2 A step-down switching regulator for automotive applications
Features
■ 2 A DC output current
■ Qualified following AEC-Q100 requirements
(see PPAP for more details)
■ 4.5 V to 38 V input voltage
■ Output voltage adjustable from 0.6 V
■ 250 kHz switching frequency, programmable
up to 1 MHz
■ Internal soft-start and enable
■ Low dropout operation: 100% duty cycle
■ Voltage feed-forward
■ Zero load current operation
■ Overcurrent and thermal protection
■ HSOP8 package
Applications
■ Dedicated to automotive applications
■ Automotive LED driving
A7985A
Datasheet − preliminary data
HSOP8 exposed pad
Description
The A7985A is a step-down switching regulator
with a 2.5 A (minimum) current limited embedded
power MOSFET, so it is able to deliver up to 2 A
current to the load depending on the application
conditions.
The input voltage can range from 4.5 V to 38 V,
while the output voltage can be set starting from
0.6 V to V
Requiring a minimum set of external components,
the device includes an internal 250 kHz switching
frequency oscillator that can be externally
adjusted up to 1 MHz.
.
IN
The HSOP package with exposed pad allows the
reduction of R
down to 40 °C/W.
thJA
Figure 1.Application circuit
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April 2012Doc ID 023128 Rev 11/45
This is preliminar y information on a new product now in development or undergoing evaluation. Details are subject to
change without notice.
Figure 22.Junction temperature vs. output current @ V
Figure 23.Junction temperature vs. output current @ V
Figure 24.Junction temperature vs. output current @ V
Figure 25.Efficiency vs. output current @ V
Figure 26.Efficiency vs. output current@ V
Figure 27.Efficiency vs. output current@ V
Master/slave synchronization. When it is left floating, a signal with a
phase shift of half a period in respect to the power turn-on is present at
the pin. When connected to an external signal at a frequency higher than
2SYNCH
3EN
4COMPError amplifier output to be used for loop frequency compensation
5FB
6FSW
7GNDGround
8V
CC
the internal one, the device is synchronized by the external signal, with
zero phase shift.
Connecting together the SYNCH pins of two devices, the one with the
higher frequency works as master and the other as slave; so the two
power turn-ons have a phase shift of half a period.
A logical signal (active high) enables the device. With EN higher than
1.2 V the device is ON and with EN lower than 0.63 V the device is OFF.
Feedback input. Connecting the output voltage directly to this pin the
output voltage is regulated at 0.6 V. To have higher regulated voltages an
external resistor divider is required from Vout to the FB pin.
The switching frequency can be increased connecting an external
resistor from the FSW pin and ground. If this pin is left floating the device
works at its free-running frequency of 250 KHz.
Unregulated DC input voltage
6/45Doc ID 023128 Rev 1
A7985AMaximum ratings
2 Maximum ratings
Table 2.Absolute maximum ratings
SymbolParameterValueUnit
VccInput voltage45
OUTOutput DC voltage-0.3 to V
FSW, COMP, SYNCHAnalog pin-0.3 to 4
ENEnable pin-0.3 to V
FBFeedback voltage-0.3 to 1.5
P
TOT
T
J
T
stg
3 Thermal data
Table 3.Thermal data
SymbolParameterValueUnit
R
thJA
1. Package mounted on demonstration board.
Maximum thermal resistance
junction-ambient
CC
V
CC
Power dissipation
< 60 °C
at T
A
HSOP2W
Junction temperature range-40 to 150°C
Storage temperature range-55 to 150°C
(1)
HSOP840°C/W
Doc ID 023128 Rev 17/45
Electrical characteristicsA7985A
4 Electrical characteristics
TJ=-40 °C to 125 °C, VCC=12 V, unless otherwise specified.
Table 4.Electrical characteristics
Values
SymbolParameterTest condition
Min.Typ.Max.
