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pin Functions
is charging, the peak supply current will be approximately
equal to 2.2 times the output current. During the time that
C
IN
is delivering charge to C
OUT
the supply current drops
to approximately 0.2 times the output current. An input
supply bypass capacitor will supply part of the peak input
current drawn by the LT1054 and average out the current
drawn from the supply. A minimum input supply bypass
capacitor of 2µF, preferably tantalum or some other low ESR
type is recommended. A larger capacitor may be desirable
in some cases, for example, when the actual input supply
is connected to the LT1054 through long leads, or when
the pulse current drawn by the LT1054 might affect other
circuitry through supply coupling.
applications inFormation
Theory of Operation
To understand the theory of operation of the LT1054, a re-
view of a basic switched-capacitor building block is helpful.
In Figure 3 when the switch is in the left position, capaci-
tor C1 will charge to voltage V1. The total charge on C1
will be q1 = C1V1. The switch then moves to the right,
discharging C1 to voltage V2. After this discharge time
the charge on C1 is q2 = C1V2. Note that charge has been
transferred from the sour
ce V1 to the output V2. The
amount of charge transferred is:
q = q1 – q2 = C1(V1 – V2)
If the switch is cycled f times per second, the charge
transfer per unit time (i.e., current) is:
I = (f)(q) = (f)[C1(V1 – V2)]
To obtain an equivalent resistance for the switched-
capacitor network we can rewrite this equation in terms
of voltage and impedance equivalence:
I=
V1– V2
1/ fC1
=
V1– V2
R
EQUIV
A new variable R
EQUIV
is defined such that R
EQUIV
= 1/fC1.
Thus the equivalent circuit for the switched-capacitor
network is as shown in Figure 4. The LT1054 has the same
switching action as the basic switched-capacitor building
block. Even though this simplification doesn’t include finite
switch on-resistance and output voltage ripple, it provides
an intuitive feel for how the device works.
These simplified circuits explain voltage loss as a function
of frequency (see Typical Performance Characteristics).
As frequency is decreased, the output impedance will
eventually be dominated by the 1/fC1 term and voltage
losses will rise.
Note that losses also rise as frequency increases. This is
caused by internal switching losses which occur due to
some finite charge being lost on each switching cycle. This
charge loss per-unit-cycle, when multiplied by the switching
frequency, becomes a current loss. At high frequency this
loss becomes significant and voltage losses again rise.
The oscillator of the LT1054 is designed to run in the
frequency band where voltage losses are at a minimum.
Regulation
T
he error amplifier of the LT1054 servos the drive to the
PNP switch to control the voltage across the input capaci-
tor (C
IN
) which in turn will determine the output voltage.
Using the reference and error amplifier of the LT1054,
an external resistive divider is all that is needed to set
the regulated output voltage. Figure 5 shows the basic
regulator configuration and the formula for calculating
the appropriate resistor values. R1 should be chosen to
f
C1
C2
R
L
V2
LT1054 • F03
V1
Figure 3. Switched-Capacitor Building Block
Figure 3. Switched-Capacitor Equivalent Circuit
C2
R
L
R
EQUIV
R
EQUIV
=
V2
LT1054 • F04
V1
1
fC1
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applications inFormation
R4
RESTART SHUTDOWN
C1
R2
C
IN
10µF
TANTALUM
C
OUT
100µF
TANTALUM
V
OUT
LT1054 • F05
V
IN
R1
2.2µF
R3
R2
R1
= + 1
WHERE V
REF
= 2.5V NOMINAL
*CHOOSE THE CLOSEST 1% VALUE
FOR EXAMPLE: TO GET V
OUT
= –5V REFERRED TO THE GROUND
PIN OF THE LT1054, CHOOSE R1 = 20k, THEN
|V
OUT
|
)
)
V
REF
2
– 40mV
R2 = 20k
= 102.6k*
+ 1
|5V|
)
)
2.5V
2
– 40mV
)
)
+ 1
|V
OUT
|
1.21V
LT1054
FB/SHDN
CAP
+
GND
CAP
V
+
OSC
V
REF
V
OUT
+
+
+
be 20k or greater because the reference output current
is limited to ≈100µA. R2 should be chosen to be in the
range of 100k to 300k. For optimum results the ratio of
C
IN
/C
OUT
is recommended to be 1/10. C1, required for
good load regulation at light load currents, should be
0.002µF for all output voltages.
A new die layout was required to fit into the physical
dimensions of the S8 package. Although the new die
of the LT1054CS8 will meet all the specifications of the
existing LT1054 data sheet, subtle differences in the
layout of the new die require consideration in some ap
-
plication circuits. In regulating mode circuits using the
1054CS8 the nominal values of the capacitors, C
IN
and
C
OUT
, must be approximately equal for proper operation
at elevated junction temperatures. This is different from
the earlier part. Mismatches within normal production
tolerances for the capacitors are acceptable. Making the
nominal capacitor values equal will ensure proper opera
-
tion at elevated junction temperatures at the cost of a
small degradation in the transient response of regulator
cir
cuits. For unregulated cir
cuits the values of C
IN
and
C
OUT
are normally equal for all packages. For S8 applica-
tions assistance in unusual applications circuits, please
consult the factory
.
It can be seen from the circuit block diagram that the
maximum regulated output voltage is limited by the supply
voltage. For the basic configuration,
|V
OUT
| referred to the
ground pin of the LT1054 must be less than the total of the
supply voltage minus the voltage loss due to the switches.
