LTC1983ES6-5#TRMPBF

LTC1983-3/LTC1983-5
7
1983fc
For more information www.linear.com/LTC1983-3
operaTion
The LTC1983-3/LTC1983-5 use a switched capacitor
charge pump to invert a positive input voltage to a regulated
3V ±4% (LTC1983-3) or –5 ±4% (LTC1983-5) output
voltage. Regulation is achieved by sensing the output
voltage through an internal resistor divider and enabling
the charge pump when the output voltage droops above
the upper trip point of COMP1. When the charge pump
is enabled, a 2-phase, nonoverlapping clock controls the
charge pump switches. Clock 1 closes the S1 switches
which enables the flying capacitor to charge up to the
V
IN
voltage. Clock 2 closes the S2 switches that invert
the V
IN
voltage and connect the bottom plate of C
F LY
to
the output capacitor at V
OUT
. This sequence of charging
and discharging continues at a free-running frequency of
900kHz (typ) until the output voltage has been pumped
down to the lower trip point of COMP1 and the charge
pump is disabled. When the charge pump is disabled, the
LTC1983 draws only 25µA (typ) from V
IN
which provides
high efficiency at low load conditions.
In shutdown mode, all circuitry is turned off and the part
draws less thanA from the V
IN
supply. V
OUT
is also dis-
connected from V
IN
and C
F LY
. The SHDN pin has a threshold
of approximately 0.7V. The part enters shutdown when
a low is applied to the SHDN pin. The SHDN pin should
not be floated; it must be driven with a logic high or low.
Open-Loop Operation
The LTC1983-3/LTC1983-5 inverting charge pumps regu
-
late at –3V/–5V respectively, unless the input voltage is
too low or the output current is too high. The equations
for output voltage regulation are as follows:
V
IN
5.06V > I
OUT
R
OUT
(LTC1983-5)
V
IN
–3.06V > I
OUT
R
OUT
(LTC1983-3)
If this condition is not met, then the part will run in open
loop mode and act as a low output impedance inverter for
which the output voltage will be:
V
OUT
= –[V
IN
–(I
OUT
R
OUT
)]
For all R
OUT
values, check the corresponding curves in
the Typical Performance Characteristics section (Note:
C
F LY
= 1µF for all R
OUT
curves). The R
OUT
value will be
different for different flying caps, as shown in the follow-
ing equation:
R
OUT
= R
OUT
(curve) 1.11Ω +
1
f
OSC
C
FLY
Short-Circuit/Thermal Protection
During short-circuit conditions, the LTC1983 will draw
several hundred milliamps from V
IN
causing a rise in the
junction temperature. On-chip thermal shutdown circuitry
disables the charge pump once the junction temperature
exceeds 155°C, and re-enables the charge pump once the
junction temperature falls back to ≈145°C. The LTC1983
will cycle in and out of thermal shutdown indefinitely
without latchup or damage until the V
OUT
short is removed.
Capacitor Selection
For best performance, it is recommended that low ESR
capacitors be used for both C
IN
and C
OUT
to reduce noise
and ripple. The C
IN
and C
OUT
capacitors should be either
ceramic or tantalum and should be 4.7µF or greater.
Aluminum electrolytic are not recommended because of
their high equivalent series resistance (ESR). If the source
impedance is very low, C
IN
may not be needed. Increas-
ing the size of C
OUT
to 10µF or greater will reduce output
voltage ripple. The flying capacitor and C
OUT
should also
have low equivalent series inductance (ESL). The board
layout is critical as well for inductance for the same reason
(the suggested board layout should be used).
A ceramic capacitor
is recommended for the
flying ca-
pacitor with a value in the range of 0.1µF to 4.7µF. Note
that a large
value flying cap (>1µF) will increase output
ripple unless C
OUT
is also increased. For very low load
applications, C1 may be reduced to 0.01µF to 0.047µF.
This will reduce output ripple at the expense of efficiency
and maximum output current.
