About ESD
Background
Most
people only think of static electricity as the shock from touching
a metal doorknob after walking across a carpet. However,
static discharge can be very dangerous in modern work environments. Electronic
devices have become more sensitive to static discharge as they've
become faster and smaller. ESD impacts productivity and
product reliability in almost every aspect of today's electronics
environment. Electrostatic control also applies to other
industries such as clean room applications and graphic arts.
ESD
affects manufacturing costs, product quality, production yields,
product reliability, and profitability. Experts have estimate
the average product losses due to static to be from 8-33%. This
could quantify the amount lost due to ESD, or electro-static
discharge, to be in the billions every year. Whether
it's the cost of a damaged diode which may only cost a few cents
or a complex hybrids which could run a company several hundred
dollars, the threat of ESD is a growing concern. Other
losses due to ESD could be costs of repair and rework, re-shipping,
extra labor..
Creating
a Static Electricity Charge
Static
electricity is an electrical charge caused by an imbalance of
electrons on a surface. This imbalance creates a measurable
electric field that can influence other objects at a distance. Electrostatic
discharge is the transfer of charge between bodies at different
electrical potentials.
Electrostatic
discharge can change the electrical characteristics of a semiconductor
device, degrading or destroying it. Electrostatic discharge
also may upset the normal operation of an electronic system,
causing equipment malfunction or failure. Another problem
caused by static electricity occurs in clean rooms. Charged
surfaces can attract and hold contaminants, making removal from
the environment difficult. When attracted to the surface
of a silicon wafer or a device's electrical circuitry, these
particulates can cause random wafer defects and reduce product
yields.
Controlling
electrostatic discharge begins with understanding how electrostatic
charge occurs in the first place. Electrostatic charge
is most commonly created by the contact and separation of two
materials. For example, a person walking across the floor
generates static electricity as shoe soles contact and then
separate from the floor surface. An electronic device
sliding into or out of a bag, magazine or tube generates an
electrostatic charge as the device's housing and metal leads
make multiple contacts and separations with the surface of
the container. While the magnitude of electrostatic charge
may be different in these examples, static electricity is indeed
generated.
Creating
electrostatic charge by contact and separation of materials is
known as "triboelectric charging." It involves the
transfer of electrons between materials. The atoms of a
material with no static charge have an equal number of positive
(+) protons in their nucleus and negative (-) electrons orbiting
the nucleus.
When
the two materials are placed in contact and then separated, negatively
charged electrons are transferred from the surface of one material
to the surface of the other material. Which material loses
electrons and which gains electrons will depend on the nature
of the two materials. The material that loses electrons
becomes positively charged, while the material that gains electrons
is negatively charged.
This
process of material contact, electron transfer and separation
is really a more complex mechanism than described here. The
amount of charge created by triboelectric generation is affected
by the area of contact, the speed of separation, relative humidity,
and other factors. Once the charge is created on a material,
it becomes an "electrostatic" charge (if it remains
on the material). This charge may be transferred from the
material, creating an electrostatic discharge, or ESD, event. Additional
factors such as the resistance of the actual discharge circuit
and the contact resistance at the interface between contacting
surfaces also affect the actual charge that can cause damage.
Examples
of Static Generation
Typical Voltage Levels |
| Means
of Generation |
10-25%
RH |
65-90%
RH |
| Walking
across carpet |
35,000V |
1,500V |
| Walking
across vinyl tile |
12,000V |
250V |
| Worker
at bench |
6,000V |
100V |
| Poly
bag picked up from bench |
20,000V |
1,200V |
| Chair
with urethane foam |
18,000V |
1,500V |
An
electrostatic charge also may be created on a material in other
ways such as by induction, ion bombardment, or contact with another
charged object. However, triboelectric charging is the
most common.
How
Material Characteristics Affect Static Charge
Triboelectric
Series
When
two materials contact and separate, the polarity and magnitude
of the charge are indicated by the materials' positions in the
triboelectric series. The triboelectric series tables show
how charges are generated on various materials. When two
materials contact and separate, the one nearer the top of the
series takes on a positive charge, the other a negative charge. Materials
further apart on the table typically generate a higher charge
than ones closer together. These tables, however, should
only be used as a general guide because there are many variables
involved that cannot be controlled well enough to ensure repeatability.
Virtually
all materials, including water and dirt particles in the air,
can be triboelectrically charged. How much charge is generated,
where that charge goes, and how quickly, are functions of the
materials' electrical characteristics.
