494/5100 to 4704 to 2030 to 200
Sprague595D220 to 3904 to 20160 to 650
1. POSCAP capacitors have some characteristics which are very similar to tantalum.
●Inductor
(1)
TAE100 to 4704 to 1625 to 35
THB/C/E100 to 4704 to 1625 to 55
The inductor value is very important as it fixes the ripple current flowing through the output
capacitor. The ripple current is usually fixed at 20 - 40% of I
I
max = 1.5 A. The approximate inductor value is obtained using the following formula:
O
, which is 0.3 - 0.6 A with
omax
Equation 20
–()
V
INVOUT
----------------------------------
L
ΔI
•=
T
ON
where T
V
OUT
is the ON time of the internal switch, given by D · T. For example, with
ON
= 3.3 V, V
= 12 V and ΔIO = 0.45 A, the inductor value is about 22 µH. The peak
IN
current through the inductor is given by:
Equation 21
ΔI
I
PKIO
-----+=
2
and it can be observed that if the inductor value decreases, the peak current (which must be
lower than the current limit of the device) increases. So, when the peak current is fixed, a
higher inductor value allows a higher value for the output current. In the Table 8.: Inductor
selection, some inductor manufacturers are listed.
Table 8.Inductor selection
ManufacturerSeriesInductor value (µH)Saturation current (A)
CoilcraftDO3316T15 to 332.0 to 3.0
CoiltronicsUP1B22 to 332.0 to 2.4
BIHM76-315 to 332.5 to 3.3
EpcosB8247615 to 332 to 3
Wurth Elektronik7445611515 to 332.5 to 3
20/37Doc ID 13956 Rev 5
A5972DApplication information
8.2 Layout considerations
The layout of switching DC-DC converters is very important to minimize noise and
interference. Power-generating portions of the layout are the main cause of noise and so
high switching current loop areas should be kept as small as possible and lead lengths as
short as possible.
High impedance paths (in particular the feedback connections) are susceptible to
interference, so they should be as far as possible from the high current paths. An layout
example is provided in Figure 11 below.
The input and output loops are minimized to avoid radiation and high frequency resonance
problems. The feedback pin connections to the external divider are very close to the device
to avoid pick-up noise.
Figure 11. Layout example
A5972D
8.3 Thermal considerations
The dissipated power of the device is tied to three different sources:
●Conduction losses due to the not insignificant R
Equation 22
P
ON
Where D is the duty cycle of the application. Note that the duty cycle is theoretically given by
the ratio between V
and VIN, but in practice it is substantially higher than this value to
OUT
R
()•
DSONIOUT
, which are equal to:
DSON
2
D•=
Doc ID 13956 Rev 521/37
Application informationA5972D
compensate for the losses in the overall application. For this reason, the switching losses
related to the R
●Switching losses due to turning ON and OFF. These are derived using the following
increases compared to an ideal case.
DSON
equation:
Equation 23
T
+()
ONTOFF
----------------------------------- -
P
SWVINIOUT
••F
2
=•I
SWVIN
•FSW••=
OUTTSW
Where T
RISE
and T
represent the switching times of the power element that cause the
FAL L
switching losses when driving an inductive load (see Figure 12). T
switching time.
Figure 12. Switching losses
●Quiescent current losses.
Equation 24
is the equivalent
SW
PQVINIQ•=
Where I
is the quiescent current.
Q
Example:
–V
–V
–I
22/37Doc ID 13956 Rev 5
IN
OUT
OUT
= 12 V
= 3.3 V
= 1.5 A
A5972DApplication information
R
has a typical value of 0.25 @ 25 °C and increases up to a maximum value of 0.5. @
is the thermal resistance junction-toambient. Considering that the device is mounted on board with a good ground plane, that it
has a thermal resistance junction-to-ambient (Rth
) of about 65 °C/W, and an ambient
J-A
temperature of about 70 °C:
Equation 27
TJ70 0.615 65 110° C≅•+=
8.4 Short-circuit protection
In overcurrent protection mode, when the peak current reaches the current limit, the device
reduces the T
frequency to approximately one third of its nominal value even when synchronized to an
external signal (see Section 5.3: Current protection). In these conditions, the duty cycle is
strongly reduced and, in most applications, this is enough to limit the current to ILIM. In any
event, in case of heavy short-circuit at the output (V
application conditions (V
peak could reach values higher than ILIM. This can be understood considering the inductor
current ripple during the ON and OFF phases:
●ON phase
Equation 28
●OFF phase
Equation 29
where V
is the voltage drop across the diode, DCRL is the series resistance of the inductor.
