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LT3748H(RevA) Просмотр технического описания (PDF) - Linear Technology

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производитель
LT3748H
(Rev.:RevA)
Linear
Linear Technology Linear
LT3748H Datasheet PDF : 30 Pages
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LT3748
APPLICATIONS INFORMATION
Although it typically does not decrease efficiency, leakage
inductance energy that would normally have been dis-
sipated in the switch or transformer is also dissipated in
the RC snubber resistor and can be calculated as:
PSNUBBER = fSW • LLEAK • ILIM2/2
An RCD clamp, shown in Figure 7, also prevents the
leakage inductance spike from exceeding the breakdown
voltage of the MOSFET switch. In most applications, there
will be a very fast voltage spike caused by a slow clamp
diode. Once the diode clamps, the leakage inductance
current is absorbed by the clamp capacitor. This period
should not last longer than 200ns so as not to interfere
with the output regulation. The clamp diode turns off after
the leakage inductance energy is absorbed and the switch
voltage is then equal to:
VDS = VIN + NPS • (VOUT + VF(DIODE))
Schottky diodes are typically the best choice for use in a
snubber, but some PN diodes can be used if they turn on
fast enough to limit the leakage inductance spike. Figures 8
and 9 show the waveform at the drain of the MOSFET
switch for the 48V output application shown in Figure 17
at maximum rated load and maximum input voltage with
an RC snubber and RCD clamp, respectively. Both solu-
tions limit the leakage spike to less than 190V, below the
200V VDS(MAX) rating of the Si7464DP MOSFET.
LLEAK
VIN
CR
VOUT+
D
GATE
NMOS
3748 F07
Figure 7. RCD Clamp
VOUT–
Leakage Inductance and Output Diode Stress
The output diode may also see increased reverse voltage
stresses from leakage inductance. While it nominally sees
a reverse voltage of the input voltage divided by the wind-
ings ratio plus the output voltage when the MOSFET power
switch turns on, the capacitance on the output diode and
the leakage inductance will cause an LC tank which may
16
ring beyond that expected reverse voltage. An RC snubber
or RCD clamp may be implemented to reduce the voltage
spike if it is desirable to use a lower reverse voltage diode.
Secondary Leakage Inductance
In addition to the previously described effects of leakage
inductance in general, leakage inductance on the secondary
in particular exhibits an additional phenomena. It forms an
inductive divider on the transformer secondary that effec-
tively reduces the size of the primary-referred flyback pulse
used for feedback. This will increase the output voltage
target by a similar percentage. Note that, unlike leakage
spike behavior, this phenomena is load independent. To the
extent that the secondary leakage inductance is a constant
percentage of mutual inductance (over manufacturing
200
180
160
140
120
100
80
60
40
20
0
0
VIN = 96V
VOUT = 48V
IOUT = 0.5A
R = 66Ω
C = 150pF
50 100 150 200 250 300
TIME (ns)
3748 F08
Figure 8. Waveform of MOSFET Drain During Normal Operation
of Figure 17 with RC Snubber (as Drawn)
200
180
160
140
120
100
80
60
40
20
0
0
VIN = 96V
VOUT = 48V
IOUT = 0.5A
R = 4.99k
C = TDK 0.22μF 250V
D = CMR1U-02M-LTC
50 100 150 200 250 300
TIME (ns)
3748 F08
Figure 9. Waveform of MOSFET Drain During Normal Operation
of Figure 17 Using RCD Clamp with Central Semiconductor
CMR1U-02M-LTC Instead of RC Snubber
3748fa

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