(Refer to Block Diagram)
LTC1983-3/LTC1983-5
8
1983fc
For more information www.linear.com/LTC1983-3
operaTion
(Refer to Block Diagram)
There are many aspects of the capacitors that must be
taken into account. First, the temperature stability of the
dielectric is a main concern. For ceramic capacitors, a
three character code specifies the temperature stability
(e.g. X7R, Y5V, etc.). The first two characters represent
the temperature range that the capacitor is specified
and the third represents the absolute tolerance that the
capacitor is specified to over that temperature range.
The ceramic capacitor used for the flying and output
capacitors should be X5R or better. Second, the volt
-
age coefficient of capacitance
for the capacitor must be
checked and the actual value usually needs to be derated
for the operating voltage (the actual value has to be larger
than the value needed to take into account the loss of
capacitance due to voltage bias across the capacitor).
Third, the frequency characteristics need to be taken into
account because capacitance goes down as the frequency
of oscillation goes up. Typically, the manufacturers have
capacitance vs frequency curves for their products. This
curve must be referenced to be sure the capacitance will
not be too small for the application. Finally, the capacitor
ESR
and ESL must be low for reasons mentioned in the
following section.
Output Ripple
Normal LTC1983 operation produces voltage ripple on the
V
OUT
pin. Output voltage ripple is required for the LTC1983
to regulate. Low frequency ripple exists due to the hyster-
esis in
the sense comparator and propagation delays in the
charg
e pump enable/disable circuits. High frequency ripple
is also present mainly due to ESR of the output capacitor.
Typical output ripple under maximum load is 60mV
P-P
with a low ESR 10µF output capacitor. The magnitude of
the ripple voltage depends on several factors. High input
voltage to negative output voltage differentials [(V
IN
+
V
OUT
) >1V] increase the output ripple since more charge
is delivered to C
OUT
per clock cycle. A large flying capacitor
(>1µF) also increases ripple for the same reason. Large
output current load and/or a small output capacitor (<10µF)
results in
higher ripple due to higher output voltage dV/dt.
High ESR capacitors
(ESR > 0.1Ω) on the output pin cause
high frequency voltage
spikes
on V
OUT
with every clock
cycle.
There are several ways to reduce the output voltage ripple.
A larger C
OUT
capacitor (22µF or greater) will reduce both
the low and high frequency ripple due to the lower C
OUT
charging and discharging dV/dt and the lower ESR typically
found with higher value (larger case size) capacitors. A
low ESR ceramic output capacitor will minimize the high
frequency ripple, but will not reduce the low frequency ripple
unless a high capacitance value is chosen. A reasonable
compromise is to use a 10µF to 22µF tantalum capacitor in
parallel with aF to 4.7µF ceramic capacitor on V
OUT
to
reduce both the low and high frequency ripple. However,
the best solution is to use 10µF to 22µF, X5R ceramic
capacitors which are available in 1206 package sizes. An
RC filter may also be used to reduce high frequency volt
-
age spikes (see Figure 1).
In
low load
or high V
IN
applications, smaller values for
C
F LY
may be used to reduce output ripple. A smaller fly-
ing capacitor (0.01µF
to 0.047µF) delivers less charge
per clock cycle to the output capacitor resulting in lower
output ripple. However, the smaller value flying caps also
reduce the maximum I
OUT
capability as well as efficiency.
