LTC3852
22
3852f
APPLICATIONS INFORMATION
Phase-Locked Loop and Frequency Synchronization
The LTC3852 has a phase-locked loop (PLL) comprised of
an internal voltage-controlled oscillator (V
CO
) and a phase
detector. This allows the turn-on of the top MOSFET to
be locked to the rising edge of an external clock signal
applied to the MODE/PLLIN pin. This phase detector is
an edge sensitive digital type that provides zero degrees
phase shift between the external and internal oscillators.
This type of phase detector does not exhibit false lock to
harmonics of the external clock.
The output of the phase detector is a pair of complemen tary
current sources that charge or discharge the external fi lter
network connected to the FREQ/PLLFLTR pin. Note that
the LTC3852 can only be synchronized to an external clock
whose frequency is within range of the LTC3852’s internal
V
CO
.This is guaranteed to be between 250kHz and 750kHz.
A simplifi ed block diagram is shown in Figure 9.
DIGITAL
PHASE/
FREQUENCY
DETECTOR
VCO
2.7V
R
LP
C
LP
3852 F09
FREQ/PLLFLTR
EXTERNAL
OSCILLATOR
MODE/
PLLIN
If the external clock frequency is greater than the internal
oscillators frequency, f
OSC
, then current is sunk con-
tinuously from the phase detector output, pulling down
the FREQ/PLLFLTR pin. When the external clock frequency
is less than f
OSC
, current is sourced continuously, pulling
up the FREQ/PLLFLTR pin. If the external and internal
frequencies are the same but exhibit a phase difference, the
current sources turn on for an amount of time corresponding
to the phase difference. The voltage on the FREQ/PLLFLTR
pin is adjusted until the phase and frequency of the internal
and external oscillators are identical. At the stable operating
point, the phase detector output is high impedance and the
lter capacitor C
LP
holds the voltage.
Figure 9. Phase-Locked Loop Block Diagram
The loop fi lter components, C
LP
and R
LP
, smooth out
the current pulses from the phase detector and provide
a stable input to the voltage-controlled oscillator. The
lter components C
LP
and R
LP
determine how fast the
loop acquires lock. Typically R
LP
is 1k to 10k and C
LP
is
2200pF to 0.01F.
When the external oscillator is active before the LTC3852
is enabled, the internal oscillator frequency will track the
external oscillator frequency as described in the preceding
paragraphs. In situations where the LTC3852 is enabled
before the external oscillator is active, a low free-running
oscillator frequency of approximately 50kHz will result. It is
possible to increase the free-running, pre-synchronization
frequency by adding a second resistor in parallel with
R
LP
and C
LP
. The second resistor will also cause a phase
difference between the internal and external oscillator
signals. The magnitude of the phase difference is inversely
proportional to the value of the second resistor.
The external clock (on MODE/PLLIN pin) input high
threshold is nominally 1.6V, while the input low thres hold
is nominally 1.2V.
Maximum Available Charge Pump Current
For the charge pump, the maximum available output
current and voltage can be calculated from the effective
open-loop output resistance, R
OL
, and the effective input
voltage, 2V
IN1(MIN)
.
+
R
OL
I
OUT
V
PUMP
2V
IN1
3852 F10
+
From Figure 10, the available current is given by:
I
PUMP
=
2V
IN1
–V
PUMP
R
OL
The actual current (into V
IN2
and INTV
CC
) should not
exceed 50mA.
Figure 10. Equivalent Open-Loop Circuit
LTC3852
23
3852f
Effective Open Loop Output Resistance (R
OL
)
The effective open loop output resistance (R
OL
) of a charge
pump is a very important parameter which determines the
strength of the charge pump. The value of this parameter
depends on many factors such as the oscillator frequency
(f
OSC
), value of the fl ying capacitor (C
FLY
), the nonoverlap
time, the internal switch resistances (R
S
), and the ESR of
the external capacitors. A fi rst order approximation for
R
OL
is given below:
R
OL
2R
S
+
1
f
OSC
•C
FLY
Typical R
OL
values as a function of temperature are shown
in Figure 11.
APPLICATIONS INFORMATION
S=1 TO 4
Charge Pump Capacitor Selection
The style and value of capacitors used with the charge
pump 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
ESR (<0.1W) ceramic capacitors be used for both C
IN
and C
PUMP
. These capacitors should be 2.2µF or greater.
Tantalum and aluminum capacitors are not recommended
because of their high ESR.
