LT1939
13
1939f
APPLICATIONS INFORMATION
Discontinuous operation occurs when I
OUT
is less than
I
L
/2 as calculated above.
Figure 4 illustrates the inductance value needed for a 3.3V
output with a maximum load capability of 2A. Referring
to Figure 4, an inductor value between 3.3µH and 4.7µH
will be suffi cient for a 15V input voltage and a switch
frequency of 750kHz. There are several graphs in the
Typical Performance Characteristics section of this data
sheet that show inductor selection as a function of input
voltage and switch frequency for several popular output
voltages and output ripple currents. Also, low inductance
may result in discontinuous mode operation, which is
okay, but further reduces maximum load current. For
details of maximum output current and discontinuous
mode operation, see Linear Technology Application Note
44. Finally, for duty cycles greater than 50% (V
OUT
/V
IN
> 0.5), there is a minimum inductance required to avoid
subharmonic oscillations. See Application Note 19 for
more information.
capacitor is required to reduce the resulting voltage
ripple at the LT1939 and to force this very high frequency
switching current into a tight local loop, minimizing EMI.
The input capacitor must have low impedance at the
switching frequency to do this effectively, and it must
have an adequate ripple current rating.
A conservative value is the RMS input current is given
by:
I
CIN(RMS)
=
I
OUT1
V
OUT1
•V
IN
V
OUT1
()
0.5
V
IN
<
I
OUT1
2
and is largest when V
IN
= 2V
OUT1
(50% duty cycle).
The frequency, V
IN
to V
OUT
ratio, and maximum load
current requirement of the LT1939 along with the input
supply source impedance, determine the energy storage
requirements of the input capacitor. Determine the worst-
case condition for input ripple current and then size the
input capacitor such that it reduces input voltage ripple to
an acceptable level. Typical values for input capacitors run
from 10µF at low frequencies to 2.2µF at higher frequencies.
The combination of small size and low impedance (low
equivalent series resistance or ESR) of ceramic capacitors
make them the preferred choice. The low ESR results in
very low voltage ripple and the capacitors can handle plenty
of ripple current. They are also comparatively robust and
can be used in this application at their rated voltage. X5R
and X7R types are stable over temperature and applied
voltage, and give dependable service. Other types (Y5V and
Z5U) have very large temperature and voltage coeffi cients
of capacitance, so they may have only a small fraction of
their nominal capacitance in your application. While they
will still handle the RMS ripple current, the input voltage
ripple may become fairly large, and the ripple current may
end up fl owing from your input supply or from other by-
pass capacitors in your system, as opposed to being fully
sourced from the local input capacitor. An alternative to a
high value ceramic capacitor is a lower value along with
a larger electrolytic capacitor, for example a 1µF ceramic
capacitor in parallel with a low ESR tantalum capacitor.
For the electrolytic capacitor, a value larger than 10µF will
be required to meet the ESR and ripple current require-
ments. Because the input capacitor is likely to see high
Figure 4. Inductor Values for 2A Maximum Load Current
(V
OUT1
= 3.3V, I
RIPPLE
= 1A)
Input Capacitor Selection
Bypass the input of the LT1939 circuit with a 4.7µF or
higher ceramic capacitor of X7R or X5R type. A lower
value or a less expensive Y5V type can be used if there
is additional bypassing provided by bulk electrolytic or
tantalum capacitors. The following paragraphs describe
the input capacitor considerations in more detail.
Step-down regulators draw current from the input sup-
ply in pulses with very fast rise and fall times. The input
INPUT VOLTAGE (V)
5
250
FREQUENCY (kHz)
500
1000
1250
1500
2500
1939 F04
750
15
10
20 25
1750
2000
2250
L = 1µH
L = 1.5µH
L = 2.2µH
L = 3.3µH
L = 4.7µH
L = 6.8µH
LT1939
14
1939f
surge currents when the input source is applied, tantalum
capacitors should be surge rated. The manufacturer may
also recommend operation below the rated voltage of the
capacitor. Be sure to place the 1µF ceramic as close as
possible to the V
IN
and GND pins on the IC for optimal
noise immunity.
A fi nal caution regarding the use of ceramic capacitors for
input bypassing. 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 LT1939. 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
Typically step-down regulators are easily compensated with
an output crossover frequency that is 1/10 of the switch-
ing frequency. This means that the time that the output
capacitor must supply the output load during a transient
step is ~2 or 3 switching periods. With an allowable 5%
drop in output voltage during the step, a good starting
value for the output capacitor can be expressed by:
C
VOUT1
=
Max Load Step
Frequency 0.05 V
OUT1
Example:
V
OUT1
= 3.3V, Frequency = 1MHz, Max Load Step = 2A
C
VOUT1
=
2
1MHz 0.05 3.3
= 12μF
The calculated value is only a suggested starting value.