V
OUT
V
OUT
LTC1983-X
10µF
TANTALUM
10µF
TANTALUM
V
OUT
V
OUT
LTC1983-X
15µF
TANTALUM
F
CERAMIC
3.9Ω
1983 F01
Figure 1. Output Ripple Reduction Techniques
LTC1983-3/LTC1983-5
9
1983fc
For more information www.linear.com/LTC1983-3
operaTion
Inrush Currents
During normal operation, V
IN
will experience current
transients in the several hundred milliamp range whenever
the charge pump is enabled. During start-up, these inrush
currents may approach 1 to 2 amps. For this reason, it is
important to minimize the source resistance between the
input supply and the V
IN
pin. Too much source resistance
may result in regulation problems or even prevent start-
up. One way that this can be avoided (especially when
the source impedance can’t be lowered due to system
constraints) is to use a large V
IN
capacitor with low ESR
right at the V
IN
pin. If ceramic capacitors are used, you may
need to addF to 10µF tantalum capacitor in parallel to
limit input voltage transients. Input voltage transients will
occur if V
IN
is applied via a switch or a plug. One example
of this situation is in USB applications.
Ultralow Quiescent Current Regulated Supply
The LTC1983 contains an internal resistor divider (refer
to the Block Diagram) that draws onlyA (typ for the
3V version) from V
OUT
during normal operation. During
shutdown, the resistor divider is disconnected from the
output and the part draws only leakage current from the
output. During no-load
conditions, applying a 1Hz to
100Hz, 2% to 5% duty cycle signal to the SHDN pin en
-
sures that the circuit of Figure 2 comes out of shutdown
frequently enough to maintain regulation even under low-
load conditions. Since the part spends nearly all of its time
in shutdown, the no-load quiescent current is essentially
zero. However, the part will still be in operation during
the time the SHDN pin is high, so the current will not be
zero and can be calculated using the following equations
to determine the approximate maximum current: I
IN(MAX)
= [(Time out of shutdown) (Burst Mode operation qui-
escent current
) + (Normal operating
I
IN
) (Time output
is being charged before the LTC1983 enters Burst Mode
operation)]/(Period of SHDN signal). This number will be
highly dependent on the amount of board leakage current
and how many devices are connected to V
OUT
(each will
draw some leakage current) and must be calculated and
verified for each different board design.
The LTC1983 must be out of shutdown for a minimum
duration of 200µs to allow enough time to sense the out
-
put and keep it in regulation. A 1Hz, 2% duty cycle signal
will keep V
OUT
in regulation under no-load conditions.
Even though the term no-load is used, there will always
be board leakage current and leakage current drawn by
anything connected to V
OUT
. This is why it is necessary
to wake the part up every once in a while to verify regula-
tion. As
the V
OUT
load current increases, the frequency
with which the part is taken out of shutdown must also
be increased to prevent V
OUT
from drooping below the
2.88V (for the 3V version) during the OFF phase (see
Figure 3). A 100Hz, 2% duty cycle signal on the SHDN pin
ensures proper regulation with load currents as high as
100µA. When load current greater than 100µA is needed,
the SHDN pin must be forced high as in normal operation.
Each time the LTC1983 comes out of shutdown, the part
delivers a minimum of one clock cycle worth of charge to
the output. Under high V
IN
(>4V) and/or low I
OUT
(<10µA)
conditions, this behavior may cause a net excess of charge
to be delivered to the output capacitor if a high frequency
signal is used on the SHDN pin (e.g., 50Hz
to 100Hz). Under
such conditions, V
OUT
will slowly drift positive and may
even go out of regulation. To avoid this potential problem
V
IN
GND
C
+
SHDN
V
OUT
C
LTC1983-3
C
FLY
1µF
CERAMIC
FROM MPU
SHDN
V
IN
C
IN
10µF
TANTALUM
C
OUT
10µF
CERAMIC
SHDN PIN WAVEFORMS:
LOW I
Q
MODE
(I
OUT
≤ 100µA)
V
OUT
LOAD ENABLE MODE
(I
OUT
= 100µA TO 100mA)
(1Hz TO 100Hz, 2% TO 5% DUTY CYCLE)
–3V ± 4%
1983 F02
3.3V TO 5.5V
Figure 2. Ultralow Quiescent Current Regulated Supply
(Refer to Block Diagram)

LTC1983ES6-5#TRMPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 100mA Inverting Charge Pump in ThinSOT
Lifecycle:
New from this manufacturer.
Delivery:
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