D
down to its minimum value (approximately 250 nsec) and the switching
ON
value and parasitic effect of external components) the current
is very small as equal to the voltage drop across parasitic components (typically the DCR of
the inductor and the V
the inductor is instead maximized as approximately equal to V
of the free wheeling diode) while during TON the voltage applied
FW
.
IN
So the Equation 28 and the Equation 29 in overcurrent conditions can be simplified to:
controlled in most of the applications (see Figure 13). When the application must sustain the
short-circuit condition for an extended period, the external components (mainly the inductor
and diode) must be selected based on this value.
In case the V
does not compensate the current increase during T
an example of a power up phase with V
is very high, it could occur that the ripple current during T
IN
= V
IN
IN MAX
(Equation 30). The Figure 15 shows
ON
= 36 V where Δ
IL TON
(Equation 31)
OFF
> Δ
IL TOFF
so the
current escalates and the balance between Equation 30 and Equation 31 occurs at a current
slightly higher than the current limit. This must be taken into account in particular to avoid
the risk of an abrupt inductor saturation.
Figure 13. Short-circuit current V
= 12 V
IN
24/37Doc ID 13956 Rev 5
A5972DApplication information
Figure 14. Short-circuit current VIN = 24 V
Figure 15. Short-circuit current V
8.5 Application circuit
Figure 16 shows the evaluation board application circuit, where the input supply voltage,
V
, can range from 4 V to 36 V and the output voltage is adjustable from 1.235 V to 6.3 V
CC
due to the voltage rating of the output capacitor,.
= 36 V
IN
Doc ID 13956 Rev 525/37
Application informationA5972D
Figure 16. Evaluation board application circuit
L1 33uH
A5972D
Table 9.Component list
ReferencePart numberDescriptionManufacturer
C1GRM42-2 X7R 475K 504.7 µF, 50 VMurata
C2POSCAP 6TAE330ML330 µF, 6.3 VSanyo
C3C1206C470J5GAC47 pF, 5%, 50 VKEMET
C4C1206C223K5RAC22 nF, 10%, 50 VKEMET
R15.6 kΩ, 1%, 0.1 W 0603Neohm
R23.3 kΩ, 1%, 0.1 W 0603Neohm
R322 kΩ, 1%, 0.1 W 0603Neohm
D1STPS3L40U2 A, 40 VSTMicroelectronics
L1DO3316T-333MLD33 µH, 2.1 ACoilcraft
26/37Doc ID 13956 Rev 5
A5972DApplication information
Figure 17. PCB layout (component side)
Figure 18. PCB layout (bottom side)
Figure 19. PCB layout (front side)
Doc ID 13956 Rev 527/37
Application informationA5972D
8.6 Positive buck-boost regulator
The device can be used to implement a step-up/down converter with a positive output
voltage.
The output voltage is given by:
Equation 32
D
-------------
V
OUT
----------------------------- -=
VINV
+
⋅=
1D–
OUT
V
OUTVIN
where the ideal duty cycle D for the buck boost converter is:
Equation 33
D
However, due to power losses in the passive elements, the real duty cycle is always higher
than this. The real value (that can be measured in the application) should be used in the
following formulas.
The peak current flowing in the embedded switch is:
Equation 34
I
SW
I
LOAD
---------------
1D–
I
RIPPLE
------------------- -+
2
I
LOAD
---------------
1D–
V
IN
---------- -
2L⋅
---------
⋅+==
f
SW
D
while its average current is equal to:
Equation 35
I
LOAD
---------------=
I
SW
1D–
This is due to the fact that the current flowing through the internal power switch is delivered
to the output only during the OFF phase.
The switch peak current must be lower than the minimum current limit of the overcurrent
protection (see Ta bl e 4 for details) while the average current must be lower than the rated
DC current of the device.
As a consequence, the maximum output current is:
Equation 36
where I
SW MAX
I
OUT MAXISW MAX
represents the rated current of the device.
1D–()⋅≅
The current capability is reduced by the term (1-D) and so, for example, with a duty cycle of
0.5, and considering an average current through the switch of 1.5 A, the maximum output
current deliverable to the load is 0.75 A.
The figure below shows the schematic circuit of this topology for a 12 V output voltage and
5 V input.
28/37Doc ID 13956 Rev 5
A5972DApplication information
Figure 20. Positive buck-boost regulator
8.7 Negative buck-boost regulator
In Figure 21, the schematic circuit for a standard buck-boost topology is shown. The output
voltage is:
Equation 37
D
V
OUT
-------------
VIN–
⋅=
1D–
where the ideal duty cycle D for the buck boost converter is:
Equation 38
V–
OUT
----------------------------- -=
D
VINV
–
OUT
The considerations given in Section 8.7 for the real duty cycle are still valid here.
