LTC4125
13
4125f
For more information www.linear.com/LTC4125
Input current limit is detected via the IMON pin. If the
voltage on the IMON pin exceeds 1.20V (V
ILIM
, typ) after
a valid exit condition is found, transmit power is reduced
to zero until the next search interval. Input current limit
is programmable using R
IN
, R
IMON
and R
IS
:
I
LIM
=
IN
R
IMON
ILIM
R
IS
=
IN
R
IMON
R
IS
Referring to the Block Diagram, V
IMON
is a gained up ver-
sion of the differential voltage across R
IS
. When V
IMON
is greater than 1.20V (V
ILIM
, typ), the input current limit
is reached. Notice that for the same values of R
IN
, R
IMON
and R
IS
, this input current limit is 150% (typ) of the input
current thresholdone of the programmable valid exit
conditions.
The final fault condition used in the algorithm is the die
temperature of the LTC4125. If the internal die temperature
of the LTC4125 ever exceeds 150°C (typ), then transmit
power is immediately reduced to zero until the next search
interval. Unlike other fault conditions, the die temperature
fault is not limited to the duration of the Optimum Power
Search period.
I
TH
vs I
LIM
As noted in the previous two sections, there are two input
current parameters whose values are determined by R
IN
,
R
IMON
and R
IS
: I
TH
(input current threshold) and I
LIM
(input
current limit). When the input current exceeds I
TH
during
the optimum power search, the search will stop and the
LTC4125 maintains operation at or slightly above this
input current level. However, if the input current exceeds
I
LIM
at any point during operation, power transmission will
cease immediately until the next search interval. The input
current limit is 150% (typ) of the input current threshold.
V
PTH1
/V
PTH2
and Pulse Width
The pulse width of each half of the full bridge driver
can be monitored using the PTH1 and PTH2 pins. When
AutoResonant drive is enabled, the pulse width is:
PW
SWx
(s) =
0.24
f
n
V
PTHx
+150ns
where f
n
is the full bridge resonant frequency, and 0.24 is
the typical normalized PTH voltage to Pulse Width Gain.
During the Optimum Power Search period, as the pulse
width increases, the voltage on the PTH pins increases as
well. When V
PTH1
or V
PTH2
exceeds 2.4V, the maximum
pulse width is guaranteed to have been reached, and the
end of search ramp fault condition stops power delivery
until the next search interval. Again, this typically indicates
that no receiver is present or that a conductive foreign
object is present.
PTHM
The pulse width of the first step in the Optimum Power
Search can be programmed using the PTHM pin. This fea
-
ture helps the Optimum Power Search find the appropriate
pulse width when the minimum transmit power levels of
the full bridge are known. This requires characterization
of the application to know that the optimum operating
point is always above a certain pulse width for all condi
-
tions. When PTHM is connected to ground, the first step
defaults to
150ns.
operaTion
LTC4125
14
4125f
For more information www.linear.com/LTC4125
TRANSMIT COIL SELECTION
There are several important parameters to consider when
making the transmit coil/inductor selection: the inductor
physical dimension, the inductance value, the inductor
quality factor (Q
L
), and the inductor saturation current.
All of these affect overall efficiency and power delivery
capability.
The physical dimension of the coil is important as it af
-
fects the overall coupling between the transmit and receive
coils.
The ideal size and shape of the transmit coil varies
depending on the application requirements. To name a
few: the end product size, shape and power requirement,
the freedom of placement desired in the final solution and
cost. As a guideline, many of the readily available wireless
power transmit coils are circular spiral coils with 50mm
diameter (Table 1). These coils are recommended as a
starting point when evaluating a design with LTC4125.
applicaTions inForMaTion
C
TX
100nF
33nF
DTH
FTH
PTHM
IS
IS
+
PTH1
PTH2
EN
NTC
SW1
SW2
FB
LTC4120-4.2
7.87k 59.0k
100k 100k
2.21k
470pF
10nF
10nF
F
47µF
x 2
11.3k
20mΩ
4.7nF
0.1µF
C
FB1
0.1µF
DC1
D
FB
D
STAT
100k
100V
348k
5.23k
24.9k
47µF
L
TX
24µH
L
RX
47µH
DR2
DR1
V
IN
V
IN
4.5V
TO
5.5V
10k
10k
+
SINGLE
CELL
Li-Ion
BATTERY
PACK
10µF
10nF
2.2µF
DFLZ39
QR1
R
NTCRX
R
NTCTX
L1
15µH
3.01k
I
IN
D
C
R
C
1k
M1
4125 07
LTC4125
FAULT
CHRG
BOOST
SW
CHGSNS
BAT
BATSNS
NTC
PROG GND FREQ INTV
CC
IMON CTD CTS GND
STATIN IN1 IN2
RUN IN DHC
L
TX
: 760308100110
C
TX
: C3216C0G2A104J160AC
C
FB1
: GRM188R72A104KA35D
DC1: CDBQR70
D
STAT
: LTST-C193KGKT-5A
D
FB
: BAS521-7
R
NTCTX
: NTHS0603N02N1002J
RED INDICATES HIGH VOLTAGE PARTS
DR1, DR2, DR3: DFLS240L
D
C
: BZT52C13
M1: Si7308DN
QR1: PMBT3904M
R
NTCRX
: NTHS0402N02N1002F
L
RX
: PCB COIL AND FERRITE: B67410-A0223-X195
OR 760308101303
L1: LPS4018-153ML
AIR GAP
3mm
TO
10mm
Figure7. LTC4125 Driving a 24μH Transmit Coil at 103kHz, with 1.3A Input Current Threshold, 119kHz Frequency
Limit and 41.5°C Transmit Coil Surface Temperature Limit in a Wireless Power System with LTC4120-4.2 as a
400mA Single Cell Li-Ion Battery Charger at the Receiver
In a typical design with LTC4125 (see Block Diagram
for component labels), the following steps are usually
followed: select a transmit coil (L
TX
), select a resonant
capacitor (C
TX
), determine the feedback voltage divider
(R
FB1
, R
FB2
), determine the input current monitor resistors
(R
IS
, R
IN
, R
IMON
), determine the frequency threshold resis-
tors (R
FTH1
, R
FTH2
), determine the Optimum Power Search
Settling Time (C
TS
), determine the Optimum Power Search
Delay Time (C
TD
), determine the pulse width of the first
step in the Optimum Power Search (R
PTHM1
, R
PTHM2
), and
finally, determine the differential FB pin voltage threshold
(R
DTH1
, R
DTH2
).