The voltage loss versus output current due to the switches
can be found in Typical Performance Characteristics. Other
configurations such as the negative doubler can provide
higher output voltages at reduced output currents (see
Typical Applications).
Capacitor Selection
For unregulated circuits the nominal values of C
IN
and C
OUT
should be equal. For regulated circuits see the section on
Regulation. While the exact values of C
IN
and C
OUT
are
noncritical, good quality, low ESR capacitors such as solid
tantalum are necessary to minimize voltage losses at high
currents. For C
IN
the effect of the ESR of the capacitor will
be multiplied by four due to the fact that switch currents
are approximately two times higher than output current and
losses will occur on both the charge and discharge cycle.
This means that using a capacitor with 1Ω of ESR for C
IN
will have the same effect as increasing the output imped-
ance of the LT1054 by 4Ω. This represents a significant
increase in the voltage losses. For C
OUT
the affect of ESR is
less dramatic. C
OUT
is alternately charged and discharged
at a current approximately equal to the output current and
the ESR of the capacitor will cause a step function to oc
-
cur in the output ripple at the switch transitions. This step
function will degrade the output regulation for changes
in output load current and should be avoided. Realizing
that large value tantalum capacitors can be expensive, a
technique that can be used is to parallel a smaller tantalum
capacitor with a large aluminum electrolytic capacitor to
gain both low ESR and reasonable cost. Where physical
size is a concern some of the newer chip type surface
mount tantalum capacitors can be used. These capacitors
are normally rated at working voltages in the 10V to 20V
range and exhibit very low ESR (in the range of 0.1Ω).
Output Ripple
The peak-to-peak output ripple is determined by the value
of the output capacitor and the output current. Peak-to-
peak output ripple may be approximated by the formula:
dV =
I
OUT
2fC
OUT
Figure 5
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applications inFormation
where dV = peak-to-peak ripple and f = oscillator frequency.
For output capacitors with significant ESR a second term
must be added to account for the voltage step at the switch
transitions. This step is approximately equal to:
(2I
OUT
)(ESR of C
OUT
)
Power Dissipation
The power dissipation of any LT1054 circuit must be
limited such that the junction temperature of the device
does not exceed the maximum junction temperature rat
-
ings. The total power dissipation must be calculated from
two components, the power loss due to voltage drops
in the switches and the power loss due to drive current
losses.
The
total power dissipated by the LT1054 can be
calculated from:
P ≈ (V
IN
|V
OUT
|)(I
OUT
) + (V
IN
)(I
OUT
)(0.2)
where both V
IN
and V
OUT
are referred to the ground pin
(Pin3) of the LT1054. For LT1054 regulator circuits, the
power dissipation will be equivalent to that of a linear
regulator. Due to the limited power handling capability of
the LT1054 packages, the user will have to limit output
current requirements or take steps to dissipate some power
external to the LT1054 for large input/output differentials.
This can be accomplished by placing a resistor in series
with C
IN
as shown in Figure 6. A portion of the input
voltage will then be dropped across this resistor without
affecting the output regulation. Because switch current is
approximately 2.2 times the output current and the resistor
will cause a voltage drop when C
IN
is both charging and
discharging, the resistor should be chosen as:
R
X
= V
X
/(4.4 I
OUT
)
where:
V
X
≈ V
IN
– [(LT1054 Voltage Loss)(1.3) + |V
OUT
|]
and I
OUT
= maximum required output current. The factor
of 1.3 will allow some operating margin for the LT1054.
For example: assume a 12V to –5V converter at 100mA
output current. First calculate the power dissipation without
an external resistor:
P = (12V –
| 5V|)(100mA) + (12V)(100mA)(0.2)
P = 700mW + 240mW = 940mW
At θ
JA
of 130°C/W for a commercial plastic device this
would cause a junction temperature rise of 122°C so that
the device would exceed the maximum junction tempera
-
ture at an ambient temperature of 25°C. Now calculate the
power dissipation with an external resistor (R
X
). First find
how much voltage can be dropped across R
X
. The maxi-
mum voltage loss of the LT1054 in the standard regulator
configuration at 100mA output current is 1.6V, so:
V
X
= 12V – [(1.6V)(1.3) + | 5V|] = 4.9V and
R
X
= 4.9V/(4.4)(100mA) = 11Ω
This resistor will reduce the power dissipated by the
LT1054 by (4.9V)(100mA) = 490mW. The total power dis
-
sipated by the LT1054 would then be (940mW – 490mW)
= 450mW. The junction temperature rise would now be
only 58°C. Although commercial devices are guaranteed
to be functional up to a junction temperature of 125°C, the
specifications are only guaranteed up to a junction tem
-
perature of 100°C, so ideally you should limit the junction
temperature to 100°C. For the above example this would
mean limiting the ambient temperature to 42°C. Other
steps can be taken to allow higher ambient temperatures.
The
thermal resistance
numbers for the LT1054 packages
represent worst-case numbers with no heat sinking and
still air. Small clip-on type heat sinks can be used to lower
the thermal resistance of the LT1054 package. In some
systems there may be some available airflow which will
help to lower the thermal resistance. Wide PC board traces
from the LT1054 leads can also help to remove heat from
the device. This is especially true for plastic packages.
C1
R2
C
IN
C
OUT
V
OUT
LT1054 • F06
V
IN
R1
R
X
LT1054
FB/SHDN
CAP
+
GND
CAP
V
+
OSC
V
REF
V
OUT
+
+
Figure 6

LT1054IS8#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Linear Voltage Regulators 100mA Sw Cap Volt Converter
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