Also the Equation 34 till Equation 36 can be used to calculate the maximum output current.
So, as an example, considering the conversion V
= 12 V to V
IN
OUT
= -5 V, I
LOAD
= 0.2 A:
Equation 39
D
5
--------------- -0.706==
512+
Equation 40
I
SW
I
LOAD
---------------
1D–
0.2
----------------------- -0.7A===
10.706–
An important thing to take into account is that the ground pin of the device is connected to
the negative output voltage. Therefore, the device is subjected to a voltage equal to V
IN-VO
which must be lower than 36 V (the maximum operating input voltage).
,
Doc ID 13956 Rev 529/37
Application informationA5972D
Figure 21. Negative buck-boost regulator
8.8 Compensation network with MLCC at the output
MLCCs (multiple layer ceramic capacitor) with values in the range of 10 µF-22 µF and rated
voltages in the range of 10 V-25 V are available today at relatively low cost from many
manufacturers.
These capacitors have very low ESR values (a few mΩ) and thus are occasionally used for
the output filter in order to reduce the voltage ripple and the overall size of the application.
However, a very low ESR value affects the compensation of the loop (see Section 7) and in
order to keep the system stable, a more complicated compensation network may be
required. However, due to the architecture of the internal error amplifier the bandwidth with
this compensation is limited.
That is why output capacitors with a not negligible ESR are suggested. The selection of the
output capacitor have to guarantee that the zero introduced by this component is inside the
designed system bandwidth and close to the frequency of the double pole introduced by the
LC filter. A general rule for the selection of this compound for the system stability is provided
in Equation 41.
Equation 41
f
Z ESR
----------------------------------------------- -=bandwidth<
2 π ESR C
1
⋅⋅⋅
f<
f
LC
Z ESR
OUT
10 fLC⋅<
The figure below shows an example of a compensation network stabilizing the system with
ceramic capacitors at the output (the optimum component value depends on the
application).
30/37Doc ID 13956 Rev 5
A5972DApplication information
Figure 22. MLCC compensation network example
Doc ID 13956 Rev 531/37
Typical characteristicsA5972D
9 Typical characteristics
Figure 23. Line regulationFigure 24. Load regulation
Vo (V)
3.312
3.308
3.304
3.3
3.296
3.292
3.288
3.284
3.28
3.276
Vcc = 12V
Vo = 3.3V
Tj = 25°C
Tj = 125°C
00.511.5
Io (A)
Figure 25. Output voltage vs junction
temperature
Figure 27. Quiescent current vs junction
temperature
Figure 26. Switching frequency vs
junction temperature
Figure 28. Shutdown current vs junction
temperature
32/37Doc ID 13956 Rev 5
A5972DTypical characteristics
Figure 29. Junction temperature vs
Figure 31. Efficiency vs output currentFigure 32. Efficiency vs output current
output current
Figure 30. Junction temperature vs
output current
Doc ID 13956 Rev 533/37
Package mechanical dataA5972D
10 Package mechanical data
In order to meet environmental requirements, ST offers these devices in different grades of
ECOPACK
specifications, grade definitions and product status are available at: www.st.com.
ECOPACK is an ST trademark.
®
packages, depending on their level of environmental compliance. ECOPACK®
34/37Doc ID 13956 Rev 5
A5972DPackage mechanical data
Table 10.SO-8 mechanical data
Dim.
MinTypMaxMinTypMax
A 1.35 1.75 0.053 0.069
A1 0.10 0.25 0.004 0.010
A2 1.10 1.65 0.043 0.065
B 0.33 0.51 0.013 0.020
C 0.19 0.25 0.007 0.010
(1)
D
4.80 5.00 0.189 0.197
E 3.80 4.00 0.15 0.157
e 1.27 0.050
H 5.80 6.20 0.228 0.244
h 0.25 0.50 0.010 0.020
L 0.40 1.27 0.016 0.050
k 0° (min.), 8° (max.)
ddd 0.10 0.004
1. Dimensions D does not include mold flash, protrusions or gate burrs. Mold flash, potrusions or gate burrs
shall not exceed 0.15mm (.006inch) in total (both side).
mm.inch
Figure 33. Package dimensions
Doc ID 13956 Rev 535/37
Revision historyA5972D
11 Revision history
Table 11.Document revision history
DateRevisionChanges
06-Aug-20071Initial release
5-Nov-20072Updated: Table 4 on page 5
2-May-20083Updated: Cover page, Table 4 on page 6
21-Aug-20084Updated: Coverpage and Table 4 on page 6
02-Nov-20095
Updated coverpage, Table 4 on page 6 and added Figure 23 on
page 32
36/37Doc ID 13956 Rev 5
A5972D
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