Insulative
Materials
A
material that prevents or limits the flow of electrons across
its surface or through its volume is called an insulator. Insulators
have an extremely high electrical resistance, generally greater
than 1 x 10E12 ohms/sq (surface resistivity) and 1 x 10E11 ohm-cm
(volume resistivity). A considerable amount of charge can
be generated on the surface of an insulator. Because an
insulative material does not readily allow the flow of electrons,
both positive and negative charges can reside on insulative surface
at the same time, although at different locations. The
excess electrons at the negatively charged spot might be sufficient
to satisfy the absence of electrons at the positively charged
spot. However, electrons cannot easily flow across the
insulative material's surface, and both charges may remain in
place for a very long time.
Conductive
Materials
A
conductive material, because it has low electrical resistance,
allows electrons to flow easily across its surface or through
its volume. Conductive materials have low electrical resistance,
generally less than 1 x 10E5 ohms/sq (surface resistivity) and
1 x 10E4 ohm-cm (volume resistivity). When a conductive
material becomes charged, the charge (i.e., the deficiency or
excess of electrons) will be uniformly distributed across the
surface of the material. If the charged conductive material
makes contact with another conductive material, the electrons
will transfer between the materials quite easily. If the
second conductor is attached to an earth grounding point, the
electrons will flow to ground and the excess charge on the conductor
will be "neutralized."
Electrostatic
charge can be created triboelectrically on conductors the same
way it is created on insulators. As long as the conductor
is isolated from other conductors or ground, the static charge
will remain on the conductor. If the conductor is grounded
the charge will easily go to ground. Or, if the charged
conductor contacts or nears another conductor, the charge will
flow between the two conductors.
Static
Dissipative Materials
Static
dissipative materials have an electrical resistance between insulative
and conductive materials (1 x 10E5 - 1 x 10E12 ohms/sq (surface
resistivity) and 1 x 10E4 - 1 x 10E11 ohm-cm (volume resistivity). There
can be electron flow across or through the dissipative material,
but it is controlled by the surface resistance or volume resistance
of the material.
As
with the other two types of materials, charge can be generated
triboelectrically on a static dissipative material. However,
like the conductive material, the static dissipative material
will allow the transfer of charge to ground or other conductive
objects. The transfer of charge from a static dissipative
material will generally take longer than from a conductive material
of equivalent size. Charge transfers from static dissipative
materials are significantly faster than from insulators, and
slower than from conductors.
Electrostatic
Fields
Charged
materials also have an electrostatic field and lines of force
associated with them. Conductive objects brought into the
vicinity of this electric field will be polarized by a process
known as induction. A negative electric field will repel
electrons on the surface of the conducting item that is exposed
to the field. A positive electric field will attract electrons
to near the surface thus leaving other areas positively charged. No
change in the actual charge on the item will occur in polarization. If,
however, the item is conductive or dissipative and is touched
to ground while polarized, charge will flow from or to ground
to compensate for the charge imbalance. If the electrostatic
field is removed and the ground contact disconnected, the charge
will be trapped on the item. If a nonconductive object
is brought into the electric field, the electrical dipoles will
tend to align with the field creating apparent surface charges. A
nonconductor cannot be charged by induction.
ESD
Damage-How Devices Fail
Electrostatic
damage to electronic devices can occur at any point from manufacture
to field service. Damage results from handling the devices
in uncontrolled surroundings or when poor ESD control practices
are used. Generally damage is classified as either a catastrophic
failure or a latent defect.
Catastrophic
Failure
When
an electronic device is exposed to an ESD event, it may no longer
function. The ESD event may have caused a metal melt,
junction breakdown, or oxide failure. The device's circuitry
is permanently damaged causing the device fail. Such failures
usually can be detected when the device is tested before shipment. If
the ESD event occurs after test, the damage will go undetected
until the device fails in operation.
Latent
Defect
A
latent defect, on the other hand, is more difficult to identify. A
device that is exposed to an ESD event may be partially degraded,
yet continue to perform its intended function. However,
the operating life of the device may be reduced dramatically. A
product or system incorporating devices with latent defects may
experience premature failure after the user places them in service. Such
failures are usually costly to repair and in some applications
may create personnel hazards.
It
is relatively easy with the proper equipment to confirm that
a device has experienced catastrophic failure. Basic performance
tests will substantiate device damage. However, latent
defects are extremely difficult to prove or detect using current
technology, especially after the device is assembled into a finished
product.
Basic
ESD Events--What Causes Electronic Devices to Fail?
ESD
damage is usually caused by one of three events: direct electrostatic
discharge to the device, electrostatic discharge from the device
or field-induced discharges. Damage to an ESDS device by
the ESD event is determined by the device's ability to dissipate
the energy of the discharge or withstand the voltage levels involved. This
is known as the device's "ESD sensitivity.
