25
LT1956/LT1956-5
1956f
current in L2 and C4 flows via the catch diode D3, charging
the negative output capacitor C6. If the negative output is
not loaded enough, it can go severely unregulated (be-
come more negative). Figure 14b shows the maximum
allowable –5V output load current (vs load current on the
5V output) that will maintain the –5V output within 3%
tolerance. Figure 14c shows the –5V output voltage regu-
lation vs its own load current when plotted for three
separate load currents on the 5V output. The efficiency of
the dual output converter circuit shown in Figure 14a is
given in Figure 14d.
POSITIVE-TO-NEGATIVE CONVERTER
The circuit in Figure 15 is a positive-to-negative topology
using a grounded inductor. It differs from the standard
approach in the way the IC chip derives its feedback signal
because the LT1956 accepts only positive feedback sig-
nals. The ground pin must be tied to the regulated negative
output. A resistor divider to the FB pin, then provides the
proper feedback voltage for the chip.
The following equation can be used to calculate maximum
load current for the positive-to-negative converter:
APPLICATIO S I FOR ATIO
WUUU
I
I
VV
VVfL
VV
VV VV
MAX
P
IN OUT
OUT IN
OUT IN
OUT IN OUT F
=
+
++
()( )
()()()
()(.)
(–.)()
2
03
03
I
P
= maximum rated switch current
V
IN
= minimum input voltage
V
OUT
= output voltage
V
F
= catch diode forward voltage
0.3 = switch voltage drop at 1.5A
Example: with V
IN(MIN)
= 5.5V, V
OUT
= 12V, L = 15µH,
V
F
= 0.63V, I
P
= 1.5A: I
MAX
= 0.36A.
INDUCTOR VALUE
The criteria for choosing the inductor is typically based on
ensuring that peak switch current rating is not exceeded.
This gives the lowest value of inductance that can be used,
but in some cases (lower output load currents) it may give
a value that creates unnecessarily high output ripple
voltage.
The difficulty in calculating the minimum inductor size
needed is that you must first decide whether the switcher
will be in continuous or discontinuous mode at the critical
point where switch current reaches 1.5A. The first step is
to use the following formula to calculate the load current
above which the switcher must use continuous mode. If
your load current is less than this, use the discontinuous
mode formula to calculate minimum inductor needed. If
load current is higher, use the continuous mode formula.
Output current where continuous mode is needed:
I
VI
VV VV V
CONT
IN P
IN OUT IN OUT F
>
+++
()()
()( )
22
4
Minimum inductor discontinuous mode:
OUTPUT**
–12V, 0.25A
V
IN
12V
1956 F15
C2
0.1µF
C
C
R
C
D1
10MQO60N
R1
36.5k
C1
100µF
20V TANT
C3
2.2µF
25V
D2
MMSD914TI
L1*
7µH
C
F
BOOST
LT1956
V
IN
SW
FB
GND
V
C
R2
4.12k
* INCREASE L1 TO 10µH OR 18µH FOR HIGHER CURRENT APPLICATIONS.
SEE APPLICATIONS INFORMATION
** MAXIMUM LOAD CURRENT DEPENDS ON MINIMUM INPUT VOLTAGE
AND INDUCTOR SIZE. SEE APPLICATIONS INFORMATION
+
Figure 15. Positive-to-Negative Converter
26
LT1956/LT1956-5
1956f
U
PACKAGE DESCRIPTIO
Minimum inductor continuous mode:
L
VV
fV V I I
VV
V
MIN
IN OUT
IN OUT P OUT
OUT F
IN
=
++
+
()( )
()( )
()
21
For a 12V to –12V converter using the LT1956 with peak
switch current of 1.5A and a catch diode of 0.63V:
IA
CONT
>
+++
=
()(.)
()( .)
.
12 1 5
412121212063
0 370
22
For a load current of 0.25A, this says that discontinuous
mode can be used and the minimum inductor needed is
found from:
LH
MIN
==µ
212 025
500 10 1 5
53
32
()(.)
(•)(.)
