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LTC4090EDJC(RevA) View Datasheet(PDF) - Linear Technology

Part Name
Description
MFG CO.
LTC4090EDJC Datasheet PDF : 28 Pages
First Prev 21 22 23 24 25 26 27 28
LTC4090/LTC4090-5
APPLICATIONS INFORMATION
where rHOT and rCOLD are the resistance ratios at the de-
sired hot and cold trip points. Note that these equations
are linked. Therefore, only one of the two trip points can
be chosen, the other is determined by the default ratios
designed in the IC. Consider an example where a 40°C
hot trip point is desired.
From the Vishay Curve 2 R-T characteristics, rHOT is 0.5758
at 40°C. Using the above equation, RNOM should be set
to 14.0k. With this value of RNOM, the cold trip point is
about -7°C. Notice that the span is now 47°C rather than
the previous 50°C. This is due to the increase in “tem-
perature gain” of the thermistor as absolute temperature
decreases.
The upper and lower temperature trip points can be inde-
pendently programmed by using an additional bias resistor
as shown in Figure 9. The following formulas can be used
to compute the values of RNOM and R1:
RNOM
=
rCOLD – rHOT
2.815
• R25C
R1= 0.409 •RNOM – rHOT •R25C
For example, to set the trip points to -5°C and 55°C with
a Vishay Curve 2 thermistor choose
RNOM
=
3.532 – 0.3467
2.815 – 0.409
10k
=
13.2k
the nearest 1% value is 13.3k.
R1 = 0.409 • 13.3k – 0.3467 • 10k = 1.97k
the nearest 1% value is 1.96k. The final solution is shown
in Figure 9 and results in an upper trip point of 55°C and
a lower trip point of -5°C.
Power Dissipation and High Temperature
Considerations
The die temperature of the LTC4090/LTC4090-5 must be
lower than the maximum rating of 110°C. This is generally
not a concern unless the ambient temperature is above
85°C. The total power dissipated inside the LTC4090/
LTC4090-5 depend on many factors, including input voltage
(IN or HVIN), battery voltage, programmed charge current,
programmed input current limit, and load current.
In general, if the LTC4090/LTC4090-5 is being powered from
IN the power dissipation can be calculated as follows:
PD = (VIN – VBAT) • IBAT + (VIN – VOUT) • IOUT
where PD is the power dissipated, IBAT is the battery
charge current, and IOUT is the application load current.
For a typical application, an example of this calculation
would be:
PD = (5V – 3.7V) • 0.4A + (5V – 4.75V) • 0.1A
= 545mW
This examples assumes VIN = 5V, VOUT = 4.75V, VBAT =
3.7V, IBAT = 400mA, and IOUT = 100mA resulting in slightly
more than 0.5W total dissipation.
If the LTC4090 is being powered from HVIN, the power
dissipation can be estimated by calculating the regulator
power loss from an efficiency measurement, and subtract-
ing the catch diode loss.
PD = (1− η) • ⎡⎣VHVOUT •(IBAT +IOUT )⎤⎦
( )
VD ⎝⎜ 1
VHVOUT
VHVIN
⎠⎟
IBAT +IOUT )+ 0.3V •IBAT
where η is the efficiency of the high voltage regulator and
VD is the forward voltage of the catch diode at I = IBAT
+ IOUT. The first term corresponds to the power lost in
converting VHVIN to VHVOUT, the second term subtracts
the catch diode loss, and the third term is the power dis-
sipated in the battery charger. For a typical application,
an example of this calculation would be:
PD = (10.87) •[4V •(1A + 0.6A)]
0.4V
⎝⎜
1
4V
12V
⎠⎟
(1A
+
0.6A)
+
0.3V
1A
=
0.7W
This example assumes 87% efficiency, VHVIN = 12V, VBAT
= 3.7V (VHVOUT is about 4V), IBAT = 1A, IOUT = 600mA
resulting in about 0.7W total dissipation. If the LTC4090-5
is being powered from HVIN, the power dissipation can
be estimated by calculating the regulator power loss from
an efficiency measurement, and subtracting the catch
diode loss.
4090fa
24

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