Unit
V
V
CCON
V
CCHYS
R
DSON
I
LIM
CC
Operating input voltage
range
4.538
Tur n - on VCC threshold4.5
VCC UVLO hysteresis0.10.4
MOSFET ONresistance
Maximum limiting
current
2.53.5A
200400mΩ
Oscillator
Switching frequency210250275kHz
FSW pin voltage1.254V
V
F
FSW
SW
DDuty cycle0100%
F
ADJ
Adjustable switching
frequency
R
= 33 kΩ1000kHz
FSW
Dynamic characteristics
V
FB
Feedback voltage4.5 V < V
< 38 V0.5820.60.618V
CC
DC characteristics
I
Q
I
QST-BY
Quiescent currentDuty cycle = 0, V
Total standby quiescent
current
= 0.8 V2.4mA
FB
2030µA
V
Enable
Device OFF level0.3
V
EN
I
EN
EN threshold voltage
Device ON level1.2
EN currentEN = V
CC
Soft-start
FSW pin floating7.38.29.8
T
SS
Soft-start duration
F
R
SW
FSW
=1 MHz,
= 33 kΩ
Error amplifier
8/45Doc ID 023128 Rev 1
V
7.510µA
ms
2
A7985AElectrical characteristics
Table 4.Electrical characteristics (continued)
Values
SymbolParameterTest condition
Min.Typ.Max.
Unit
V
CH
V
CL
I
O SOURCE
I
O SINK
G
High level output
voltage
Low level output voltage V
Source COMP pinV
Sink COMP pinV
Open loop voltage gain
V
Synchronization function
V
S_IN,HI
V
S_IN,LO
t
S_IN_PW
I
SYNCH,LO
V
S_OUT,HI
t
S_OUT_PW
High input voltage23.3
Low input voltage1
Input pulse width
Slave sink currentV
Master output amplitude I
Output pulse widthSYNCH floating110ns
Protection
Thermal shutdown150
T
SHDN
Hysteresis30
< 0.6 V3
V
FB
> 0.6 V0.1
FB
= 0.5 V, V
FB
= 0.7 V, V
FB
(1)
V
S_IN,HI
V
S_IN,HI
SYNCH
SOURCE
= 3 V, V
= 2 V, V
= 2.9 V0.71mA
= 4.5 mA2V
= 1 V19mA
COMP
= 0.75 V30mA
COMP
100dB
= 0 V100
S_IN,LO
= 1 V300
S_IN,LO
V
V
ns
°C
1. Guaranteed by design.
Doc ID 023128 Rev 19/45
Functional descriptionA7985A
5 Functional description
The A7985A is based on a “voltage mode”, constant frequency control. The output voltage
is sensed by the feedback pin (FB) compared to an internal reference (0.6 V) providing
V
OUT
an error signal that, compared to a fixed frequency sawtooth, controls the ON and OFF time
of the power switch.
The main internal blocks are shown in the block diagram in Figure 3. They are:
●A fully integrated oscillator that provides sawtooth to modulate the duty cycle and the
synchronization signal. Its switching frequency can be adjusted by an external resistor.
The voltage and frequency feed-forward are implemented
●Soft-start circuitry to limit inrush current during the startup phase
●Voltage mode error amplifier
●Pulse width modulator and the relative logic circuitry necessary to drive the internal
power switch
●High-side driver for embedded P-channel power MOSFET switch
●Peak current limit sensing block, to handle overload and short-circuit conditions
●A voltage regulator and internal reference. It supplies internal circuitry and provides a
fixed internal reference
●A voltage monitor circuitry (UVLO) that checks the input and internal voltages
●A thermal shutdown block, to prevent thermal run-away.
Figure 3.Block diagram
TRIMMINGUVLO
TRIMMINGUVLOUVLO
EN
EN
COMP
COMP
0.6V
0.6V
SOFT-
SOFT-
START
START
EN
EN
FB
FB
REGULATOR
REGULATOR
REGULATOR
&
&
&
BANDGAP
BANDGAP
BANDGAP
1.254V3.3V
1.254V3.3V
THERMAL
THERMAL
SHUTDOWN
SHUTDOWN
E/A
E/A
OSCILLATOR
OSCILLATOR
FSW
FSW
PWM
PWM
GND
GND
PEAK
PEAK
CURRENT
CURRENT
LIMIT
LIMIT
SRQ
SRQ
SYNCH
SYNCH
&
&
PHASE SHIFT
PHASE SHIFT
SYNCH
SYNCH
DRIVER
DRIVER
VCC
VCC
OUT
OUT
10/45Doc ID 023128 Rev 1
A7985AFunctional description
5.1 Oscillator and synchronization
Figure 4 shows the block diagram of the oscillator circuit. The internal oscillator provides a
constant frequency clock. Its frequency depends on the resistor externally connected to the
FSW pin. If the FSW pin is left floating, the frequency is 250 kHz; it can be increased as
shown in Figure 6 by an external resistor connected to ground.
