Leakage current
Peak pulse current
Capacitance per line
Dynamic resistance
min.max.max.typ.max.typ.max.
VVmAµAVm
6.17.2113110067.59.5
R
V
V
CL
slope : 1 / R
IRM@V
RM
V
RM
BR
I
RM
I
R
d
RdαTC C
note 1note 23V bias3V bias
Ω10
I
PP
-4
/°CpFpF
V
2/9
ESDALC6V1W5
Fig. 1: Relative variation of peak pulse power
versus initial junction temperature.
Ppp[Tj initial] / Ppp [Tj initial = 25°C]
1.1
1.0
0.9
0.8
0.7
0.6
0.5
0.4
0.3
0.2
0.1
0.0
0255075100125150175
Tj(°C)
Fig. 3: Junction capacitance versus reverse voltage
applied (typical values).
C(pF)
14
12
F=1MHz
Vosc=30mV
Tj=25°C
RMS
Fig. 2: Peak pulse power versusexponential pulse
duration.
Ppp(W)
100
tp(µs)
10
110100
Tj initial = 25°C
Fig. 4: Clamping voltage versus peak pulse current (maximum values, rectangular waveform).
Ipp(A)
100.0
10
8
6
4
2
0
012345
VR(V)
Fig. 5: Relative variation of leakage current versus
junction temperature (typical values).
IR [Tj] / IR [Tj=25°C]
100
10
1
255075100125
Tj(°C)
10.0
1.0
Vcl(V)
0.1
0 102030405060
tp=2.5µs
Tj initial =25°C
Fig. 6: Application example
I/02
I/01
Connector
I/04
I/03
IC
to be
protected
3/9
ESDALC6V1W5
TECHNICAL INFORMATION
1. ESD protection by ESDALC6V1W5
With the focus of lowering the operation levels, the problem of malfunction caused by the environment is
critical. Electrostatic discharge (ESD) is a major cause of failure in electronic systems.
As a transient voltage suppressor, ESDALC6V1W5 is an ideal choice for ESD protection by suppressing
ESDevents. It is capableof clamping theincoming transient toa low enough levelsuch that anydamage is
prevented on the device protected by ESDALC6V1W5.
ESDALC6V1W5 serves as a parallel protection elements, connected between the signal line and ground.
As the transient rises above the operating voltage of the device, the ESDALC6V1W5 becomes a low
impedance path diverting the transient current to ground.
The clamping voltage is given by the following formula:
=VBR+ Rd.I
V
CL
As shown in figure A1, the ESD strikes are clamped by the transient voltage suppressor.
Fig. A1: ESD clamping behavior
G
R
I
PP
PP
Rd
R
V
G
V
BR
V(i/o)
ESD surgeESDALC6V1W5
Tohave a goodapproximation of the remainingvoltages at both Vi/o side, we providethe typical dynamical
resistance value Rd. By taking into account the following hypothesis:
Rg > Rd and Rload > Rd
we have:
Vi oVR
/=+×
()
The results of the calculation done Vg = 8kV, Rg = 330Ω (IEC61000-4-2 standard), V
Rd = 1.1Ω (typ.) give:
V i oVolts
/,=32 8
()
This confirms the very low remaining voltage across the device to be protected. It is also important to note
that in this approximation the parasitic inductance effect was not taken into account. This could be a few
tenths of volts during a few ns at the Vi/o side.
BRd
V
R
g
g
L OAD
Device
to be
protected
= 6.1V (min) and
BR
4/9
ESDALC6V1W5
Fig. A2: ESD test board
Fig. A3: ESD test configuration
TEST BOARD
V(i/o)
V(i/o)
± 8kV
ESD Contact
discharge
The measurements done here after show very clearly (Fig. A4) the high efficiency of the ESD protection:
the clamping voltage V(i/o) becomes very close to +V
Fig. A4b).
Fig. A4: Remaining voltage during ESD surge
(positive way, Fig. A4a) and -VBR(negative way,
BR
I/O1, I/O2, I/O3 or I/O4
V(i/o)
B2
V(i/o)
a: Response in the positive wayb: Response in the negative way
V(i/o)
5/9
ESDALC6V1W5
CROSSTALK BEHAVIOR
Fig. A5: Crosstalk phenomenon
RG1
V
G1
RG2
VG2
Line 1
Line 2
R
L1
R
L2
αβ
αβ
V+ V
1G112G2
V+ V
2G221G1
DRIVERSRECEIVERS
Thecrosstalk phenomena are dueto the coupling between 2lines. Coupling factors ( β12or β21 ) increase
when the gap across lines decreases, particularly in silicon dice. In the example above, the expected
signal on load R
the V
phenomenon has to be taken into account when the drivers impose fast digital data or high frequency
analog signals. The perturbed line will be more affected if it works with low voltage signal or high load
impedance (few kΩ)
signal represents the effect of the crosstalk phenomenon of the line 1 on the line 2. This
G1
is α2VG2, in fact the real voltage at this point has got an extra value β21VG2. This part of
L2
Fig. A6: Analog crosstalk measurements
RFTEST BOARD
TEST BOARD
To Port1
To Port1To Port1
6/9
I/O4
I/O4
I/O1
I/O1
To Port2
To Port2To Port2
ESDALC6V1W5
Fig. A7: Typical analog crosstalk measurements.
ESDALC6V1W5 :typical analog crosstalk response
0.00
dB
-10.00
-20.00
-30.00
-40.00
-50.00
-60.00
-70.00
-80.00
-90.00
-100.0
1.0M3.0M10.0M30.0M100.0M 300.0M1.0G3.0G
Figure A6gives the measurement circuit for the analog crosstalk application. In figure A7, the curve shows
the effect of the line I/O1 on the line I/O4. In usual frequency range of analog signals (up to 100MHz) the
effect on disturbed line is less than -60dB.
f/Hz
Fig. A8: Digital crosstalk measurements configu-
Fig. A9: Digital crosstalk results.
ration.
0 - 3kV
pulse generator
F= 5MHz
R
t = 3ns
I/O1
V
G1
I/O4
unloaded
GND
β21 G1V
unloaded
VG1
β21 G1V
rise time: t= 3ns
10-90%
crosstalk
Figure A8 shows the measurement circuit used to quantify the crosstalk effect in a classical digital
application.
Figure A9 shows that in such a condition, the impact on the disturbed lineis less than 50mV peak to peak.
No data disturbance was noted on the concerned line. The measurements performed with falling edges
give an impact within the same range.
Mechanical specifications
Lead platingTin-lead
Lead plating thickness5µm min.
25 µm max.
Lead materialSn / Pb
(70% to 90% Sn)
Lead coplanarity10µm max.
Body materialMoldedepoxy
Epoxy meetsUL94,V0
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