LTC3858-2
16
38582f
APPLICATIONS INFORMATION
Figure 3. Sense Lines Placement with Inductor or Sense Resistor
The Typical Application on the first page is a basic
LTC3858-2 application circuit. LTC3858-2 can be config-
ured to use either DCR (inductor resistance) sensing or low
value resistor sensing. The choice between the two current
sensing schemes is largely a design trade-off between
cost, power consumption and accuracy. DCR sensing
is becoming popular because it saves expensive current
sensing resistors and is more power efficient, especially
in high current applications. However, current sensing
resistors provide the most accurate current limits for the
controller. Other external component selection is driven
by the load requirement, and begins with the selection of
R
SENSE
(if R
SENSE
is used) and inductor value. Next, the
power MOSFETs and Schottky diodes are selected. Finally,
input and output capacitors are selected.
Current Limit Programming
The I
LIM
pin is a tri-level logic input which sets the maximum
current limit of the converter. When I
LIM
is grounded, the
maximum current limit threshold voltage of the current
comparator is programmed to be 30mV. When I
LIM
is
floated, the maximum current limit threshold is 50mV.
When I
LIM
is tied to INTV
CC
, the maximum current limit
threshold is set to 75mV.
SENSE
+
and SENSE
Pins
The SENSE
+
and SENSE
pins are the inputs to the current
comparators. The common mode voltage range on these
pins is 0V to 28V (Abs Max), enabling the LTC3858-2 to
regulate output voltages up to a nominal 24V (allowing
plenty of margin for tolerances and transients).
The SENSE
+
pin is high impedance over the full common
mode range, drawing at most ±1µA. This high impedance
allows the current comparators to be used in inductor
DCR sensing.
The impedance of the SENSE
pin changes depending on
the common mode voltage. When SENSE
is less than
INTV
CC
– 0.5V, a small current of less than 1µA flows out
of the pin. When SENSE
is above INTV
CC
+ 0.5V, a higher
current (~550µA) flows into the pin. Between INTV
CC
0.5V and INTV
CC
+ 0.5V, the current transitions from the
smaller current to the higher current.
Filter components mutual to the sense lines should be
placed close to the LTC3858-2, and the sense lines should
run close together to a Kelvin connection underneath the
current sense element (shown in Figure 3). Sensing cur-
rent elsewhere can effectively add parasitic inductance
and capacitance to the current sense element, degrading
the information at the sense terminals and making the
programmed current limit unpredictable. If inductor DCR
sensing is used (Figure 4b), resistor R1 should be placed
close to the switching node, to prevent noise from coupling
into sensitive small-signal nodes.
C
OUT
TO SENSE FILTER,
NEXT TO THE CONTROLLER
INDUCTOR OR R
SENSE
3858 F03
Low Value Resistor Current Sensing
A typical sensing circuit using a discrete resistor is shown
in Figure 4a. R
SENSE
is chosen based on the required
output current.
The current comparator has a maximum threshold
V
SENSE(MAX)
determined by the I
LIM
setting. The current
comparator threshold voltage sets the peak of the induc-
tor current, yielding a maximum average output current,
I
MAX
, equal to the peak value less half the peak-to-peak
ripple current, ΔI
L
. To calculate the sense resistor value,
use the equation:
R
SENSE
=
V
SENSE(MAX)
I
MAX
+
ΔI
L
2
When using the controller in very low dropout conditions,
the maximum output current level will be reduced due to
the internal compensation required to meet stability cri-
terion for buck regulators operating at greater than 50%
duty factor. A curve is provided in the Typical Performance
Characteristics section to estimate this reduction in peak
output current depending upon the operating duty factor.
LTC3858-2
17
38582f
(4a) Using a Resistor to Sense Current (4b) Using the Inductor DCR to Sense Current
Figure 4. Current Sensing Methods
APPLICATIONS INFORMATION
Inductor DCR Sensing
For applications requiring the highest possible efficiency
at high load currents, the LTC3850 is capable of sensing
the voltage drop across the inductor DCR, as shown in
Figure 4b. The DCR of the inductor represents the small
amount of DC resistance of the copper wire, which can be
less than 1m for todays low value, high current inductors.
In a high current application requiring such an inductor,
power loss through a sense resistor would cost several
points of efficiency compared to inductor DCR sensing.
If the external R1||R2 • C1 time constant is chosen to be
exactly equal to the L/DCR time constant, the voltage drop
across the external capacitor is equal to the drop across
the inductor DCR multiplied by R2/(R1 + R2). R2 scales the
voltage across the sense terminals for applications where
the DCR is greater than the target sense resistor value.
To properly dimension the external filter components, the
DCR of the inductor must be known. It can be measured
using a good RLC meter, but the DCR tolerance is not
always the same and varies with temperature; consult
the manufacturers’ data sheets for detailed information.