To improve the line transient performance, keeping the PWM gain constant versus the input
voltage, the voltage feed-forward is implemented by changing the slope of the sawtooth
according to the input voltage change (see Figure 5.a).
The slope of the sawtooth also changes if the oscillator frequency is increased by the
external resistor. In this way, a frequency feed-forward is implemented (Figure 5.b) in order
to keep the PWM gain constant versus the switching frequency (see Section 6.4 for PWM
gain expression).
On the SYNCH pin the synchronization signal is generated. This signal has a phase shift of
180° with respect to the clock. This delay is useful when two devices are synchronized
connecting the SYNCH pin together. When SYNCH pins are connected, the device with the
higher oscillator frequency works as master, so the slave device switches at the frequency
of the master but with a delay of half a period. This minimizes the RMS current flowing
through the input capacitor (see the L5988D datasheet).
Figure 4.Oscillator circuit block diagram
Clock
ClockClock
FSW
FSW
The device can be synchronized to work at a higher frequency feeding an external clock
signal. The synchronization changes the sawtooth amplitude, changing the PWM gain
(Figure 5.c). This change must be taken into account when the loop stability is studied. To
minimize the change of the PWM gain, the free-running frequency should be set (with a
resistor on the FSW pin) only slightly lower than the external clock frequency. This preadjusting of the frequency changes the sawtooth slope in order to render negligible the
truncation of sawtooth, due to the external synchronization.
Clock
Clock
Generator
Generator
Synchronization
Synchronization
Ramp
Ramp
Generator
Generator
SYNCH
SYNCH
Sawtooth
Sawtooth
Doc ID 023128 Rev 111/45
Functional descriptionA7985A
Figure 5.Sawtooth: voltage and frequency feed-forward; external synchronization
Figure 6.Oscillator frequency versus the FSW pin resistor
Soft-start is essential to assure the correct and safe startup of the step-down converter. It
avoids inrush current surge and makes the output voltage increase monothonically.
The soft-start is performed by a staircase ramp on the non-inverting input (V
) of the error
REF
amplifier. So the output voltage slew rate is:
Equation 1
VREF
⎛⎞
1
------- -+
⋅=
⎝⎠
R2
where SR
OUT
SR
SR
is the slew rate of the non-inverting input, while R1and R2 is the resistor
VREF
R1
divider to regulate the output voltage (see Figure 7). The soft-start staircase consists of 64
steps of 9.5 mV each, from 0 V to 0.6 V. The time base of one step is of 32 clock cycles. So
the soft-start time and then the output voltage slew rate depend on the switching frequency.
Figure 7.Soft-start scheme
Soft-start time results:
Equation 2
SS
TIME
32 64⋅
--------------------=
Fsw
For example, with a switching frequency of 250 kHz, the SS
Doc ID 023128 Rev 113/45
TIME
is 8 ms.
Functional descriptionA7985A
5.3 Error amplifier and compensation
The error amplifier (E/A) provides the error signal to be compared with the sawtooth to
perform the pulse width modulation. Its non-inverting input is internally connected to a 0.6 V
voltage reference, while its inverting input (FB) and output (COMP) are externally available
for feedback and frequency compensation. In this device the error amplifier is a voltage
mode operational amplifier, so with high DC gain and low output impedance.
The uncompensated error amplifier characteristics are shown in Ta bl e 5 .
In continuous conduction mode (CCM), the transfer function of the power section has two
poles due to the LC filter and one zero due to the ESR of the output capacitor. Different
kinds of compensation networks can be used depending on the ESR value of the output
capacitor. In case the zero introduced by the output capacitor helps to compensate the
double pole of the LC filter, a Type II compensation network can be used. Otherwise, a Type
III compensation network must be used (see Section 6.4 for details of the compensation
network selection).
The methodology to compensate the loop is to introduce zeroes to obtain a safe phase
margin.
5.4 Overcurrent protection
The A7985A implements the overcurrent protection sensing current flowing through the
power MOSFET. Due to the noise created by the switching activity of the power MOSFET,
the current sensing is disabled during the initial phase of the conduction time. This avoids an
erroneous detection of a fault condition. This interval is generally known as “masking time”
or “blanking time”. The masking time is about 200 ns.
