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1766IFE View Datasheet(PDF) - Linear Technology

Part Name
Description
Manufacturer
1766IFE Datasheet PDF : 30 Pages
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LT1766/LT1766-5
APPLICATIONS INFORMATION
Thermal resistance for the LT1766 packages is influenced
by the presence of internal or backside planes.
SSOP (GN16) package: With a full plane under the GN16
package, thermal resistance will be about 85°C/W.
TSSOP (exposed pad) package: With a full plane under
the TSSOP package, thermal resistance will be about
45°C/W.
To calculate die temperature, use the proper thermal
resistance number for the desired package and add in
worst-case ambient temperature:
TJ = TA + (θJA • PTOT)
When estimating ambient, remember the nearby catch
diode and inductor will also be dissipating power:
PDIODE
=
(VF
)(VIN
– VOUT
VIN
)(ILOAD)
VF = Forward voltage of diode (assume 0.63V at 1A)
PDIODE
=
(0.63)(40
40
5)(1)
=
0.55W
PINDUCTOR = (ILOAD)2 (RL)
RL = Inductor DC resistance (assume 0.1Ω)
PINDUCTOR (1)2 (0.1) = 0.1W
Only a portion of the temperature rise in the external inductor
and diode is coupled to the junction of the LT1766. Based
on empirical measurements the thermal effect on LT1766
junction temperature due to power dissipation in the external
inductor and catch diode can be calculated as:
ΔTJ(LT1766) ≈ (PDIODE + PINDUCTOR)(10°C/W)
Using the example calculations for LT1766 dissipation, the
LT1766 die temperature will be estimated as:
TJ = TA + (θJA • PTOT) + [10 • (PDIODE + PINDUCTOR)]
With the GN16 package (θJA = 85°C/W), at an ambient
temperature of 60°C:
TJ = 60 + (85 • 0.53) + (10 • 0.65) = 112°C
With the TSSOP package (θJA = 45°C/W), at an ambient
temperature of 60°C:
TJ = 60 + (45 • 0.53) + (10 • 0.65) = 90°C
Die temperature can peak for certain combinations of VIN,
VOUT and load current. While higher VIN gives greater
switch AC losses, quiescent and catch diode losses, a
lower VIN may generate greater losses due to switch DC
losses. In general, the maximum and minimum VIN levels
should be checked with maximum typical load current
for calculation of the LT1766 die temperature. If a more
accurate die temperature is required, a measurement of
the SYNC pin resistance (to GND) can be used. The SYNC
pin resistance can be measured by forcing a voltage no
greater than 0.5V at the pin and monitoring the pin cur-
rent over temperature in an oven. This should be done
with minimal device power (low VIN and no switching
(VC = 0V)) in order to calibrate SYNC pin resistance with
ambient (oven) temperature.
Note: Some of the internal power dissipation in the IC,
due to BOOST pin voltage, can be transferred outside
of the IC to reduce junction temperature, by increasing
the voltage drop in the path of the boost diode D2 (see
Figure 9). This reduction of junction temperature inside
the IC will allow higher ambient temperature operation for
a given set of conditions. BOOST pin circuitry dissipates
power given by:
PDISS(BOOST)
=
VOUT
• (ISW / 36) • VC2
VIN
Typically VC2 (the boost voltage across the capacitor C2)
equals Vout. This is because diodes D1 and D2 can be
considered almost equal, where:
VC2 = VOUT – VFD2 – (–VFD1) = VOUT
Hence the equation used for boost circuitry power dissi-
pation given in the previous Thermal Calculations section
is stated as:
PDISS(BOOST)
=
VOUT
• (ISW / 36)• VOUT
VIN
Here it can be seen that boost power dissipation increases
as the square of VOUT. It is possible, however, to reduce VC2
below VOUT to save power dissipation by increasing the
voltage drop in the path of D2. Care should be taken that
VC2 does not fall below the minimum 3.3V boost voltage
required for full saturation of the internal power switch.
1766fc
21

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