LTC1046CN8#PBF

LTC1046
4
1046fb
AMBIENT TEMPERATURE (°C)
–55
26
OSCILLATOR FREQUENCY, f
OSC
(kHz)
30
32
34
36
38
40
25 50 100 125
1046 G11
28
–25 0 75
V
+
= 5V
C
OSC
= 0pF
AMBIENT TEMPERATURE (°C)
0
1
OSCILLATOR FREQUENCY, f
OSC
(kHz)
10
100
1457
1046 G10
23 6
T
A
= 25°C
C
OSC
= 0pF
CCHARA TERIST
ICS
UW
AT
Y
P
I
CA
LPER
F
O
R
C
E
TEST CIRCUIT
Figure 1
Oscillator Frequency as a Oscillator Frequency vs
Function of Supply Voltage Temperature
(Using Test Circuit in Figure 1)
C
OSC
EXTERNAL
OSCILLATOR
C2
10µF
V
OUT
V
+
(5V)
R
L
I
S
I
L
1046 F01
1
2
3
4
8
7
6
5
V
+
OSC
LV
V
OUT
BOOST
CAP
+
GND
CAP
LTC1046
C1
10µF
+
+
EXTERNAL CAPACITOR (PIN 7 TO GND), C
OSC
(pF)
1
0.1
OSCILLATOR FREQUENCY, f
OSC
(kHz)
1
10
100
10 100 10000
1046 G09
1000
V
+
= 5V
T
A
= 25°C
PIN 1 = OPEN
PIN 1 = V
+
LOAD CURRENT, I
L
(mA)
0
2.5
OUTPUT VOLTAGE (V)
2.0
1.5
1.0
0.5
0.0
0.5
2
4
6
8
1046 G07
10 12 14 16 18 20
1.0
1.5
2.0
2.5
SLOPE = 52
T
A
= 25°C
V
+
= 2V
f
OSC
= 8kHz
C1 = C2 = 10µF
LOAD CURRENT, I
L
(mA)
0
–5
OUTPUT VOLTAGE (V)
–4
–3
–2
–1
0
1
10 20 30 40
1046 G08
50 60 70 80 90 100
2
3
4
5
SLOPE = 27
T
A
= 25°C
V
+
= 5V
f
OSC
= 30kHz
C1 = C2 = 10µF
Output Voltage vs Load Current Output Voltage vs Load Current Oscillator Frequency as a
for V
+
= 2V for V
+
= 5V Function of C
OSC
5
LTC1046
1046fb
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Theory of Operation
To understand the theory of operation of the LTC1046, a
review of a basic switched capacitor building block is
helpful.
In Figure 2, when the switch is in the left position, capacitor
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 source, 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).
Examination of Figure 4 shows that the LTC1046 has the
same switching action as the basic switched capacitor
building block. With the addition of finite switch ON
resistance and output voltage ripple, the simple theory,
although not exact, provides an intuitive feel for how the
device works.
For example, if you examine power conversion efficiency
as a function of frequency (see typical curve), this simple
theory will explain how the LTC1046 behaves. The loss,
and hence the efficiency, is set by the output impedance.
As frequency is decreased, the output impedance will
eventually be dominated by the 1/fC1 term and power
efficiency will drop. The typical curves for power effi-
ciency versus frequency show this effect for various capaci-
tor values.
Note also that power efficiency decreases as frequency
goes up. 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
the power efficiency starts to decrease.
Figure 3. Switched Capacitor Equivalent Circuit
Figure 4. LTC1046 Switched Capacitor
Voltage Converter Block Diagram
C2
R
EQUIV
=
1046 F03
V2V1
R
L
R
EQUIV
1
fC1
1046 F04
CAP
+
(2)
CAP
(4)
GND
(3)
V
OUT
(5)
V
+
(8)
LV
(6)
3x
(1)
OSC
(7)
OSC +2
CLOSED WHEN
V
+
> 3.0V
C1
C2
BOOST
SW1 SW2
φ
φ
+
+
Figure 2. Switched Capacitor Building Block
C1
f
C2
1046 F02
V2V1
R
L
Rewriting in terms of voltage and impedance equivalence,
I
VV
fC
VV
R
EQUIV
=
()
=
12
11
12
/
.
A new variable, R
EQUIV
, has been defined such that
R
EQUIV
= 1/fC1. Thus, the equivalent circuit for the switched
capacitor network is as shown in Figure 3.
LTC1046
6
1046fb
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LV (Pin 6)
The internal logic of the LTC1046 runs between V
+
and LV
(Pin 6). For V
+
greater than or equal to 3V, an internal
switch shorts LV to GND (Pin 3). For V
+
less than 3V, the
LV pin should be tied to ground. For V
+
greater than or
equal to 3V, the LV pin can be tied to ground or left floating.
OSC (Pin 7) and BOOST (Pin 1)
The switching frequency can be raised, lowered or driven
from an external source. Figure 5 shows a functional
diagram of the oscillator circuit.
By connecting the BOOST (Pin 1) to V
+
, the charge and
discharge current is increased and, hence, the frequency
is increased by approximately three times. Increasing the
frequency will decrease output impedance and ripple for
higher load currents.
Loading Pin 7 with more capacitance will lower the fre-
quency. Using the BOOST pin in conjunction with external
capacitance on Pin 7 allows user selection of the fre-
quency over a wide range.
Driving the LTC1046 from an external frequency source
can be easily achieved by driving Pin 7 and leaving the
BOOST pin open, as shown in Figure 6. The output current
from Pin 7 is small, typically 15µA, so a logic gate is
capable of driving this current. The choice of using a CMOS
logic gate is best because it can operate over a wide supply
voltage range (3V to 15V) and has enough voltage swing
to drive the internal Schmitt trigger shown in Figure 5. For
5V applications, a TTL logic gate can be used by simply
adding an external pull-up resistor (see Figure 6).
Capacitor Selection
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 1 of ESR for C
IN
will have the same effect as increasing the output imped-
ance of the LTC1046 by 4. This represents a significant
increase in the voltage losses. For C
OUT
the effect of ESR
is less dramatic. C
OUT
is alternately charged and dis-
charged at a current approximately equal to the output
current, and the ESR of the capacitor will cause a step
function to occur, 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 alumi-
num 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 0.1).
Figure 6. External Clocking
C2
V
+
100k
OSC INPUT
REQUIRED FOR TTL LOGIC
–(V
+
)
1046 F06
1
2
3
4
8
7
6
5
V
+
OSC
LV
V
OUT
BOOST
CAP
+
GND
CAP
LTC1046
C1
NC
+
+
Figure 5. Oscillator
OSC
(7)
1046 F05
LV
(6)
BOOST
(1)
14pF
I2I
I2I
V
+
SCHMITT
TRIGGER

LTC1046CN8#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Switched Cap Volt Conv 50mA
Lifecycle:
New from this manufacturer.
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