If the overcurrent limit is reached, the power MOSFET is turned off, implementing the pulseby-pulse overcurrent protection. Under an overcurrent condition, the device can skip turn-on
pulses in order to keep the output current constant and equal to the current limit. If, at the
end of the “masking time”, the current is higher than the overcurrent threshold, the power
MOSFET is turned off and one pulse is skipped. If, at the following switching-on, when the
“masking time” ends, the current is still higher than the overcurrent threshold, the device
skips two pulses. This mechanism is repeated and the device can skip up to seven pulses.
While, if at the end of the “masking time” the current is lower than the over current threshold,
the number of skipped cycles is decreased by one unit (see Figure 8).
So the overcurrent/short-circuit protection acts by switching off the power MOSFET and
reducing the switching frequency down to one eighth of the default switching frequency, in
order to keep constant the output current around the current limit.
14/45Doc ID 023128 Rev 1
A7985AFunctional description
This kind of overcurrent protection is effective if the output current is limited. To prevent the
current from diverging, the current ripple in the inductor during the ON-time must not be
higher than the current ripple during the OFF-time. That is:
The enable feature allows the device to be put into stand-by mode. With the EN pin lower
than 0.3 V, the device is disabled and the power consumption is reduced to less than 30 µA.
With the EN pin lower than 1.2 V, the device is enabled. If the EN pin is left floating, an
internal pull-down ensures that the voltage at the pin reaches the inhibit threshold and the
device is disabled. The pin is also V
compatible.
CC
5.6 Hysteretic thermal shutdown
The thermal shutdown block generates a signal that turns off the power stage if the junction
temperature goes above 150 °C. Once the junction temperature goes back to about 130 °C,
the device restarts in normal operation. The sensing element is very close to the PDMOS
area, so ensuring an accurate and fast temperature detection.
16/45Doc ID 023128 Rev 1
A7985AApplication information
6 Application information
6.1 Input capacitor selection
The capacitor connected to the input must be capable of supporting the maximum input
operating voltage and the maximum RMS input current required by the device. The input
capacitor is subject to a pulsed current, the RMS value of which is dissipated over its ESR,
affecting the overall system efficiency.
So the input capacitor must have an RMS current rating higher than the maximum RMS
input current and an ESR value compliant with the expected efficiency.
The maximum RMS input current flowing through the capacitor can be calculated as:
Equation 6
2
2D
I
RMSIO
⋅
D
----------------- -–
where Io is the maximum DC output current, D is the duty cycle, η is the efficiency.
Considering η=1, this function has a maximum at D=0.5 and it is equal to Io/2.
2
D
------ -+⋅=
2
η
η
In a specific application the range of possible duty cycles must be considered in order to find
out the maximum RMS input current. The maximum and minimum duty cycles can be
calculated as:
Equation 7
V
+
OUTVF
MAX
---------------------------------------=
–
V
INMINVSW
D
and
Equation 8
V
+
OUTVF
-----------------------------------------=
V
–
INMAXVSW
where V
D
MIN
is the forward voltage on the freewheeling diode and VSW is voltage drop across
F
the internal PDMOS.
The peak-to-peak voltage across the input capacitor can be calculated as:
Equation 9
V
PP
I
O
------------------------------
CINFSW⋅
D
⎛⎞
--- -–
1
⎝⎠
η
D
--- -
D
1D–()⋅+⋅ESR I
η
⋅+⋅=
O
where ESR is the equivalent series resistance of the capacitor.
Doc ID 023128 Rev 117/45
Application informationA7985A
Given the physical dimension, ceramic capacitors can well meet the requirements of the
input filter sustaining a higher input RMS current than electrolytic/tantalum types. In this
case, the equation of C
as a function of the target VPP can be written as follows:
IN
Equation 10
C
IN
I
O
-------------------------------
V
⋅
PPFSW
D
⎛⎞
--- -–
1
⎝⎠
η
D
--- -
D
1D–()⋅+⋅⋅=
η
neglecting the small ESR of ceramic capacitors.
Considering η=1, this function has its maximum in D=0.5, therefore, given the maximum
peak-to-peak input voltage (V
PP_MAX
), the minimum input capacitor (C
IN_MIN
) value is:
Equation 11
I
O
PP_MAXFSW
Ty p i ca l l y, C
of V
INMAX
C
IN_MIN
is dimensioned to keep the maximum peak-to-peak voltage in the order of 1%
In Figure 6, some multi-layer ceramic capacitors suitable for this device are reported.
