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General
Description
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Using
4-arm, 350-ohm bonded foil or 500-ohm bonded semiconductor bridges, these
tough stainless-steel load cells yield high accuracy and linearity in any
number of industrial and research applications, with exceptional
structural resistance to off-axis loading, side-loading, and other
extraneous forces (see Load Cell Side and
Bending Forces), and with safe overload protection for up to 50%
over capacity.
Daytronic
provides three basic types of general-purpose DC-excited strain gage load
cells:
Load
buttons and other load cell accessories
are also offered.
How
They Work
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Strain
Gages
The
resistance strain gage is an electrical sensing device that varies
its resistance as a linear function of the strain experienced by the
structural surface to which it is bonded. "Strain" is the
deformation of a solid material as the result of applied forces (internal
or external), and is normally expressed in units of microinches per
inch (or "microstrain").
A
typical strain gage consists of a conductive grid pattern of etched
metallic foil, mounted on a thin base of epoxy or fiberglass. It can
then be bonded to a surface in such a way that any subsequent deformation
of the surface produces a like deformation of the gages.
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Typical
Etched foil Gage Patterns |
When
the gage is deformed, its electrical resistance changes. This fact
is explained partly by simple geometry. That is, when a conductor is
stretched lengthwise, its cross-sectional area decreases, with a
consequent increases in resistance. It is also partly explained by
changes in the actual resistivity of the gage material when
subjected to strain.
For
a given amount of unit strain (ΔL/L), the gage will undergo a
corresponding change in resistance (ΔR/R). The ratio of the
unit change in resistance to the unit change in length is known as the gage
factor (Fg) of the gage:
Fg
= (ΔR/R) / (ΔL/L)
Conventional
foil gages have standardized nominal resistance values of 120 and 350
ohms, and typically exhibit gage factors between 1.5 and 3.5. In
typical transducer applications, they are subjected to full-scale design
strain levels ranging from 500 to 2000 microstrain.
Strain
Gage Transducers
In
transducers, strain gage configurations are employed to measure weight,
pressure, torque, and similar phenomena, by sensing the
deformation of calibrated beams, diaphragms, or other flexures to which mechanical
force is applied. Strain gage transducers can be rugged,
compact, linear, highly accurate, and readily compensated for wide
temperature ranges. They can be operated with many types of
available AC and DC instruments, are are widely used in industrial and
research measurement and control systems.
Through
proper flexure design and gage placement, a linear relationship can be
achieved between the applied force and the sensed strain. The Wheatstone
Bridge circuit shown below is almost universally used in load cells
and other strain gage transducers, because it facilitates cancellation of
unwanted temperature effects. (In any reliable load cell, thermal
expansion and temperature resistance effects must be made to cancel.
In particular, temperature effects on the modulus of elasticity of
the flexure materials must be compensated, using carefully trimmed
temperature-sensitive resistors (Rm in the figure)).

If
the gages within a load cell are connected in a balanced Wheatstone Bridge
circuit, and are excited by a source of AC or DC voltage, the transducer
will produce an electrical output which is a direct linear function of the
excitation voltage and the magnitude of the applied mechanical input:
Eout(mV)
= Ein(V) • K • F/100
where
K = Calibration Factor (mV/V, full scale)
F = Input variable (% of full scale)
Transducer
sensitivity is expressed in terms of millivolts per volt (mV/V).
The exact value of "K" for each instrument is determined by
measurement at the time of manufacture and is furnished as part of that
instrument's calibration data. For conventional transducers, this
value usually falls between 0.5 and 3.0.
Excitation
voltage can be either AC or DC, and is usually limited by heating
considerations to a maximum of 10 volts for 120-ohm bridges and 20 volts
for 350-ohm bridges (although good practice dictates somewhat lower
values).
Load
Cell Side and Bending Forces [Back
] |

Load
Cell Applications [Back
] |
For
many more load cell applications, see the Applications
pages for specific Daytronic instrument families.

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