Increase the value if transient response needs improvement
or reduce the capacitance if size is a priority. The output
capacitor fi lters the inductor current to generate an output
with low voltage ripple. It also stores energy in order to
satisfy transient loads and to stabilize the LT1939’s control
loop. The switching frequency of the LT1939 determines
the value of output capacitance required. Also, the current
mode control loop doesn’t require the presence of output
capacitor series resistance (ESR). For these reasons, you
are free to use ceramic capacitors to achieve very low
output ripple and small circuit size. Estimate output ripple
with the following equations:
V
RIPPLE
=
I
L
8 Frequency C
OUT1
For ceramic capacitors and,
V
RIPPLE
= ΔI
L
• ESR
For electrolytic (tantalum and aluminum)
where ΔI
L
is the peak-to-peak ripple current in the
inductor.
The RMS content of this ripple is very low, and the RMS
current rating of the output capacitor is usually not of
concern.
Another constraint on the output capacitor is that it must
have greater energy storage than the inductor; if the stored
energy in the inductor is transferred to the output, you
would like the resulting voltage step to be small compared
to the regulation voltage. For a 5% overshoot, this require-
ment becomes:
C
OUT1
> 10 L
I
LIM
V
OUT1
2
Finally, there must be enough capacitance for good transient
performance. The last equation gives a good starting point.
Alternatively, you can start with one of the designs in this
data sheet and experiment to get the desired performance.
This topic is covered more thoroughly in the section on
loop compensation.
The high performance (low ESR), small size and robust-
ness of ceramic capacitors make them the preferred type
for LT1939 applications. However, all ceramic capacitors
are not the same. As mentioned above, many of the high
value capacitors use poor dielectrics with high tempera-
ture and voltage coeffi cients. In particular, Y5V and Z5U
types lose a large fraction of their capacitance with ap-
plied voltage and temperature extremes. Because the loop
stability and transient response depend on the value of
C
OUT
, you may not be able to tolerate this loss. Use X7R
and X5R types. You can also use electrolytic capacitors.
APPLICATIONS INFORMATION
LT1939
15
1939f
The ESRs of most aluminum electrolytics are too large to
deliver low output ripple. Tantalum and newer, lower ESR
organic electrolytic capacitors intended for power supply
use, are suitable and the manufacturers will specify the
ESR. The choice of capacitor value will be based on the
ESR required for low ripple. Because the volume of the
capacitor determines its ESR, both the size and the value
will be larger than a ceramic capacitor that would give you
similar ripple performance. One benefi t is that the larger
capacitance may give better transient response for large
changes in load current.
Catch Diode
The diode D1 conducts current only during switch off
time. Use a Schottky diode to limit forward voltage drop to
increase effi ciency. The Schottky diode must have a peak
reverse voltage that is equal to regulator input voltage and
sized for average forward current in normal operation.
Average forward current can be calculated from:
I
D(AVG)
=
I
OUT1
V
IN
•V
IN
V
OUT1
()
The only reason to consider a larger diode is the worst-
case condition of a high input voltage and shorted output.
With a shorted condition, diode current will increase to a
typical value of 3A, determined by the peak switch current
limit of the LT1939. This is safe for short periods of time,
but it would be prudent to check with the diode manu-
facturer if continuous operation under these conditions
can be tolerated.
BST Pin Considerations
The capacitor and diode tied to the BST pin generate
a voltage that is higher than the input voltage. In most
cases a 0.47µF capacitor and fast switching diode (such
as the CMDSH-3 or FMMD914) will work well. Almost
any type of fi lm or ceramic capacitor is suitable, but the
ESR should be <1 to ensure it can be fully recharged
during the off time of the switch. The capacitor value can
be approximated by:
C
BST
=
I
OUT1(MAX)
•DC
50 V
OUT1
V
BST(MIN)
()
f
where I
OUT1(MAX)
is the maximum load current, and
V
BST(MIN)
is the minimum boost voltage to fully saturate
the switch.
Figure 5 shows four ways to arrange the boost circuit.
The BST pin must be more than 2.2V above the SW pin
for full effi ciency.
APPLICATIONS INFORMATION
Figure 5. BST Pin Considerations
V
BST
– V
SW
= V
X
V
BST(MAX)
= V
X
V
X
> V
IN
+ 3V
(5d)(5c)
(5b)
V
BST
– V
SW
= V
IN
V
BST(MAX)
= 2 •V
IN
V
IN
V
IN
D2
D1
D1
D1
D1
(5a)
LT1939
LDRV
BST
SW
V
BST
– V
SW
= V
OUT1
V
BST(MAX)
= V
IN
+ V
OUT1
V
BST
– V
SW
= V
OUT2
V
BST(MAX)
= V
IN
+ V
OUT2
V
OUT2
2.5V
V
OUT1
V
OUT2
C3
V
IN
V
IN
D2
LT1939
LDRV
BST
SW
V
OUT1
V
IN
V
IN
LT1939
LDRV
BST
SW
V
OUT1
C3
V
IN
V
IN
D2
LT1939
LDRV
BST
SW
D2
V
OUT1
C3
1939 F05

LT1939EDD#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Monolithic 2A Step-Down Regulator Plus Linear Regulator/Controller
Lifecycle:
New from this manufacturer.
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