Table 6.Input MLCC capacitors
ManufacturerSeriesCap value (µF)Rated voltage (V)
Taiyo Yuden
UMK325BJ106MM-T1050
GMK325BJ106MN-T1035
muRataGRM32ER71H475K4.750
A ceramic bypass capacitor, as close to the VCC and GND pins as possible, so that
additional parasitic ESR and ESL are minimized, is suggested in order to prevent instability
on the output voltage due to noise. The value of the bypass capacitor can go from 100 nF to
1 µF.
6.2 Inductor selection
The inductance value fixes the current ripple flowing through the output capacitor. So the
minimum inductance value in order to have the expected current ripple must be selected.
The rule to fix the current ripple value is to have a ripple at 20%-40% of the output current.
In continuous current mode (CCM), the inductance value can be calculated by the following
equation:
18/45Doc ID 023128 Rev 1
A7985AApplication information
Equation 12
VINV
∆I
L
–
OUT
------------------------------- -
L
⋅
T
ON
+
V
OUTVF
-----------------------------
L
⋅==
T
OFF
where T
time of the external diode (in CCM, F
fixed V
section to calculate minimum duty). So by fixing ∆I
is the conduction time of the internal high-side switch and T
ON
, is obtained at maximum T
OUT
=1/(TON + T
SW
, that is at minimum duty cycle (see previous
OFF
)). The maximum current ripple, at
OFF
=20% to 30% of the maximum output
L
current, the minimum inductance value can be calculated:
Equation 13
1D
+
------------------------
⋅=
OFF
–
MIN
F
SW
).
where F
is the switching frequency, 1/(TON + T
SW
For example, for V
value to have ∆I
L
V
OUTVF
MIN
-----------------------------
∆I
MAX
L
=5 V, VIN=24 V, IO=2 A and FSW=250 kHz, the minimum inductance
OUT
=30% of IO is about 28 µH.
The peak current through the inductor is given by:
Equation 14
∆I
L
I
I
LPK,
--------+=
O
2
is the conduction
OFF
So if the inductor value decreases, then the peak current (that must be lower than the
minimum current limit of the device) increases. According to the maximum DC output
current for this product family (2 A), the higher the inductor value, the higher the average
output current that can be delivered, without triggering the overcurrent protection.
In Ta ble 7 below, some inductor part numbers are listed.
Table 7.Inductors
ManufacturerSeriesInductor value (µH)Saturation current (A)
Coilcraft
Wurth
SUMIDA
MSS10383.8 to 103.9 to 6.5
MSS104812 to 223.84 to 5.34
PD Type L8.2 to 153.75 to 6.25
PD Type M2.2 to 4.74 to 6
CDRH6D226/HP1.5 to 3.33.6 to 5.2
CDR10D48MN6.6 to 124.1 to 5.7
Doc ID 023128 Rev 119/45
Application informationA7985A
6.3 Output capacitor selection
The current in the capacitor has a triangular waveform which generates a voltage ripple
across it. This ripple is due to the capacitive component (charge or discharge of the output
capacitor) and the resistive component (due to the voltage drop across its ESR). So the
output capacitor must be selected in order to have a voltage ripple compliant with the
application requirements.
The amount of the voltage ripple can be calculated starting from the current ripple obtained
by the inductor selection.
Equation 15
∆I
∆V
OUT
ESR ∆I
⋅
MAX
Usually the resistive component of the ripple is much higher than the capacitive one, if the
output capacitor adopted is not a multi-layer ceramic capacitor (MLCC) with very low ESR
value.
The output capacitor is important also for loop stability: it fixes the double LC filter pole and
the zero due to its ESR. In Section 6.4, how to consider its effect in the system stability is
illustrated.
MAX
---------------------------------------------+=
8C
⋅⋅
OUTfSW
For example, with V
to have a ∆V
OUT
=0.01·V
=5 V, VIN=24 V, ∆IL=0.9 A (resulting by the inductor value), in order
OUT
, if the multi-layer ceramic capacitors are adopted, 10 µF are
OUT
needed and the ESR effect on the output voltage ripple can be neglected. In case of notnegligible ESR (electrolytic or tantalum capacitors), the capacitor is chosen taking into
account its ESR value. So, in the case of 330 µF with ESR=70 mΩ, the resistive component
of the drop dominates and the voltage ripple is 43 mV.