The value of C
PUMP
directly controls the amount of
output ripple for a given load current. Increasing the size
of C
PUMP
will reduce the output ripple at the expense of
3852 F11
TEMPERATURE (oC)
100
050
EFFECTIVE OPEN-LOOP OUTPUT RESISTANCE (7)
V
IN
= 2.7V
V
PUMP
= 4.5V
–50
8
7
6
5
4
Figure 11. Typical R
OL
vs Temperature
higher minimum turn-on time. The peak-to-peak output
ripple of a charge pump is approximately given by the
expression:
V
RIPPLE(PP)
I
PUMP
2f
OSC
•C
PUMP
where f
OSC
is the charge pump frequency (typically 1.2MHz)
and C
PUMP
is the value of the V
PUMP
storage capacitor.
Also, the value and style of the C
PUMP
capacitor can
signifi cantly affect the stability of the charge pump. As
shown in the Functional Diagram, the charge pump
uses a linear control loop to adjust the strength of the
charge pump to match the current required at the output.
The error signal of this loop is stored directly on the
output storage capacitor. This output capacitor also
serves to form the dominant pole of the control loop.
To prevent ringing or instability on the charge pump,
it is important to maintain at least 1µF of capacitance over
all conditions.
Excessive ESR on the C
PUMP
capacitor can degrade the
loop stability of the charge pump. Its closed loop output
resistance is designed to be 0.5W. For a 50mA load current
change, the output voltage will change by about 25mV. If
the output capacitor has 0.5W 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 or
instability could result. Ceramic capacitors typically have
exceptional ESR performance and combined with a good
board layout should yield very good stability and load
transient performance.
As the value of C
PUMP
controls the amount of output ripple,
the value of C
IN
controls the amount of ripple present at
the input pin (V
IN1
). The input current to the charge pump
will be relatively constant during the input charging phase
or the output charging phase but will drop to zero during
the nonoverlap times. Since the nonoverlap time is small
(~25ns), 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 voltage drop in the ESR. Therefore,
ceramic capacitors are again recommended for their
exceptional ESR performance.
LTC3852
24
3852f
Further input noise reduction can be achieved by powering
V
IN1
through a very small series inductor as shown in
Figure 12. 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.
APPLICATIONS INFORMATION
LTC3852
0.22µF
2.2µF
V
IN1
GND1
1cm OF PCB TRACE
10nH
V
IN
11
12
3852 F12
Flying Capacitor Selection
Warning: A polarized capacitor such as tantalum or
aluminum should never be used for the fl ying capacitor
since its voltage can reverse upon start-up of the
charge pump. Low ESR ceramic capacitors should always
be used for the fl ying capacitor.
The fl ying capacitor controls the strength of the charge
pump. In order to achieve the rated output current, it is
necessary to have at least 1µF of capacitance for the fl y ing
capacitor.
Ceramic Capacitors
Ceramic capacitors of different materials lose their capac-
itance with higher temperature and voltage at different rates.
For example, a capacitor made of X5R or X7R material
will retain most of its capacitance from –40°C to 85°C
whereas a Z5U or Y5V style capacitor will lose considerable
capacitance over that range. Z5U and Y5V capacitors
may also have a 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 discussing 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
Figure 12. 10nH Inductor Used for
Additional Input Noise Reduction
provide any more capacitance than a 0.22µF 10V X7R
capacitor available in the same 0603 case. In fact, for the
charge pump, these capacitors can be considered roughly
equivalent. The capacitor manufacturers data sheet should
be consulted to ensure the desired capacitance at all temp-
eratures and voltages.
Table 1 shows a list of ceramic capacitor manufacturers
and how to contact them:
Table 1.
AVX www.avx.com
Kemet www.kemet.com
Murata www.murata.com
Taiyo Yuden www.t-yuden.com
TDK www.component.tdk.com
Vishay www.vishay.com
Effi ciency Considerations
The percent effi ciency of a switching regulator is equal to
the output power divided by the input power times 100. It
is often useful to analyze the individual loss components
to determine what limits the effi ciency and which change
would produce the biggest improvement. The effi ciency
can be expressed as:
% Effi ciency = 100% – (L1 + L2 + L3 + ...)
where L1, L2, etc. are the individual losses as a percentage
of input power.
Although all dissipative elements in the circuit produce
losses, there are fi ve main sources of power loss in
LTC3851 circuits: 1) I
2
R losses, 2) transition losses in the
top MOSFET, 3) gate charge losses within the controller
due to the input capacitance of the power MOSFETs,
4) the DC bias current of the controller (V
IN2
), and 5) the
effi ciency of the charge pump.
1. I
2
R losses are predicted from the DC resistances of the
fuse (if used), top and bottom MOSFET on-resistances,
the inductor DCR and the current sense resistor (if used).
In continuous conduction mode (CCM), the average
output current fl ows through the inductor (L) and sense
resistor (R
SENSE
), but is “chopped” between the top
and bottom MOSFETs. Since the two MOSFETs rarely
have the same R
ON
, an effective MOSFET resistance

LTC3852EUDD#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Low Input Voltage Synchronous Step-Down Controller
Lifecycle:
New from this manufacturer.
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