Discharge
to the Device
An
ESD event can occur when any charged conductor (including the
human body) discharges to an ESDS (electrostatic discharge sensitive)
device. The most common cause of electrostatic damage is
the direct transfer of electrostatic charge from the human body
or a charged material to the electrostatic discharge sensitive
(ESDS) device. When one walks across a floor, an electrostatic
charge accumulates on the body. Simple contact of a finger
to the leads of an ESDS device or assembly allows the body to
discharge, possibly causing device damage. The model used
to simulate this event is the Human Body Model (HBM). A
similar discharge can occur from a charged conductive object,
such as a metallic tool or fixture. The model used to characterize
this event is known as the Machine Model.
Discharge
from the Device
The
transfer of charge from an ESDS device is also an ESD event. Static
charge may accumulate on the ESDS device itself through handling
or contact with packaging materials, worksurfaces, or machine
surfaces. This frequently occurs when a device moves across
a surface or vibrates in a package. The model used to
simulate the transfer of charge from an ESDS device is referred
to as the Charged Device Model (CDM). The capacitance and
energies involved are different from those of a discharge to
the ESDS device. In some cases, a CDM event can be more
destructive than the HBM for some devices.
The
trend towards automated assembly would seem to solve the problems
of HBM ESD events. However, it has been shown that components
may be more sensitive to damage when assembled by automated equipment. A
device may become charged, for example, from sliding down the
feeder. If it then contacts the insertion head or another
conductive surface, a rapid discharge occurs from the device
to the metal object.
Field
Induced Discharges
Another
event that can directly or indirectly damage devices is termed
Field Induction. As noted earlier, whenever any object
becomes electrostatically charged, there is an electrostatic
field associated with that charge. If an ESDS device is
placed in that electrostatic field, a charge may be induced on
the device. If the device is then momentarily grounded
while within the electrostatic field, a transfer of charge from
the device occurs as a CDM event. If the device is removed
from the region of the electrostatic field and grounded again,
a second CDM event will occur as charge (of opposite polarity
from the first event) is transferred from the device.
How
Much Static Protection is Needed?
As
noted earlier, damage to an ESDS device by the ESD event is determined
by the device's ability to dissipate the energy of the discharge
or withstand the voltage levels involved-its ESD sensitivity. Defining
the ESD sensitivity of electronic components is the first step
in determining the degree of ESD protection required. Test
procedures based on the models of ESD events help define the
sensitivity of components to ESD. These procedures will
be covered in a future article in this series.
Many
electronic components are susceptible to ESD damage at relatively
low voltage levels. Many are susceptible at less than 100
volts, and many disk drive components have sensitivities below
10 volts. Current trends in product design and development
pack more circuitry onto these miniature devices, further increasing
their sensitivity to ESD and making the potential problem even
more acute.
Summary
In
this introductory article on electrostatic discharge, we have
discussed the basics of electrostatic charge and discharge, types
of failures, ESD events, and device sensitivity. We can
summarize this discussion as follows:
1. Virtually
all materials, even conductors, can be triboelectrically charged.
2. The
level of charge is affected by material type, speed of contact
and separation, humidity, and several other factors.
3. Electrostatic
fields are associated with charged objects.
4. Electrostatic
discharge can damage devices so they fail immediately, or ESD
may result in latent damage that may escape immediate attention,
but cause the device to fail prematurely once in service.
5. Electrostatic
discharge can occur throughout the manufacturing, test, shipping,
handling, or operational processes.
6. Component
damage can occur as the result of a discharge to the device,
from the device, or from charge transfers resulting from electrostatic
fields. Devices vary significantly in their sensitivity
to ESD.
Protecting
your products from the effects of static damage begins by understanding
these key concepts of ESD. Armed with this information,
you can then begin to develop an effective ESD control program.
References
We
would like to thank the MidWest
Chapter ESD Association for allowing us to use this
data.
ESD-ADV
1.0, Glossary, ESD Association, Rome NY.
ESD
TR20.20, Handbook, ESD Association, Rome, NY.
ESD
ADV 11.2, Triboelectric Charge Accumulation Testing,
ESD Association, Rome, NY.
ANSI/ESD
S20.20-Standard for the Development of Electrostatic Discharge
Control Program, ESD Association, Rome, NY.

Footnotes
(1)Stephen
A. Halperin, "Guidelines for Static Control Management," Eurostat,
1990.
(2)Lonnie
Brown and Dan Burns, "The ESD Control Process as a Tool
for Managing Quality," Electronic Packaging and Production, April
1990, pp 50-53.
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