The output capacitor is also important to sustain the output voltage when a load transient
with high slew rate is required by the load. When the load transient slew rate exceeds the
system bandwidth the output capacitor provides the current to the load. So if the high slew
rate load transient is required by the application, the output capacitor and system bandwidth
must be chosen in order to sustain the load transient.
In Ta ble 8 below some capacitor series are listed.
Table 8.Output capacitors
ManufacturerSeriesCap value (µF)Rated voltage (V)ESR (mΩ)
muRata
PANASONIC
SANYOTPA/B/C100 to 4704 to 1640 to 80
TDKC322522 to 1006.3< 5
GRM3222 to 1006.3 to 25< 5
GRM3110 to 476.3 to 25< 5
ECJ10 to 226.3< 5
EEFCD10 to 686.315 to 55
20/45Doc ID 023128 Rev 1
A7985AApplication information
6.4 Compensation network
The compensation network must assure stability and good dynamic performance. The loop
of the A7985A is based on the voltage mode control. The error amplifier is a voltage
operational amplifier with high bandwidth. So by selecting the compensation network the
E/A is considered as ideal, that is, its bandwidth is much larger than the system one.
The transfer functions of the PWM modulator and the output LC filter are studied (see
Figure 10). The transfer function of the PWM modulator, from the error amplifier output
(COMP pin) to the OUT pin, results:
Equation 16
V
G
PW0
IN
---------=
V
s
where V
is the sawtooth amplitude. As seen in Section 5.1, the voltage feed-forward
S
generates a sawtooth amplitude directly proportional to the input voltage, that is:
Equation 17
V
KV
⋅=
S
IN
In this way the PWM modulator gain results constant and equal to:
Equation 18
V
1
IN
G
PW0
---------
V
s
--- -18===
K
The synchronization of the device with an external clock provided through the SYNCH pin
can modify the PWM modulator gain (see Section 5.1 to understand how this gain changes
and how to keep it constant in spite of the external synchronization).
Figure 9.The error amplifier, the PWM modulator and the LC output filter
V
V
CC
CC
V
V
FB
FB
REF
REF
E/A
E/A
V
V
S
S
COMP
COMP
PWM
PWM
L
OUT
OUT
G
G
PW0
PW0
Doc ID 023128 Rev 121/45
L
ESR
ESR
G
G
LC
LC
C
C
OUT
OUT
Application informationA7985A
The transfer function on the LC filter is given by:
As seen in Section 5.3, two different kinds of network can compensate the loop. In the two
following paragraphs the guidelines to select the Type II and Type III compensation network
are illustrated.
6.4.1 Type III compensation network
The methodology to stabilize the loop consists in placing two zeroes to compensate the
effect of the LC double pole, thereby increasing phase margin; then to place one pole in the
origin to minimize the DC error on the regulated output voltage; finally to place other poles
far from the zero dB frequency.
If the equivalent series resistance (ESR) of the output capacitor introduces a zero with a
frequency higher than the desired bandwidth (that is: 2π∗ESR∗COUT<1/BW), the Type III
compensation network is needed. Multi-layer ceramic capacitors (MLCC) have very low
ESR (<1 mΩ), with very high frequency zero, so a Type III network is adopted to compensate
the loop.
In Figure 10, the Type III compensation network is shown. This network introduces two
zeroes (f
Equation 22
22/45Doc ID 023128 Rev 1
, fZ2) and three poles (fP0, fP1, fP2). They are expressed as:
In Figure 12 the module and phase of the open loop gain is shown. The bandwidth is about
32 kHz and the phase margin is 51°.
24/45Doc ID 023128 Rev 1
A7985AApplication information
Figure 12. Open loop gain Bode diagram with ceramic output capacitor
Doc ID 023128 Rev 125/45
Application informationA7985A
6.4.2 Type II compensation network
If the equivalent series resistance (ESR) of the output capacitor introduces a zero with a
frequency lower than the desired bandwidth (that is: 2π∗ESR∗COUT>1/BW), this zero helps
stabilize the loop. Electrolytic capacitors show not-negligible ESR (>30 mΩ), so with this kind
of output capacitor the Type II network combined with the zero of the ESR allows the
stabilizing of the loop.