.
In practice, the inductor should be increased by about
30% over the calculated minimum to handle losses and
variations in value. This suggests a minimum inductor of
7µH for this application.
Ripple Current in the Input and Output Capacitors
Positive-to-negative converters have high ripple current
in the input capacitor. For long capacitor lifetime, the
RMS value of this current must be less than the high
frequency ripple current rating of the capacitor. The
following formula will give an
approximate
value for RMS
ripple current.
This formula assumes continuous mode
and large inductor value
. Small inductors will give some-
what higher ripple current, especially in discontinuous
mode. The exact formulas are very complex and appear
in Application Note 44, pages 29 and 30. For our pur-
poses here I have simply added a fudge factor (ff). The
value for ff is about 1.2 for higher load currents and L
15µH. It increases to about 2.0 for smaller inductors at
lower load currents.
Capacitor I ff I
V
V
RMS OUT
OUT
IN
=()( )
ff = 1.2 to 2.0
The output capacitor ripple current for the positive-to-
negative converter is similar to that for a typical buck
regulator—it is a triangular waveform with peak-to-peak
value equal to the peak-to-peak triangular waveform of the
inductor. The low output ripple design in Figure 14 places
the input capacitor between V
IN
and the regulated negative
output. This placement of the input capacitor significantly
reduces the size required for the output capacitor (versus
placing the input capacitor between V
IN
and ground).
The peak-to-peak ripple current in both the inductor and
output capacitor (assuming continuous mode) is:
I
P-P
P-P
=
==
+
++
=
DC V
fL
DC Duty Cycle
VV
VVV
I RMS
I
IN
OUT F
OUT IN F
COUT
()
12
The output ripple voltage for this configuration is as low as
the typical buck regulator based predominantly on the
inductor’s triangular peak-to-peak ripple current and the
ESR of the chosen capacitor (see Output Ripple Voltage in
Applications Information).
Diode Current
Average
diode current is equal to load current.
Peak
diode
current will be considerably higher.
Peak diode current:
ContinuousMode
I
VV
V
VV
LfV V
DiscontinuousMode
IV
Lf
OUT
IN OUT
IN
IN OUT
IN OUT
OUT OUT
=
+
+
+
=
()()()
()()( )
()( )
()()
2
2
Keep in mind that during start-up and output overloads,
average diode current may be much higher than with
normal loads. Care should be used if diodes rated less than
1A are used, especially if continuous overload conditions
must be tolerated.
27
LT1956/LT1956-5
1956f
U
PACKAGE DESCRIPTIO
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen-
tation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
FE Package
16-Lead Plastic TSSOP (4.4mm)
(Reference LTC DWG # 05-08-1663)
Exposed Pad Variation BB
FE16 (BB) TSSOP 0203
0.09 – 0.20
(.0036 – .0079)
0
° – 8°
0.45 – 0.75
(.018 – .030)
4.30 – 4.50*
(.169 – .177)
6.40
BSC
134
5
6
7
8
10 9
4.90 – 5.10*
(.193 – .201)
16 1514 13 12 11
1.10
(.0433)
MAX
0.05 – 0.15
(.002 – .006)
0.65
(.0256)
BSC
2.94
(.116)
0.195 – 0.30
(.0077 – .0118)
2
RECOMMENDED SOLDER PAD LAYOUT
0.45 ±0.05
0.65 BSC
4.50 ±0.10
6.60 ±0.10
1.05 ±0.10
2.94
(.116)
3.58
(.141)
3.58
(.141)
MILLIMETERS
(INCHES)
*DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH
SHALL NOT EXCEED 0.150mm (.006") PER SIDE
NOTE:
1. CONTROLLING DIMENSION: MILLIMETERS
2. DIMENSIONS ARE IN
3. DRAWING NOT TO SCALE
SEE NOTE 4
4. RECOMMENDED MINIMUM PCB METAL SIZE
FOR EXPOSED PAD ATTACHMENT

LT1956IFE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Hi V, 1.5A, 500kHz Buck Sw Regs
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union