The following discussion elaborates on factors that need
to be considered for each of these steps. For further clar
-
ity, an example for each step is discussed in the context
of the application circuit shown in Figure7.
LTC4125
15
4125f
For more information www.linear.com/LTC4125
(I
RMS-MAX
) before thermal rise (from 25°C ambient) in the
die causes the internal thermal shutdown to stop power
delivery in the coil.
In the specific application shown in Figure7, a 24μH coil
(760308100110) from Würth is used. It has a 50mm di
-
ameter, a Q value of 140 at 100kHz as well as a saturation
current greater than
10A.
T
RANSMITTER RESONANT CAPACITOR SELECTION
The factors to consider when selecting the transmitter
capacitor are similar to the factors discussed previously
when making the inductor choice: the capacitance value,
the capacitor quality factor (Q
C
), and the voltage rating
of the capacitor. The physical dimension of the capacitor
is usually not a big factor since overall application size is
driven mainly by the size of the transmit coil.
First and foremost the parameter to consider is the ca
-
pacitance value itself.
T
he LTC4125 is designed to work
with resonant frequencies between 50kHz and 250kHz.
The AutoResonant feature of the LTC4125 ensures that
the series LC network is driven at the resonant frequency
of the LC network:
f
o
=
1
2π LC
Another important factor is the parasitic dissipative com-
ponent of the capacitance. As with the inductor, one way
to measure this component is by looking at the quality
factor of
the capacitor. The capacitor quality factor is
described as:
Q
C
=
1
ωCR
C
=
1
2πfCR
C
where ω is the target frequency in radians, f is the target
frequency in Hz, and R
C
is the capacitor effective series
resistance. The higher the Q, the more ideal that particular
capacitor is at that frequency.
For a given value of inductance, frequency and current
amplitude, the voltage that is developed across the inductor
and the capacitor is well defined. The capacitor voltage
Table 1. Recommended Transmit Coils
MANUFACTURER PART NUMBER
INDUCTANCE
(µH)
SIZE
(mm)
QUALITY
FACTOR AT
100kHz
Würth 760308110 24 53 x 53 140
Würth 760308100110 24
Dia. 50
140
Würth 760308100111 6.3
Dia. 50
100
Inter Technical L41200T06 5 52 x 52 80
TDK WT505090-
20K2-A10-G
24
Dia. 50
50
TDK WT505090-
10K2-A11-G
6.3
Dia. 50
100
Another important parameter to consider is the inductance
value of the coil itself. This value needs to be considered in
relation to the receive coil inductance value and the overall
wireless power system coupling between the transmit and
the receive coil. The ratio of the two inductance values
together with the coupling factor determines the voltage
and current possible on the receive coil, and therefore the
power delivery capability of the system.
The quality factor of an inductor at a particular frequency
is defined as follows:
Q
L
=
ω
L
R
L
=
2
π
fL
R
L
where ω is the target frequency in radians, f is the target
frequency in Hz, and R
L
is the inductor effective series
resistance. The higher the Q, the more efficient that par-
ticular inductor is in carrying current at that frequency.
A
typical 24µH
transmit coil that is used to deliver power
up to 5W across a 1mm to 15mm distance has a quality
factor of ≈50 to 150 at 100kHz operating frequency.
Many commercially available transmit coils use ferrite
material to help boost the inductance value as well as
shape the magnetic field created by the transmit coil to
increase coupling and power delivery. However, ferrite
material limits the saturation current level. The satura
-
tion current level needs to be higher than the maximum
current amplitude generated in the LC resonant structure
to ensure predictable inductance values and prevent po
-
tential thermal runaways. The monolithic switches inside
the LTC4125 allow switches RMS current of up to 3.5A
applicaTions inForMaTion

LTC4125EUFD#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Wireless Charging ICs 5W AutoResonant Wireless Pwr Transmitter
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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