In Figure 15 the module and phase of the open loop gain is shown. The bandwidth is about
36 kHz and the phase margin is 53°.
28/45Doc ID 023128 Rev 1
A7985AApplication information
Figure 15. Open loop gain Bode diagram with electrolytic/tantalum output capacitor
Doc ID 023128 Rev 129/45
Application informationA7985A
6.5 Thermal considerations
The thermal design is important to prevent the thermal shutdown of the device if the junction
temperature goes above 150 °C. The three different sources of losses within the device are:
a) conduction losses due to the not-negligible R
equal to:
Equation 34
of the power switch; these are
DS(on)
P
ONRDSONIOUT
where D is the duty cycle of the application and the maximum R
220 mΩ. Note that the duty cycle is theoretically given by the ratio between V
()2D⋅⋅=
overtemperature is
DS(on)
OUT
and VIN,
but actually it is quite higher to compensate the losses of the regulator. So the conduction
losses increase compared with the ideal case.
b) switching losses due to power MOSFET turn-on and turn-off; these can be
calculated as:
Equation 35
T
+()
RISETFALL
where T
RISE
P
SWVINIOUT
and T
FALL
----------------------------------------------
2
Fsw⋅⋅⋅ V
are the overlap times of the voltage across the power switch (VDS)
⋅⋅⋅==
INIOUTTSWFSW
and the current flowing into it during turn-on and turn-off phases, as shown in Figure 16.
T
is the equivalent switching time. For this device the typical value for the equivalent
SW
switching time is 40 ns.
c) Quiescent current losses, calculated as:
Equation 36
P
QVINIQ
where I
The junction temperature T
is the quiescent current (IQ=2.4 mA).
Q
can be calculated as:
J
Equation 37
T
JTA
where T
R
thJA
is the ambient temperature and P
A
is the equivalent thermal resistance junction to ambient of the device; it can be
RthJAP
is the sum of the power losses just seen.
TOT
calculated as the parallel of many paths of heat conduction from the junction to the ambient.
For this device the path through the exposed pad is the one conducting the largest amount
30/45Doc ID 023128 Rev 1
⋅=
⋅+=
TOT
A7985AApplication information
of heat. The RthJA measured on the demonstration board described in the following
paragraph is about 40 °C/W for the HSOP package.
Figure 16. Switching losses
6.6 Layout considerations
The PC board layout of the switching DC/DC regulator is very important to minimize the
noise injected in high impedance nodes and interference generated by the high switching
current loops.
In a step-down converter, the input loop (including the input capacitor, the power MOSFET
and the freewheeling diode) is the most critical one. This is due to the fact that the high
value pulsed current is flowing through it. In order to minimize the EMI, this loop must be as
short as possible.
The feedback pin (FB) connection to the external resistor divider is a high impedance node,
so the interference can be minimized by placing the routing of the feedback node as far as
possible from the high current paths. To reduce the pick-up noise, the resistor divider must
be placed very close to the device.
To filter the high frequency noise, a small bypass capacitor (220 nF - 1 µF) can be added as
close as possible to the input voltage pin of the device.
Thanks to the exposed pad of the device, the ground plane helps to reduce the thermal
resistance junction to ambient; so a large ground plane enhances the thermal performance
of the converter allowing high power conversion.
In Figure 17 a layout example is shown.
Doc ID 023128 Rev 131/45
Application informationA7985A
Figure 17. Layout example
32/45Doc ID 023128 Rev 1
A7985AApplication information
6.7 Application circuit
In Figure 18 the demonstration board application circuit is shown.
The A7985A can implement the step-up/down converter with a positive output voltage.
Figure 34 shows the schematic: one power MOSFET and one Schottky diode are added to
the standard buck topology to provide a 12 V output voltage with input voltage from 4.5 V to
38 V.
Figure 34. Positive buck-boost regulator
The relationship between input and output voltage is:
Equation 38
D
-------------
V
OUTVIN
⋅=
1D–
so the duty cycle is:
Equation 39
V
D
OUT
--------------------------------=
V
+
OUTVIN
The output voltage isn’t limited by the maximum operating voltage of the device (38 V),
because the output voltage is sensed only through the resistor divider. The external power
MOSFET maximum drain to source voltage, must be higher than output voltage; the
maximum gate to source voltage must be higher than the input voltage (in Figure 34, if V
IN
is
higher than 16 V, the gate must be protected through a Zener diode and resistor).
