10
LTC1875
1875f
OPERATIO
U
Slope Compensation and Inductor Peak Current
Slope compensation is required in order to prevent sub-
harmonic oscillation at high duty cycles. It is accom-
plished by internally adding a compensating ramp to the
inductor current signal at duty cycles in excess of 40%. As
a result, the maximum inductor peak current is reduced for
duty cycles >40%. This is shown in the decrease of the
inductor peak current as a function of duty cycle graph in
Figure 3.
Figure 3. Maximum Inductor Peak Current vs Duty Cycle
APPLICATIO S I FOR ATIO
WUUU
The basic LTC1875 application circuit is shown on the first
page of this data sheet. External component selection is
driven by the load requirement and begins with the selec-
tion of L followed by C
IN
and C
OUT
.
Inductor Value Calculation
The inductor selection will depend on the operating fre-
quency of the LTC1875. The internal nominal frequency is
550kHz, but can be externally synchronized from 350kHz
to 750kHz.
The operating frequency and inductor selection are inter-
related in that higher operating frequencies allow the use
of smaller inductor and capacitor values. However, oper-
ating at a higher frequency results in lower efficiency
because of increased switching losses.
The inductor value has a direct effect on ripple current. The
ripple current I
L
decreases with higher inductance or
frequency and increases with higher input voltages.
∆=
()()
I
fL
V
V
V
L OUT
OUT
IN
1
1–
(1)
Accepting larger values of I
L
allows the use of smaller
inductors, but results in higher output voltage ripple.
A reasonable starting point for setting ripple current is
I
L
= 0.3(I
MAX
).
The inductor value also has an effect on Burst Mode
operation. The transition to low current operation begins
when the inductor current peaks fall to approximately
500mA. Lower inductor values (higher I
L
) will cause this
to occur at lower load currents, which can cause a dip in
efficiency in the upper range of low current operation. In
Burst Mode operation, lower inductance values will cause
the burst frequency to increase.
Inductor Selection
The inductor should have a saturation current rating
greater than the peak inductor current set by the current
comparator of LTC1875. Also, consideration should be
given to the resistance of the inductor. Inductor conduc-
tion losses are directly proportional to the DC resistance
of the inductor.
Manufacturers sometimes provide maxi-
mum current ratings based on the allowable losses in the
inductor.
Suitable inductors are available from Coilcraft, Coiltron-
ics, Dale, Sumida, Toko, Murata, Panasonic and other
manufacturers.
DUTY CYCLE (%)
0
MAXIMUM INDUCTOR PEAK CURRENT (mA)
2200
2000
1800
1600
1400
1200
1000
800
20 40 60 80
1875 F03
100
V
IN
= 3V
11
LTC1875
1875f
C
IN
and C
OUT
Selection
In continuous mode, the source current of the top MOSFET
is a trapezoidal waveform of duty cycle V
OUT
/V
IN
. To
prevent large voltage transients, a low ESR input capacitor
sized for the maximum RMS current must be used. The
maximum RMS input capacitor current is given by:
II
VVV
V
RMS CIN OMAX
OUT IN OUT
IN
()
/
(– )
[]
12
This formula has a maximum at V
IN
= 2V
OUT
, where
I
RMS
= I
OUT
/2. This simple worst-case condition is com-
monly used for design because even significant devia-
tions do not offer much relief. Note that the capacitor
manufacturer’s ripple current ratings are often based on
2000 hours of life. This makes it advisable to further
derate the capacitor, or choose a capacitor rated at a
higher temperature than required. Several capacitors may
also be paralleled to meet size or height requirements in
the design. Always consult the manufacturer if there are
any questions.
Depending on how the LTC1875 circuit is powered up,
you may need to check for input voltage transients. Input
voltage transients may be caused by input voltage steps
or by connecting the circuit to an already powered up
source such as a wall adapter. The sudden application of
input voltage will cause a large surge of current in the
input leads that will store energy in the parasitic induc-
tance of the leads. This energy will cause the input voltage
to swing above the DC level of the input power source and
it may exceed the maximum voltage rating of the input
capacitor and LTC1875.
The easiest way to suppress input voltage transients is to
add a small aluminum electrolytic capacitor in parallel
with the low ESR input capacitor. The selected capacitor
needs to have the right amount of ESR in order to critically
dampen the resonant circuit formed by the input lead
inductance and the input capacitor. The typical values of
ESR will fall in the range of 0.5 to 2 and capacitance
will fall in the range of 5µF to 50µF.
