LTC3216EDE#PBF

LTC3216
7
3216fc
OPERATION
connected between the I
SET2
or I
SET1
pin and GND. The
resistor values needed to attain the desired current levels
can be determined by equation 1.
R
SET1/2
= 3965/I
LED
(1)
A resistor value of 2k or less (i.e. a short-circuit) will
cause the LTC3216 to enter overcurrent shutdown mode.
This mode will prevent damage to the part by shutting
down the high power sections of the chip.
Regulation is achieved by sensing the voltage at the CPO
pin and modulating the charge pump strength based
on the error signal. The CPO regulation voltages are set
internally, and are dependent on the charge pump mode
as shown in Table 1.
Table 1. Charge Pump Output Regulation Voltages
CHARGE PUMP MODE V
CPO
1.5x 4.6V
2x 5.1V
In shutdown mode all circuitry is turned off and the
LTC3216 draws a very low current from the V
IN
supply.
Furthermore, CPO is weakly connected to V
IN
. The LTC3216
enters shutdown mode when both the EN1 and EN2 pins
are brought low. Since EN1 and EN2 are high impedance
CMOS inputs they should never be allowed to fl oat. To
ensure that their states are defi ned they must always be
driven with valid logic levels.
Thermal Protection
The LTC3216 has built-in overtemperature protection. Ther-
mal shutdown circuitry will shutdown the I
LED
output when
the junction temperature exceeds approximately 150°C. It
will re-enable the I
LED
output once the junction temperature
drops back to approximately 135°C. The LTC3216 will cycle
in and out of thermal shutdown indefi nitely without latch
up or damage until the heat source is removed.
Soft-Start
To prevent excessive inrush current during start-up and
mode switching, the LTC3216 employs built-in soft-start
circuitry. Soft-start is achieved by increasing the amount
of current available to the output charge storage capacitor
linearly over a period of approximately 250µs.
Charge Pump Strength
When the LTC3216 operates in either the 1.5x mode or
2x mode, the charge pump can be modeled as a Theve-
nin-equivalent circuit to determine the amount of current
available from the effective input voltage and effective
open-loop output resistance, R
OL
(Figure 1).
Figure 1. Charge Pump Open-Loop Thevenin-Equivalent Circuit
+
+
CPO
R
OL
1.5V
IN
OR
2V
IN
R
OL
is dependent on a number of factors including the
oscillator frequency, fl ying capacitor values and switch
resistances.
From Figure 1, we can see that the output current is
proportional to:
(1.5V
IN
– CPO)/R
OL
or (2V
IN
– CPO)/R
OL
(2)
in the 1.5x mode or 2x mode respectively.
Current Levels
The LTC3216 may be programmed to have three discrete
current levels. These are the LOW, HIGH and LOW +
HIGH current levels. The LOW and HIGH currents are set
by the resistors connected between I
SET1
and I
SET2
pins,
respectively, to GND. The LOW + HIGH current mode
supplies a current that is equal to sum of the LOW and
HIGH currents.
Due to the low output impedance of this part, care should
be taken in selecting current levels. This part can supply up
to 500mA continuously, and up to 1A for pulsed operation
with a 10% duty cycle. Pulsed operation may be achieved
by toggling the EN1 and EN2 bits. In either continuous
or pulsed operation, proper board layout is required for
effective heat sinking.
Mode Switching
The LTC3216 will automatically switch from 1x mode to
1.5x mode, and subsequently from 1.5x mode to 2x mode
LTC3216
8
3216fc
V
IN
, CPO Capacitor Selection
The style and value of capacitors used with the LTC3216
determine several important parameters such as regulator
control loop stability, output ripple, charge pump strength
and minimum start-up time.
To reduce noise and ripple, it is recommended that low
equivalent series resistance (ESR) ceramic capacitors be
used for both C
VIN
and C
CPO
. Tantalum and aluminum
capacitors are not recommended because of their high
ESR.
The value of C
CPO
directly controls the amount of output
ripple for a given load current. Increasing the size of
C
CPO
will reduce the output ripple at the expense of higher
start-up current. The peak-to-peak output ripple for 1.5x
mode is approximately given by the expression:
V
RIPPLE(P-P)
= I
OUT
/(3f
OSC
• C
CPO
) (3)
Where f
OSC
is the LTC3216’s oscillator frequency (typically
900kHz) and C
CPO
is the output storage capacitor.
Both the style and value of the output capacitor can sig-
nifi cantly affect the stability of the LTC3216. As shown in
the Block Diagram, the LTC3216 uses a control loop to
adjust the strength of the charge pump to match the cur-
rent required at the output. The error signal of this loop
is stored directly on the output charge storage capacitor.
The charge storage capacitor also serves as the dominant
pole for the control loop. To prevent ringing or instability,
it is important for the output capacitor to maintain at least
2.2µF of actual capacitance over all conditions.
Likewise, excessive ESR on the output capacitor will tend
to degrade the loop stability of the LTC3216. The closed
loop output resistance of the LTC3216 is designed to be
76m. For a 100mA load current change, the error signal
will change by about 7.6mV. If the output capacitor has
76m or more of ESR, the closed-loop frequency response
will cease to roll off in a simple one pole fashion and poor
load transient response of instability could result. Multilayer
ceramic chip capacitors typically have exceptional ESR
performance. MLCCs combined with a tight board layout
will yield very good stability. As the value of C
CPO
controls