The current flowing through the internal power MOSFET is transferred to the load only
during the OFF time, so according to the maximum DC switch current (2.0 A), the maximum
output current for the buck boost topology can be calculated from the following equation.
Doc ID 023128 Rev 137/45
Application ideasA7985A
Equation 40
I
OUT
-------------
1D–
2 A<=
I
SW
where I
is the average current in the embedded power MOSFET in the ON time.
SW
To chose the right value of the inductor and to manage transient output current, which, for a
short time, can exceed the maximum output current calculated by Equation 40, also the
peak current in the power MOSFET must be calculated. The peak current, shown in
Equation 41, must be lower than the minimum current limit (2.5 A).
Equation 41
I
SW,PK
--------------------------------------------
r
I
OUT
OUT
-------------
1D–
V
OUT
LF
⋅⋅
1
SW
r
-- -+3.7A<⋅=
2
⋅=
1D–()
2
I
where r is defined as the ratio between the inductor current ripple and the inductor DC
current.
Therefore, in the buck boost topology the maximum output current depends on the
application conditions (firstly input and output voltage, secondly switching frequency and
inductor value).
In Figure 35 the maximum output current for the above configuration is depicted, varying the
input voltage from 4.5 V to 38 V.
The dashed line considers a more accurate estimation of the duty cycles given by Equation
42, where power losses across diodes, the external power MOSFET, and the internal power
MOSFET are taken into account.
Figure 35. Maximum output current according to max. DC switch current (2.0 A):
The A7985A can implement the step-up/down converter with a negative output voltage.
Figure 34 shows the schematic to regulate -5 V: no further external components are added
to the standard buck topology.
The relationship between input and output voltage is:
Equation 43
so the duty cycle is:
Equation 44
V
OUT
D
VIN–
V
OUT
------------------------------- -=
V
OUTVIN
across the internal and
SWE
D
-------------
⋅=
1D–
–
As in the positive one, in the inverting buck-boost the current flowing through the power
MOSFET is transferred to the load only during the OFF time. So according to the maximum
DC switch current (2.0 A), the maximum output current can be calculated from Equation 40,
where the duty cycle is given by Equation 44.
Figure 36. Inverting buck-boost regulator
Doc ID 023128 Rev 139/45
Application ideasA7985A
The GND pin of the device is connected to the output voltage so, given the output voltage,
the input voltage range is limited by the maximum voltage the device can withstand across
VCC and GND (38 V). Therefore, if the output is -5 V, the input voltage can range from 4.5 V
to 33 V.
As in the positive buck-boost, the maximum output current according to application
conditions is shown in Figure 37. The dashed line considers a more accurate estimation of
the duty cycles given by Equation 45, where power losses across diodes and the internal
power MOSFET are taken into account.
Figure 37. Maximum output current according to switch max. peak current (2.0 A):
V
=-5 V
O
40/45Doc ID 023128 Rev 1
A7985APackage mechanical data
8 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
packages, depending on their level of environmental compliance. ECOPACK®
®
is an ST trademark.
Table 10.HSOP8 mechanical data
mminch
Dim
Min.Typ.Max.Min.Typ.Max.
A1.70 0.0669
A10.000.1500.000.0059
A21.250.0492
b0.310.510.01220.0201
c0.170.250.00670.0098
D4.804.905.000.18900.19290.1969
E5.806.006.200.22830.23620.2441
E13.803.904.000.14960.15350.1575
e1.270.0500
h0.250.500.00980.0197
L0.401.270.01570.0500
k0.008.000.3150
ccc0.100.0039
Doc ID 023128 Rev 141/45
Package mechanical dataA7985A
Figure 38. Package dimensions
$MM4YP
%MM4YP
!-V
42/45Doc ID 023128 Rev 1
A7985AOrder codes
9 Order codes
Table 11.Order codes
Order codesPackagePackaging
A7985AHSOP8Tube
A7985ATRHSOP8Tape and reel
Doc ID 023128 Rev 143/45
Revision historyA7985A
10 Revision history
Table 12.Document revision history
DateRevisionChanges
19-Apr-20121Initial release.
44/45Doc ID 023128 Rev 1
A7985A
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