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Noise Control in Strain Gage
Measurements
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Electrostatic Noise
Reduction
Shielding
The simplest and most effective barrier against
electrostatic noise pickup is a conductive shield,
sometimes referred to as a Faraday cage. It functions
by capturing the charges that would otherwise reach
the signal wiring. Once collected, these charges must
be drained off to a satisfactory ground (or reference
potential). If not provided with a low-resistance
drainage path, the charges can be coupled into the
signal conductors through the shield-to-cable
capacitance (Fig. 501.3).
Fig. 501.3 - Electrostatic shielding.
The two most popular types of cable shields are
braided wire and conductive foil. The braided-shield
construction provides about 95 percent coverage of
the cable, and is characteristically low in
resistance. Although commonly higher in resistance,
foil shields give 100 percent cable coverage, and are
also easier to terminate. Following are commercially
available examples of the two types of shielded
cable:
When long reaches of multiple conductors are run
adjacent to each other, problems with crosstalk
between conductors can be encountered. With runs of
50 feet (15 m) or more, significant levels of noise
can be induced into sensitive conductors through both
magnetic and electrostatic coupling. Even though
bridge-excitation conductors may carry only a
millivolt of noise, there can be significant coupling
to signal conductors to produce potentially
troublesome microvolt-level noise in those
conductors. The noise transfer can be minimized by
employing an instrumentation cable composed of
individually shielded pairs - one pair for
excitation, and one pair for the signal. This type of
construction is embodied in Micro-Measurements Type
422-DSV cable. When using such cable (those having
separate shields), both shields should be grounded at
the instrument end of the cable. Electromagnetic
coupling between excitation and signal pairs can be
reduced somewhat by using a cable that has its
conductor pairs twisted on separate axes. Belden No.
8730 cable has the conductor pairs separately
twisted, including one pair shielded with foil.
The shield-to-conductor capacitance can also become
significant for long runs, since the capacitance is
proportional to the cable length. Therefore, a
significant portion of the residual noise can be
coupled from even a well-grounded shield to the
sensitive conductors. To minimize this effect, some
strain gage instruments (for example, Vishay
Measurements Group Instruments Division's
2300 System
) incorporate a feature called a driven guard. A
driven guard (also known as a driven shield)
functions by maintaining the shield at a voltage
equal to the average signal, or common-mode voltage.
Since, with this arrangement, the voltage difference
between the conductors and shield is essentially
zero, the effective capacitance is decreased, and
there is minimal noise transfer. The result is a very
quiet shield. It is important to note that, for
proper operation, the driven shield is connected at
only one end to the driven-guard pin on the
instrument input connector. The driven shield is
ordinarily surrounded by a second shield, which
should be grounded at one end.
In a fully guarded amplifier system (for example,
Vishay Measurements Group Instruments Division's
Model
2200 System
), the common-mode voltage of the bridge excitation
supply and the signal input terminals
"float" to the level on the guard shield.
Connecting the shield to the test structure or source
of common-mode voltage at the gage installation site
can provide very effective noise reduction since the
voltage between signal conductors and the shield is
minimized.
Leakage to Ground
Another often-overlooked source of noise is
leakage-to-ground through the strain gage and/or the
cabling. If excessive, this leakage can cause noise
transfer from the specimen to the gage circuit, since
even supposedly well-grounded specimens may carry
some noise. It is not uncommon to have strain gages
installed on nominally grounded test objects which,
in fact, have noise levels expressible in volts. And,
of course, any strain gage installation on a
conductive specimen forms a classic capacitor which
can couple noise from the specimen to the gage. In
light of these considerations, it is always a good
practice to make certain that the specimen is
properly grounded and that leakage between the gage
circuit and the specimen is well within bounds.
Prior to connecting leadwires to the strain gage,
the insulation resistance from the gage to the
specimen should be measured with a megohm meter such
as the Instruments Division's
Model 1300 Gage
Installation Tester
. A reading of 10 000 megohms is normally
considered a minimum for satisfactory system
operation. Readings below this level are indicative
of a possibly troublesome gage installation which can
deteriorate with time and strain. It should also be
kept in mind, for gage installations which will
operate at elevated temperatures, that leakage
resistance tends to decrease as the temperature
increases.
After cable placement and connection at the gage-end
of the cable, the following resistance measurements
should be made, preferably from the instrument-end of
the cable: conductor-to-ground, shield-to-ground, and
conductor-to-shield. Because of distributed leakage,
these resistances may be somewhat lower than the
gage-to-specimen resistance; but cables with
significantly lower resistances should be
investigated, and the excessive leakage eliminated to
avoid potential noise problems.
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