The selection of C
OUT
is driven by the required effective
series resistance (ESR). Typically, once the ESR require-
ment is satisfied, the capacitance is adequate for filtering.
The output ripple V
OUT
is determined by:
∆≅ +
V I ESR
fC
OUT L
OUT
1
8
where f = operating frequency, C
OUT
= output capacitance
and I
L
= ripple current in the inductor. The output ripple
is highest at maximum input voltage since I
L
increases
with input voltage. For the LTC1875, the general rule for
proper operation is:
ESR
COUT
< 0.125
The choice of using a smaller output capacitance in-
creases the output ripple voltage due to the frequency
dependent term but can be compensated for by using
capacitor(s) of very low ESR to maintain low ripple volt-
age. The I
TH
pin compensation components can be opti-
mized to provide stable high performance transient
response regardless of the output capacitor selected.
Manufacturers such as Taiyo Yuden, AVX, Kemet and
Sanyo should be considered for low ESR, high perfor-
mance capacitors. The POSCAP solid electrolytic chip
capacitor available from Sanyo is an excellent choice for
output bulk capacitors due to its low ESR/size ratio. Once
the ESR requirement for C
OUT
has been met, the RMS
current rating generally far exceeds the I
RIPPLE(P-P)
requirement.
Output Voltage Programming
The output voltage is set by a resistor divider according to
the following formula:
VV
R
R
OUT
=+
08 1
1
2
.
(2)
The external resistor divider is connected to the output,
allowing remote voltage sensing as shown in Figure 4.
APPLICATIO S I FOR ATIO
WUUU
12
LTC1875
1875f
APPLICATIO S I FOR ATIO
WUUU
filter network on the PLL_LPF pin. The relationship be-
tween the voltage on the PLL_LPF pin and operating
frequency is shown in Figure 5. A simplified block diagram
is shown in Figure 6.
If the external frequency (V
SYNC/MODE
) is greater than
550kHz, the center frequency, current is sourced continu-
ously, pulling up the PLL_LPF pin. When the external
frequency is less than 550kHz, current is sunk continu-
ously, pulling down the PLL_LPF 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. Thus the
voltage on the PLL_LPF pin is adjusted until the phase and
frequency of the external and internal oscillators are
identical. At this stable operating point the phase com-
parator output is open and the filter capacitor C
LP
holds the
voltage.
The loop filter 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 filter
components C
LP
and R
LP
determine how fast the loop
acquires lock. Typically R
LP
= 10k and C
LP
is 2200pF to
0.01µF. When not synchronized to an external clock, the
internal connection to the VCO is disconnected. This
disallows setting the internal oscillation frequency by a DC
voltage on the V
PLLLPF
pin.
Figure 5. Relationship Between Oscillator Frequency
and Voltage at PLL_LPF Pin
DIGITAL
PHASE/
FREQUENCY
DETECTOR
SYNC/
MODE
PLL_LPF
2.4V
C
LP
1875 F06
R
LP
VCO
Figure 6. Phase-Locked Loop Block Diagram
Phase-Locked Loop and Frequency Synchronization
The LTC1875 has an internal voltage-controlled oscillator
and phase detector comprising a phase-locked loop. This
allows the MOSFET turn-on to be locked to the rising edge
of an external frequency source. The frequency range of
the voltage-controlled oscillator is 350kHz to 750kHz. The
phase detector used is an edge sensitive digital type that
provides zero degrees phase shift between the external
and internal oscillators. This type of phase detector will not
lock up on input frequencies close to the harmonics of the
VCO center frequency. The PLL hold-in range f
H
is equal
to the capture range, f
H
= f
C
= ±200kHz.
The output of the phase detector is a pair of complemen-
tary current sources charging or discharging the external
V
FB
LTC1875
0.8V V
OUT
6V
SGND
R2
1875 F04
R1
Figure 4. Setting the LTC1875 Output Voltage
V
PLLLPF
(V)
0
OSC FREQUECNY (kHz)
1000
900
800
700
600
500
400
300
200
100
0
1875 F05
0.5 1 1.5 2

LTC1875EGN#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 15uA Quiescent Current, 1.5A Synch Step-dwn Reg
Lifecycle:
New from this manufacturer.
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