LT8631
13
8631fa
For more information www.linear.com/LT8631
APPLICATIONS INFORMATION
Choosing the Output Voltage
The output voltage is programmed with a resistor divider
between the output and the FB pin. Choose the 1% resis
-
tors according to:
R1= R2
V
OUT
0.808
1
Reference designators refer to the Block Diagram in
Figure 1.
If low input quiescent current and good light-load efficiency
are desired, use large resistor values for the FB resistor
divider. The current flowing in the divider acts as a load
current, and will increase the no-load input current to the
converter, which is approximately:
I
Q
= I
QVIN
+ I
QVOUT
+
V
OUT
R1+R2
V
OUT
V
IN
1
n
where I
QVIN
is the quiescent current of the LT8631 and the
second term is the quiescent current drawn from the output
(Iqvout) plus current in the feedback divider reflected to
the input of the buck operating at its light load efficiency
n. For a 5V application with R1 = 1MΩ and R2 = 191kΩ,
the feedback divider draws 4.2µA. With V
IN
= 12V I
QVIN
= 3.6µA, I
QVOUT
= 10µA and n = 50%, the no-load quies-
cent current is approximately 16µA. For applications with
output
voltages less than 2.8V, I
QVOUT
= 0µA and I
QVIN
is
typically 16µA. Graphs of I
QVIN
and I
QVOUT
vs V
OUT
are in
the Typical Performance Characteristics section.
When using FB resistors greater than 200k, a 4.7pF to 10pF
phase lead capacitor should be connected from V
OUT
to FB.
Choosing the Switching Frequency
The LT8631 switching frequency can be programmed over
a 100kHz to 1MHz range by using a resistor tied from RT
to ground. A table showing the necessary R
T
value for a
desired switching frequency is shown in Table 1.
The switching frequency selected determines the efficiency,
solution size, and input voltage range for the desired
frequency. High frequency operation permits the use
of
smaller
inductor and capacitor values which reduces the
overall solution size. However, as the switching frequency
increases. efficiency decreases as well as the input voltage
range for constant frequency operation.
Table 1. SW Frequency vs R
T
Value
FREQUENCY (kHz) R
RT
(kΩ)
100 187
200 60.4
300 35.7
400 25.5
500 19.6
600 15.8
700 13.3
800 11.5
900 10
1000 8.66
Switching Frequency and Input Voltage Range
Once the switching frequency has been determined, the
input voltage range for fixed frequency operation of the
regulator can be determined.
The minimum input voltage for fixed frequency operation
is determined by either the V
IN
undervoltage lockout, or
the following equation:
V
IN(MIN)
=
V
OUT
+ V
SW(BOT)
1 f
SW
t
OFF(MIN)
V
SW(BOT)
+ V
SW(TOP)
where V
OUT
is the output voltage, V
SW(TOP)
and V
SW(BOT)
are the internal switch drops (~0.775V, ~0.550V, respec-
tively at maximum load), F
SW
is the switching frequency
(set by RT), and t
OFF(MIN)
is the minimum switch off-time
(see the Electrical Characteristics).
If the input voltage falls below V
IN(MIN)
(dropout mode), the
LT8631 will automatically reduce the switching frequency
from the programmed value to obtain the highest possible
output voltage. The lower limit on the switching frequency
in dropout mode is determined by the boost threshold.
When the voltage between the BST and SW pins is less
than the boost threshold, a minimum off-time pulse is
generated to recharge the boost capacitor.
LT8631
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The maximum input voltage for fixed frequency operation
is determined by either the 100V maximum input voltage,
or the following equation:
F
SW(MAX)
=
V
OUT
+ V
SW(BOT)
t
ON(MIN)
V
IN
V
SW(TOP)
+ V
SW(BOT)
( )
where V
IN
is the typical input voltage, V
OUT
is the output
voltage, V
SW(TOP)
and V
SW(BOT)
are the internal switch
drops (~0.775V, ~0.550V, respectively at maximum load)
and t
ON(MIN)
is the minimum top switch on-time (see the
Electrical Characteristics).
If the input voltage rises above V
IN(MAX)
, the LT8631 will
automatically reduce the switching frequency from the
programmed value to maintain output regulation.
Inductor Selection and Maximum Output Current
A good first choice for the inductor value is:
L =
V
OUT
+ V
SW(BOT)
0.6 f
SW
where f
SW
is the switching frequency in MHz, V
OUT
is the
output voltage, and V
SW(BOT)
is the bottom switch drop
(~0.550V) and L is the inductor value in µH.
The inductor must be chosen with an RMS current rating
that is greater than the maximum expected output load of
the application. In addition, the saturation current (typically
labeled ISAT) rating of the inductor must be higher than
the load current plus 1/2 of the inductor ripple current:
I
L(PEAK)
= I
LOAD(MAX)
+ 1/2 ΔIL
where ΔIL is the inductor ripple current and I
LOAD(MAX)
is
the maximum output load for a given application.
The peak-to-peak ripple current in the inductor can be
calculated as follows:
ΔIL =
V
OUT
L F
SW
1
V
OUT
V
IN(MAX)
where F
SW
is the switching frequency in MHz and L is
the value of the inductor in µH. Therefore, the maximum
output current that the LT8631 will deliver depends on
the switch current limit, the inductor value, and the input
and output voltages. The inductor value may have to be
increased if the inductor ripple current does not allow suf
-
ficient maximum current (I
OUT(MAX)
) given the switching
frequency and maximum input voltage used in the desired
application.
