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PDF LT1944-1 Data sheet ( Hoja de datos )
| Número de pieza | LT1944-1 | |
| Descripción | Dual Micropower Step-Up DC/DC Converter | |
| Fabricantes | Linear | |
| Logotipo |  |
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FEATURES
s Low Quiescent Current:
20µA in Active Mode
<1µA in Shutdown Mode
s Operates with VIN as Low as 1.2V
s Low VCESAT Switches: 85mV at 70mA
s Uses Small Surface Mount Components
s High Output Voltage: Up to 34V
s Tiny 10-Pin MSOP Package
U
APPLICATIO S
s Small TFT LCD Panels
s Handheld Computers
s Battery Backup
s Digital Cameras
LT1944-1
Dual Micropower Step-Up
DC/DC Converter
DESCRIPTIO
The LT®1944-1 is a dual micropower step-up DC/DC
converter in a 10-pin MSOP package. One converter is
designed with a 100mA current limit and a 400ns off-time;
the other with a 175mA current limit and a 1.5µs off-time.
The 1.5µs off-time converter is ideal for generating an
output voltage that is close to the input voltage (i.e. a Li-
Ion to 5V converter, or a two-cell to 3.3V converter). With
an input voltage range of 1.2V to 15V, the LT1944-1 is ideal
for a wide variety of applications. Both converters feature
a quiescent current of only 20µA at no load, which further
reduces to 0.5µA in shutdown. A current limited, fixed off-
time control scheme conserves operating current, result-
ing in high efficiency over a broad range of load current.
Tiny, low profile inductors and capacitors can be used to
minimize footprint and cost in space-conscious portable
applications.
, LTC and LT are registered trademarks of Linear Technology Corporation.
TYPICAL APPLICATIO
Triple Output Power Supply (5V, 15V, –10V) for LCD Displays
VIN
2.7V
TO 4.2V
C1
4.7µF
L1
22µH
D1
8
VIN
4
SHDN2
6
4.7pF
SW2
5
FB2
LT1944-1
2
SHDN1
1
FB1
GND PGND PGND SW1
3 7 9 10
5V
40mA
1M
C2
4.7µF
324k
178k
L2
22µH
C1, C2: TAIYO YUDEN JMK212BJ475
C3, C4: TAIYO YUDEN EMK212BJ105
C5: TAIYO YUDEN EMK107BJ104
D1, D2, D3, D4: CENTRAL SEMI CMDSH3
L1, L2: MURATA LQH3C220
4.7pF
D2
2M
C5
0.1µF
D3
5V
D4
C3
1µF
15V
2.5mA
C4
1µF
–10V
1944-1 TA01 1mA
90
85
80
75
70
65
60
55
50
0.1
5V Output Efficiency
VIN = 4.2V
VIN = 2.7V
1 10
LOAD CURRENT (mA)
100
1944-1 TA01a
1
1 page  
LT1944-1
APPLICATIO S I FOR ATIO
Choosing an Inductor
Several recommended inductors that work well with the
LT1944-1 are listed in Table 1, although there are many
other manufacturers and devices that can be used. Con-
sult each manufacturer for more detailed information and
for their entire selection of related parts. Many different
sizes and shapes are available. Use the equations and
recommendations in the next few sections to find the
correct inductance value for your design.
Table 1. Recommended Inductors
PART
VALUE (µH) MAX DCR (Ω)
LQH3C4R7 4.7 0.26
LQH3C100 10 0.30
LQH3C220 22 0.92
CD43-4R7
CD43-100
CDRH4D18-4R7
CDRH4D18-100
4.7
10
4.7
10
0.11
0.18
0.16
0.20
DO1608-472
DO1608-103
DO1608-223
4.7
10
22
0.09
0.16
0.37
VENDOR
Murata
(714) 852-2001
www.murata.com
Sumida
(847) 956-0666
www.sumida.com
Coilcraft
(847) 639-6400
www.coilcraft.com
systems with output voltages below 7V, a 10µH inductor
is the best choice, even though the equation above might
specify a smaller value. This is due to the inductor current
overshoot that occurs when very small inductor values are
used (see Current Limit Overshoot section).
For higher output voltages, the formula above will give
large inductance values. For a 2V to 20V converter (typical
LCD Bias application), a 74µH inductor is called for with
the above equation, but a 22µH inductor could be used
without excessive reduction in maximum output current.
Inductor Selection—SEPIC Regulator
The formula below calculates the approximate inductor
value to be used for a SEPIC regulator using the LT1944-1.
As for the boost inductor selection, a larger or smaller
value can be used.
L
=
2
VOUT +
ILIM
VD
tOFF
Inductor Selection—Boost Regulator
The formula below calculates the appropriate inductor
value to be used for a boost regulator using the LT1944-1
(or at least provides a good starting point). This value
provides a good tradeoff in inductor size and system
performance. Pick a standard inductor close to this value.
A larger value can be used to slightly increase the available
output current, but limit it to around twice the value
calculated below, as too large of an inductance will in-
crease the output voltage ripple without providing much
additional output current. A smaller value can be used
(especially for systems with output voltages greater than
12V) to give a smaller physical size. Inductance can be
calculated as:
( )VOUT − VIN MIN + VD
L = ILIM tOFF
where VD = 0.4V (Schottky diode voltage), ILIM = 100mA
(or 175mA) and tOFF = 400ns (or 1.5µs); for designs with
varying VIN such as battery powered applications, use the
minimum VIN value in the above equation. For most
Current Limit Overshoot
For the constant off-time control scheme of the LT1944-1,
the power switch is turned off only after the current limit
is reached. There is a 100ns delay between the time when
the current limit is reached and when the switch actually
turns off. During this delay, the inductor current exceeds
the current limit by a small amount. The peak inductor
current can be calculated by:
IPEAK
=
ILIM
+
VIN(MAX) −
L
VSAT
100ns
Where VSAT = 0.25V (switch saturation voltage). The
current overshoot will be most evident for systems with
high input voltages and for systems where smaller induc-
tor values are used. This overshoot can be beneficial as it
helps increase the amount of available output current for
smaller inductor values. This will be the peak current seen
by the inductor (and the diode) during normal operation.
For designs using small inductance values (especially at
input voltages greater than 5V), the current limit over-
shoot can be quite high. Although it is internally current
5
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| Páginas | Total 8 Páginas | |
| PDF Descargar | [ Datasheet LT1944-1.PDF ] | |
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