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Electrostatic discharge is defined as the transfer of electrostatic
charge between bodies at different electrostatic potentials caused by direct
contact or induced by an electrostatic field.
The usual ESD consists of the release of stored charge from a capacitive
item, the capacitive item in the most fundamental form is the human body. Other
typical charge storing bodies include chassis, clothing, chairs etc. Most ESD
failures occur below the human sense of feeling to static discharge which begins
at about 4000 V. However, majority of integrated circuits and many discrete
parts fail at thresholds below 4000V. The sensation of feeling from static
discharge is rare occurrence except under extremely dry atmospheric conditions.
Typical
susceptibility levels:
| Technology | Susceptibility level |
| MOSFET,JFET | 150V to 250 V |
| Bipolar Opamp, Schottky diode, ECL | 400V to 500V |
| CMOS | 800V |
| Schottky TTL, thin film resistor, TTL | 1000V to 1500V |
| Bipolar transistor | 1500V |
2.
ESD and EOS (Electrical Overstress):
Electrical overstress (EOS) failure other than ESD is usually of longer
time duration, generally greater than 50 ms.
Typical EOS sources are 230 VAC, 50 Hz, accidental short to a dc or ac potential
exceeding the gate-oxide breakdown or system transients of varying durations. In
these cases the heating is normally sustained longer than during the typical ESD
exposure, thus resulting in more extensive damage. Generally, EOS transients are
of longer duration than ESD transients. In
addition EOS- caused failures can be of either forward or reverse bias. Forward
bias EOS is typically evidenced by resultant damage of high currents such as
melting and / vaporization of intra-connects. For example, a TTL input gate
exposed to 14V for 200 ms with a peak current of 500 mA resulting in the
high current melting of intraconnects.
The most prevalent junction damage from ESD occurs in the reverse biased
condition and is evidenced by a degraded I-V characteristic. Degradation can be
from a nearly negligible shift of the curve to a short circuit. Physical damage
is invisible upon microscopic examination of the chip surface, except in most
severe cases.
For a surface, the resistance
decreases in proportion to the width, W, and increases proportionately with
length, l.
Resistivity, R is given by
R= k l /W
Where k is a proportionality
constant.
In case of a square, where l
=W, the equation reduces to
R=k
As can be seen from the
equation, if l=W, the size of l and W does not matter, so the size of the square
is immaterial. In other words,
rs
= surface resistivity =k = resistance when l = W
Antistatic
: 10 9 to 10 14
However, the above are only
indicative and the limits may be tailored to individual requirements if
necessary.
Effect of humidity:
Higher humidity will increase the moisture content of materials to
varying degrees depending upon the material. This increased moisture content
will reduce the resistivity.
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