Overload or short-circuit conditions can cause the induc
-
tor current to exceed the LT8631's peak current limit in
less
than the typical minimum on-time (tonmin) of 100ns.
Once the LT8631's typical peak current limit (Ilimpk) of
2A is exceeded, it will not switch on until the current in
the inductor has dropped below the peak current limit. If
the loaded/shorted condition still exists when the LT8631
resumes switching, the maximum inductor current will
be greater than the LT8631 peak current and at worst
case will be:
I
L(MAX)
=
V
INMAX
L
tonmin +Ilimpk
The LT8631 safely tolerates this condition. However, if
this condition can occur, the ISAT rating of the inductor
should be increased from I
L(PEAK)
to I
L(MAX)
.
The optimum inductor for a given application may differ
from the one indicated by this design guide. A larger value
inductor provides a higher maximum load current and
reduces the output voltage ripple. For applications requir
-
ing smaller
load currents, the value of the inductor may
be
lower and the LT8631 may operate with higher ripple
current. This allows use of a physically smaller inductor,
or one with a lower DCR resulting in higher efficiency. Be
aware that low inductance may result in discontinuous
mode operation, which further reduces maximum load
current.
For more information about maximum output current
and discontinuous operation, see Linear Technology’s
Application Note 44.
Finally, for duty cycles greater than 50% (V
OUT
/V
IN
> 0.5),
a minimum inductance is required to avoid subharmonic
oscillation. See Application Note 19.
Input Capacitor Selection
Bypass the LT8631 input with a 2.2µF or higher ceramic
capacitor of X7R or X5R type placed as close as possible
APPLICATIONS INFORMATION
LT8631
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8631fa
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to the V
IN
pin and ground. Y5V types have poor perfor-
mance over temperature and applied voltage, and should
not
be used. Note that larger input capacitance is required
when a lower switching frequency is used. If the input
power source has high impedance, or there is significant
inductance due to long wires or cables, additional bulk
capacitance may be necessary. This can be provided with
a low performance electrolytic capacitor.
A word of caution regarding the use of ceramic capacitors
at the input. A ceramic input capacitor can combine with
stray inductance to form a resonant tank circuit. If power
is applied quickly (for example, by plugging the circuit
into a live power source) this tank can ring, doubling the
input voltage and damaging the LT8631. The solution is to
either clamp the input voltage or dampen the tank circuit
by adding a lossy capacitor in parallel with the ceramic
capacitor. For details, see Application Note 88.
Output Capacitor Selection
The output capacitor has two essential functions. Along
with the inductor, it filters the square wave generated
by the LT8631 to produce the DC output. In this role it
determines the output ripple, thus low impedance at
the
switching
frequency is important. The second function
is to store energy in order to satisfy transient loads and
stabilize the LT8631's control loop. Since the LT8631 uses
current mode control, it does not require the presence of
output capacitor series resistance (ESR) for stability. Low
ESR or ceramic capacitors should be used to achieve very
low output ripple and small circuit size.
A 47µF, X5R or X7R ceramic capacitor with a voltage rating
greater than the desired output voltage is an excellent first
choice for most applications. The 47µF output capacitor
will provide low output ripple with good transient response.
Increasing the value will reduce the output voltage ripple and
improve transient response, but may increase application
cost and require more board space. Decreasing the value
may save cost and board space but will increase output
voltage ripple, degrade transient performance, and may
cause loop instability. Increasing or decreasing the output
capacitor may require increasing or decreasing the 4.7pF
feedforward capacitor placed between the V
OUT
and FB
pins to optimize transient response. See the Typical Ap-
plications section in the data sheet for suggested output
and feedforward capacitor values.
Note that even X5R and
X7R type ceramic capacitors have
a
DC bias effect which reduces their capacitance when a
DC voltage is applied. It is not uncommon for capacitors
offered in the smallest case sizes to lose more than 50%
of their capacitance when operated near their rated volt
-
age. As
a result it is sometimes necessary to use a larger
capacitance
value, larger case size, or use a higher voltage
rating in order to realize the intended capacitance value.
Consult the manufacturer’s data for the capacitor you
select to be assured of having the necessary capacitance
for the application.
Ceramic Capacitors
Ceramic capacitors are small, robust, and have very low
ESR. However, ceramic capacitors can cause problems
when used with the LT8631 due to their piezoelectric nature.
When in Burst Mode operation, the LT8631's switching
frequency depends on the load current, and at very light
loads the LT8631 can excite the ceramic capacitor at audio
frequencies, generating audible noise. Since the LT8631
operates at a lower current limit during Burst Mode opera
-
tion, the noise is typically very quiet to the casual ear. If this
noise is unacceptable, use a high performance tantalum
or electrolytic capacitor at the output.
Low noise ceramic
capacitors are also available.
Enable Pin
The
LT8631 is in shutdown when the EN/UV pin is low
and active when the pin is high. The rising threshold of
the EN/UV comparator is 1.19V, with 17mV of hysteresis.
The EN/UV pin can be tied to V
IN
if the shutdown feature
is not used, or tied to a logic level if shutdown control is
required.
Adding a resistor divider from V
IN
to EN/UV programs the
LT8631 to regulate the output only when V
IN
is above a
desired voltage (see the Block Diagram). Typically, the
EN/UV threshold is used in situations where the supply is
current limited, or has a relatively high source resistance. A
switching regulator draws constant power from the source,
APPLICATIONS INFORMATION

LT8631IFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 100V, 1A Synchronous Micropower Step-Down Regulator
Lifecycle:
New from this manufacturer.
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