the amount of output ripple, the value of C
VIN
controls the
amount of ripple present at the input pin (V
IN
). The input
current to the LTC3216 will be relatively constant while
the charge pump is on either the input charging phase or
the output charging phase but will drop to zero during the
clock nonoverlap times. Since the nonoverlap time is small
(~15ns), these missing “notches” will result in only a small
perturbation on the input power supply line. Note that a
higher ESR capacitor such as tantalum will have higher
input noise due to the input current change times the ESR.
Therefore, ceramic capacitors are again recommended for
their exceptional ESR performance. Input noise can be
further reduced by powering the LTC3216 through a very
small series inductor as shown in Figure 2. A 10nH inductor
will reject the fast current notches, thereby presenting a
nearly constant current load to the input power supply.
For economy, the 10nH inductor can be fabricated on the
PC board with about 1cm (0.4") of PC board trace.
OPERATION
whenever a dropout condition is detected at the I
LED
pin.
In the LOW current mode, the part will wait approximately
150ms after dropout is detected before switching to the
next mode. In the HIGH and LOW + HIGH current modes,
the part will wait approximately 2ms before switching to
the next mode. These delays allow the LED to warm up
and reduce its forward voltage which may remove the
dropout condition.
In order to reset the part back into 1x mode, the LTC3216
must be brought into shutdown (EN1 = EN2 = LOW). Im-
mediately after the part has been brought to shutdown,
it may be set to the desired output current level via the
EN1 and EN2 pins. An internal comparator will not allow
the main switches to connect V
IN
and CPO in 1x mode
until the voltage at the CPO pin has decayed to less than
or equal to the voltage at the V
IN
pin.
APPLICATIONS INFORMATION
LTC3216
9
3216fc
APPLICATIONS INFORMATION
Flying Capacitor Selection
Warning: Polarized capacitors such as tantalum or alumi-
num should never be used for the fl ying capacitors since
their voltage can reverse upon start-up of the LTC3216.
Ceramic capacitors should always be used for the fl ying
capacitors.
The fl ying capacitors control the strength of the charge
pump. In order to achieve the rated output current it is
necessary to have at least 2.2µF of actual capacitance
for each of the fl ying capacitors. Capacitors of different
materials lose their capacitance with higher temperature
and voltage at different rates. For example, a ceramic
capacitor made of X7R material will retain most of its
capacitance from –40
o
C to 85
o
C whereas a Z5U or Y5V
style capacitor
will lose considerable capacitance over that range. Z5U and
Y5V capacitors may also have a very poor voltage coeffi cient
causing them to lose 60% or more of their capacitance when
the rated voltage is applied. Therefore, when comparing
different capacitors, it is often more appropriate to compare
the amount of achievable capacitance for a given case size
rather than comparing the specifi ed capacitance value. For
example, over rated voltage and temperature conditions,
a 1µF, 10V, Y5V ceramic capacitor in a 0603 case may not
provide any more capacitance than a 0.22µF, 10V, X7R
available in the same case. The capacitor manufacturers
data sheet should be consulted to determine what value
of capacitor is needed to ensure minimum capacitances
at all temperatures and voltages.
Table 2 shows a list of ceramic capacitor manufacturers
and how to contact them.
Table 2. Recommended Capacitor Vendors
AVX www.avxcorp.com
Kemet www.kemet.com
Murata www.murata.com
Taiyo Yuden www.t-yuden.com
Vishay www.vishay.com
TDK www.tdk.com
Layout Considerations and Noise
Due to its high switching frequency and the transient
currents produced by the LTC3216, careful board layout
is necessary. A true ground plane and short connections
to all capacitors will improve performance and ensure
proper regulation under all conditions.
The fl ying capacitor pins C1
+
, C2
+
, C1
and C2
will have
very high edge rate waveforms. The large dv/dt on these
pins can couple energy capacitively to adjacent PCB runs.
Magnetic fi elds can also be generated if the fl ying capacitors
are not close to the LTC3216 (i.e., the loop area is large).
To decouple capacitive energy transfer, a Faraday shield
may be used. This is a grounded PCB trace between the
sensitive node and the LTC3216 pins. For a high quality
AC ground, it should be returned to a solid ground plane
that extends all the way to the LTC3216.
Power Effi ciency
To calculate the power effi ciency (η) of a white LED
driver chip, the LED power should be compared to the
input power. The difference between these two numbers
represents lost power whether it is in the charge pump
or the current sources. Stated mathematically, the power
effi ciency is given by:
(4)

P
LED
P
IN
The effi ciency of the LTC3216 depends upon the mode in
which it is operating. Recall that the LTC3216 operates
as a pass switch, connecting V
IN
to CPO, until dropout
is detected at the I
LED
pin. This feature provides the op-
timum effi ciency available for a given input voltage and
Figure 2. 10nH Inductor Used for Input Noise
Reduction (Approximately 1cm of Wire)
V
IN
GND
LTC3216
2.2µF0.1µF
10nH
3216 F02

LTC3216EDE#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
LED Lighting Drivers 1A L N Hi C LED Ch Pump w/ Independent T
Lifecycle:
New from this manufacturer.
Delivery:
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