Using the inductor ripple current value from the Inductor
Value Calculation section, the target sense resistor value is:
R
SENSE(EQUIV)
=
V
SENSE(MAX)
I
MAX
+
ΔI
L
2
To ensure that the application will deliver full load current
over the full operating temperature range, choose the
minimum value for the Maximum Current Sense Thresh-
old Voltage (V
SENSE(MAX)
) in the Electrical Characteristics
table (30mV, 50mV or 75mV depending on the state of
the I
LIM
pin).
Next, determine the DCR of the inductor. When provided,
use the manufacturers maximum value, usually given at
20°C. Increase this value to account for the temperature
coefficient of copper, which is approximately 0.4%/°C. A
conservative value for T
L(MAX)
is 100°C.
To scale the maximum inductor DCR to the desired sense
resistor (R
D
) value, use the divider ratio:
R
D
=
R
SENSE(EQUIV)
DCR
MAX
atT
L(MAX)
V
IN
V
IN
INTV
CC
BOOST
TG
SW
BG
PLACE CAPACITOR NEAR
SENSE PINS
SENSE
+
SENSE
SGND
LTC3858-2
V
OUT
R
SENSE
38582 F04a
V
IN
V
IN
INTV
CC
BOOST
TG
SW
BG
*PLACE C1 NEAR
SENSE PINS
INDUCTOR
DCRL
SENSE
+
SENSE
SGND
LTC3858-2
V
OUT
38582 F04b
R1
R2C1*
(R1
||
R2) t C1 =
L
DCR
R
SENSE(EQ)
= DCR
R2
R1 + R2
LTC3858-2
18
38582f
APPLICATIONS INFORMATION
C1 is usually selected to be in the range of 0.1µF to 0.47µF.
This forces R1||R2 to around 2k, reducing error that might
have been caused by the SENSE
+
pin’s ±1µA current.
The equivalent resistance R1||R2 is scaled to the room
temperature inductance and maximum DCR:
R1|| R2 =
L
DCR at 20°C
()
•C1
The sense resistor values are:
R1=
R1|| R2
R
D
; R2 =
R1 R
D
1–R
D
The maximum power loss in R1 is related to duty cycle,
and will occur in continuous mode at the maximum input
voltage:
P
LOSS
R1=
V
IN(MAX)
–V
OUT
()
•V
OUT
R1
Ensure that R1 has a power rating higher than this value.
If high efficiency is necessary at light loads, consider
this power loss when deciding whether to use inductor
DCR sensing or sense resistors. Light load power loss
can be modestly higher with a DCR network than with a
sense resistor, due to the extra switching losses incurred
through R1. However, DCR sensing eliminates a sense
resistor, reduces conduction losses and provides higher
efficiency at heavy loads. Peak efficiency is about the same
with either method.
Inductor Value Calculation
The operating frequency and inductor selection are inter-
related in that higher operating frequencies allow the use
of smaller inductor and capacitor values. So why would
anyone ever choose to operate at lower frequencies with
larger components? The answer is efficiency. A higher
frequency generally results in lower efficiency because
of MOSFET gate charge losses. In addition to this basic
trade-off, the effect of inductor value on ripple current and
low current operation must also be considered.
The inductor value has a direct effect on ripple current. The
inductor ripple current ΔI
L
decreases with higher induc-
tance or higher frequency and increases with higher V
IN
:
ΔI
L
=
1
f
()
L
()
V
OUT
1–
V
OUT
V
IN
Accepting larger values of ΔI
L
allows the use of low
inductances, but results in higher output voltage ripple
and greater core losses. A reasonable starting point for
setting ripple current is ΔI
L
= 0.3(I
MAX
). The maximum
ΔI
L
occurs at the maximum input voltage.
The inductor value also has secondary effects. The tran-
sition to Burst Mode operation begins when the average
inductor current required results in a peak current below
30% of the current limit determined by R
SENSE
. Lower
inductor values (higher ΔI
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 decrease.
Inductor Core Selection
Once the value for L is known, the type of inductor must
be selected. High efficiency converters generally cannot
afford the core loss found in low cost powdered iron cores,
forcing the use of more expensive ferrite or molypermalloy
cores. Actual core loss is independent of core size for a
fixed inductor value, but it is very dependent on inductance
value selected. As inductance increases, core losses go
down. Unfortunately, increased inductance requires more
turns of wire and therefore copper losses will increase.
Ferrite designs have very low core loss and are preferred
for high switching frequencies, so design goals can con-
centrate on copper loss and preventing saturation. Ferrite
core material saturates “hard,” which means that induc-
tance collapses abruptly when the peak design current is
exceeded. This results in an abrupt increase in inductor
ripple current and consequent output voltage ripple. Do
not allow the core to saturate!

LTC3858IUH-2#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Low IQ, Dual, 2-Phase Synchronous Step-Down Controller without OVP
Lifecycle:
New from this manufacturer.
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