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Connector Degradation Mechanism
By
Robert S. Mroczkowski, Sc.D
Bishop & Associates Inc.
This is the first in a
series of articles about connector degradation mechanisms. The purpose
of this article is to provide a rationale as to why they are important
to connector performance. Following articles will discuss degradation
mechanisms in additional detail. At the end of this article, you will be
able to provide feedback on this subject and also be able to participate
in an online discussion with others in the industry. If you have
specific questions regarding future topics, email them to
questions@connectorsupplier.com, and we will respond.
Connectors are used in order to provide a separable connection between
two subsystems. There are many reasons separability is necessary,
ranging from manufacturing convenience to performance upgrades. When
mated, however, the connector should not introduce any unacceptable
resistance between the systems. “Unacceptable” resistance means any
resistance that could cause malfunction of the system either through
signal distortion or power loss, depending on the application
requirement. The reason connector degradation mechanisms are important
is that they are the potential source of resistance increases, and,
therefore, field failures over time.
Let’s begin with a brief review of connector resistance. Figure 1 shows
a cross section of a generic signal connector. The equation in Figure 1
indicates the various sources of resistance within the connector. RO
is the overall resistance of the connector, and is the resistance
between a probe attached to the conductor behind the crimped connection,
and a probe making contact to the appropriate pad on the printed circuit
board containing the press-in compliant pin connection. Two permanent
connection resistances, RP.C., are shown—the resistance of
the crimped connection and the compliant pin connection. Similarly,
there are two bulk resistances—RBulk—the bulk resistance of
the post contact and that of the parallel resistance combination of the
two beams of the receptacle contact. Only one interface, or separable
contact resistance, RC, is shown, because it is difficult to
separate the parallel resistances of the two contact points. The overall
connector resistance is the sum of the individual permanent connection
resistances, the post and receptacle contact bulk resistances, and the
separable contact resistance, because all these resistances are
electrically in series.

Figure 1. Schematic illustration of the components of connector
resistance. Overall, RO, bulk, RBulk ,
permanent connection, RP.C , and contact interface, RC
, resistance contributions are shown.
For the sake of
discussion, let us assume that the measured overall resistance, RO,
is 15 milliohms. Given that assumption, take a minute or two at this
point and guesstimate the relative contributions of the permanent, bulk,
and separable interface resistances to the overall connector
resistances.
In this example, and these values are typical of a soft-shell style
connector, the bulk resistances will make up the majority of the overall
resistance, approaching 14 milliohms. The permanent connection
resistances will be of the order of a few hundred microohms and the
separable interface resistance of the order of a milliohm.
Though the bulk resistance of the connector contacts is by far the
largest contributor to the connector resistance, it is also the most
stable. The bulk resistance of the individual contacts is determined by
the materials of manufacture of the contacts and their overall geometry.
In a simple example, consider the resistance of a length of a conductor,
which is given by
Rcond. =
r l/a.
In this equation,
r
is the resistivity of the conductor, or in a connector, the contact
spring material, “l” is the length of the conductor, and “a” is the
cross-sectional area of the conductor, or in a connector, the geometry
of the contact spring system. For a given material choice, say phosphor
bronze, and contact geometry, these parameters are constants and,
therefore, the bulk resistance of a connector is constant.
The permanent connection resistance and the interface, or separable
connection, resistance, are variable. It is these resistance
contributions that are susceptible to a variety of degradation
mechanisms, as will be discussed in later articles. At this point,
suffice it to say that if a connector is subjected to a test program to
assess its performance, harsh environments, heat, age, vibration, etc.,
and the overall connector resistance changes from the original15
milliohms to, say, 100 milliohms, the change in resistance will occur in
the separable and permanent connection resistances. The separable
interface resistance is the most susceptible to degradation because the
requirement for separability places limitations on the forces and
deformations that can be applied to create the separable interface.
Simplistically, there are two major separable interface requirements
that limit those forces and deformations. The connector mating force is
the first and most obvious requirement. To realize high pin count
connectors, the mating force of the individual contacts must be
controlled, and the contact normal force is one of the major parameters
that is limited by that requirement. For example, separable connection
contact forces are of the order of tens to a few hundred grams, while
insulation displacement connection, or IDC, forces are of the order of a
few thousand grams, as are the forces in compliant press-in connections.
The high forces typical of such permanent connections provide much
greater mechanical stability and lower resistances than can be realized
with the significantly lower forces of separable connections.
In a similar fashion, the higher forces of permanent connections allows
for greater deformation of the contact surfaces, compared to that of
separable connections. Crimped connections are the most obvious example
where significant deformation of the crimp terminal, as well as of the
individual conductor strands, are obvious. The forces of IDC and
compliant pin interfaces also permit much larger deformations of the
contact surfaces. As with the higher forces, the larger surface
deformations of permanent connections reduce their resistance as
compared to separable contact resistances.
