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LTC1645 Просмотр технического описания (PDF) - Linear Technology

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LTC1645 Datasheet PDF : 24 Pages
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LTC1645
APPLICATIO S I FOR ATIO
No bulk capacitance is present to slow the rate of rise and
heavily damp the parasitic resonance. Instead, the fast
edge shock excites a resonant circuit formed by a combi-
nation of wiring harness, backplane and circuit board
parasitic inductances and FET capacitance. In theory, the
peak voltage should rise to 2X the input supply, but in
practice the peak can reach 2.5X, owing to the effects of
voltage dependent FET capacitance.
The absolute maximum VCCn potential for the LTC1645 is
13.2V; any circuit with an input of 5V or greater should be
scrutinized for ringing. A well-bypassed backplane should
not escape suspicion: circuit board trace inductances of as
little as 10nH can produce sufficient ringing to overvoltage
VCC.
Check ringing with a fast storage oscilloscope (such as a
LECROY 9314AL DSO) by attaching coax or a probe to VCC
and GND, then repeatedly inserting the circuit board into
the backplane. Figures 5a and 5b show typical results in a
12V application with different VCC lead lengths. The peak
amplitude reaches 22V, breaking down the ESD protection
diode in the process.
There are two methods for eliminating ringing: clipping
and snubbing. A transient voltage suppressor is an effec-
tive means of limiting peak voltage to a safe level.
Figure␣ 6 shows the effect of adding an ON Semiconductor,
1SMA12CAT3, on the waveform of Figure 5.
Figures 7a and 7b show the effects of snubbing with
different RC networks. The capacitor value is chosen as
10X to 100X the FET COSS under bias and R is selected for
best damping—1to 50depending on the value of
parasitic inductance.
8'
12V –+
POWER
LEADS
SCOPE
PROBE
R1
0.01
IRF7413
+
10
VOUT
CLOAD
LTC1645
0.1µF
1645 F05
24V
24V
0V
0V
1µs/DIV
1645 F05a
(a) Undamped VCC Waveform (48" Leads)
1µs/DIV
1645 F05b
(b) Undamped VCC Waveform (8" Leads)
Figure 5. Ring Experiment
9

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