The deformation of separable connection surfaces is also limited by
another separable interface requirement: mating durability. High surface
deformations generally result in high surface wear, which in turn may
result in the loss of any contact coating, gold or tin for example, on
the contact surface. The loss of such coatings will increase the
corrosion susceptibility of the contact surface, as will be discussed in
subsequent articles.
The combination of these two separable interface requirements, mating
force and mating durability, limit the deformations and mechanical
stability of separable interfaces, and is the reason for the lower
electrical stability of separable interfaces, as compared to permanent
connections.
The same limitations also explain why the electrical resistance of
separable interfaces is lower than that of permanent connections. In
general, the larger the area in contact between two surfaces, the lower
the electrical resistance of the interface. In effect, the contact area
between two surfaces is analogous to the cross-sectional area in the
equation, for the resistance of a length of conductor, Rcond.
= rl/a. Because separable connections have a lower contact area
than permanent connections, they have a higher electrical resistance.
To summarize, the reduced force of separable connections results in
lower mechanical stability and the reduced contact area results in
higher electrical resistance as compared to permanent connections.
These same issues, reduced contact force and reduced contact area,
directly affect the susceptibility of separable contact interfaces to
degradation. Figure 2 shows a schematic illustration of a separable
contact interface at high magnification. The main point of the figure is
to illustrate that, on the microscale of such contact interfaces, all
surfaces are rough. This dictates that the contact interface itself will
consist of a distribution of contact spots, called a-spots or
asperities, rather than a full area contact. This asperity structure is
what gives rise to the contact interface resistance. The reduced contact
area, consisting of a distribution of a-spots over some geometric area
depending on the geometry of the surfaces in contact, introduces a
resistance, called constriction resistance, that results from the
current flow being constricted to flow through the individual a-spots.
Constriction resistance can be reduced by increasing the contact area by
various means, but never eliminated. Therefore, a connector must always
introduce some resistance into an electrical system. From this
perspective, the prime objective of connector design is to control both
the magnitude and stability of the resistance that is introduced.

Figure 2: Schematic
illustration of the structure of a contact interface resulting from
the intrinsic surface roughness on the microscale of the contact
interface.
As
mentioned, the magnitude of interface resistance is determined by the
contact area that is created as the plug and receptacle contacts engage
one another. There are two major factors that affect the stability of
contact resistance: disturbance of the contact interface and corrosion
of the a-spots. These effects define the connector degradation
mechanisms that will be discussed in the following articles. In summary,
these mechanisms are:
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Corrosion in and around
the contact interface, so as to reduce the contact area. Two
corrosion related mechanisms will be discussed: Surface corrosion,
which directly impacts the contact area, and induced or fretting
motions, which can enhance the susceptibility of the contact
interface to corrosion.
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Loss of the integrity of
the contact plating, by inadequate plating and/or plating wear,
resulting in enhanced susceptibility to corrosion. Most connector
contacts are plated with either a noble finish, such as gold, or a
non-noble finish, generally tin. One of the main purposes of these
platings is to protect the base metal of the contact spring, usually
a copper alloy, from corrosion. The corrosion susceptibility of
noble and non-noble finishes is different and each will be discussed
separately.
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Loss in contact force,
leading to reduced mechanical stability and increased susceptibility
of the contact interface to fretting motions. The major mechanisms
leading to reduction in contact forces in connectors are
overstressing of contacts and stress relaxation. Stress relaxation
is a time-dependent loss in contact force, due to time/temperature
exposures.
Each of these degradation mechanisms will be discussed in more detail in
following articles.
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Dr. Robert S. Mroczkowski
Director Technology, Bishop and Associates Inc.
In 1998, Dr. Mroczkowski founded connNtext associates, a
firm providing consulting services in connector applications
to the electronics industry. Dr. Mroczkowski has over 30
years experience in various aspects of the electronics
industry. He joined AMP Inc. in 1971. While at AMP, his
responsibilities included consulting on connector design,
materials, and reliability concerns within AMP, and
providing an interface to AMP customers on the same issues.
In 1990 he joined the AMP Advanced Development Laboratories,
where he was responsible for the development of microstrip
cable connectors and a new microcoaxial connector for
medical ultrasound diagnostic equipment. Dr. Mroczkowski
retired in 1998 as an AMP principal. He is the author of the
McGraw Hill Electronics Connector Handbook, has
contributed chapters on connectors and interconnections to a
number of packaging handbooks, and written more than 20
technical papers. He holds seven patents. In 1997, Dr.
Mroczkowski received the Lifetime Achievement Award of the
International Institute of Connector and Interconnection
Technology.
He holds a bachelor’s, master’s, and doctorate of
science degrees in physical metallurgy from the
Massachusetts Institute of Technology.
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