Selecting High Temperature
and Cryogenic Aerospace Sensors
Accelerometers and pressure sensors
for measuring in extreme environments need special consideration
during the design and manufacturing process. Specialized applications
frequently require the use of a single sensor model, which must
be capable of operating over temperature ranges from -420 to
+1,200°F (-251 to +649°C), and of giving high accuracy,
stability, and reliability.
Typical applications for high-temperature aerospace sensors include
measuring gas turbine engines in-flight and in test cells, as
well as rocket motors and thruster assemblies. The same sensor
might be required to withstand radiation and be used to monitor
the vibrations inside a nuclear power plant or on a space vehicle,
or the cryogenic properties of liquid propellants. These environments
present many challenges.
Materials and construction must be optimized, not only to enhance
high-temperature performance, but also to allow operation in
the presence of gamma and neutron radiation without degradation.

Material selection
Piezoelectric sensors are made from both natural and ferroelectric
ceramic crystals. The choice of crystal depends on environmental
and performance requirements. Each material has unique features
and advantages, which characterize its performance in various
applications. Natural crystals tend to provide the highest temperature
ranges and the lowest pyroelectric outputs. However, ferroelectric
ceramics offer extended frequency ranges and smaller sizes for
equivalent charge outputs.
Single, natural crystals, such as quartz or tourmaline are inherently
piezoelectric. Most natural materials are single crystals grown
in laboratories rather than mined, which results in consistent
quality with a reduced risk of supply. In addition, the man-made
aspect of a natural crystal enables development of new, higher
performance variations.
Ferroelectric ceramic materials on the other hand are not inherently
piezoelectric. A ceramic is composed of many crystals in random
orientation. For the ceramic to become piezoelectric the dipoles
must be aligned. The alignment/ polarization process involves
applying a high voltage to the material to align polar-regions
within the ferroelectric ceramic element. This process is known
as poling.
Ferroelectric ceramics exhibit
higher sensitivity or charge output per imposed unit of force.
The most common material, bismuth titanate, has an output ten
times that of the most common high-temperature natural crystal,
tourmaline. Bismuth titanate can be used up to 950°F (510°C).
Various compounds may be added to the ceramic material to alter
sensor characteristics but high temperature ranges come at the
expense of sensitivity.
A natural single-crystal material can be employed in either shear
or compression mode. In compression mode, the material creates
an electric charge in the same direction as the applied force.
Lead zirconate titanate (PZT) is a ceramic material that is widely
used in temperature environments as high as 550°F (288°C).
In shear mode, the material creates a charge in the direction
perpendicular to the applied force. PZT can be designed into
sensors using both shear and compression mode, but is most efficient
in the shear mode since it has a higher charge output and upper
temperature range.
Typically, shear mode configurations are more efficient than
compression because there is greater bandwidth and higher output
with smaller size. In addition, since the required preload force
that holds the crystal in place is perpendicular to the polarization
axis, a shear design has extremely stable output over time. This
enables extensive design flexibility and performance optimization.
There are numerous temperatures, bandwidths, mounting, and other
trade-offs that must be considered in high-temperature applications.
Temperature effects exist beyond the limitation of the operating
environment. Temperature changes may produce extraneous outputs
and may change the sensitivity and other parameters. Piezoelectric
sensors cannot produce an output in response to a constant temperature
because they cannot produce an output in response to a constant
input: they are self-generating. They can, however, produce an
output in response to a change in temperature.
The piezoelectric
element itself is often pyroelectric; that is it generates an
output in response to temperature. In addition, temperature or
temperature gradients may change the preload stress on the element
because of thermal expansion. Temperature change inside a sensor,
where output would be affected is relatively slow due to the
thermal transfer. Therefore, thermal outputs are at low frequencies
where they are attenuated by the low frequency of the system.
For this reason, thermal output is not usually a problem. Sometimes
piezoelectric sensors can show sharp spikes in their output after
a large temperature change; this can be related to electrostatic
surface discharges in the pyroelectric fields. Spikes that continue
after a pyroelectric discharge can be related to both the piezoelectric
material and the design of the individual components and the
processing of the sensor.
A design that utilizes ferroelectric ceramics materials in compression
mode will have a greater pyroelectric output than that of a piezoelectric
shear design or one using a separate natural crystal.
This is because of two effects: in compression mode accelerometers,
piezoelectric material is directly coupled to the environment
through the base of the sensor. Also, the ferroelectric material
is sensitive to uniform temperature changes on those surfaces
perpendicular to the axis of polarization.
However, pyroelectric output is a very low frequency phenomenon
that is typically well below the frequency ranges of interest
and can be avoided by the use of high-pass filtering within measurement
system electronics.
Challenges
The maximum operating temperature of these sensors is controlled
by two design challenges: the first is a property of the piezoelectric
material known as the Curie temperature in piezoceramics, or
the twinning temperature in natural materials. This is the temperature
at which the material loses its piezoelectric properties.
The second design challenge is a sensor's insulation resistance,
which decreases rapidly with temperature. A low insulation resistance
charge amplifier and charge converters must be specifically designed
to operate with sensors having low insulation resistance values.
If the charge output is being measured, the frequency response
will not be affected, but the low frequency noise will tend to
increase. And some charge measuring equipment will not tolerate
low input resistance and will clip the output signal. Ordinarily,
the leakage resistance of a sensor is understood and the appropriate
signal conditioning is used so there will be no noticeable effects.
Whenever a sensor is exposed to temperature changes, other parameters
such as sensitivity and sensor capacitance also change. Changes
should be predictable and repeatable but every component and
process associated with building the sensor are influenced by
the crystal material. Manufacturers should test ever}' high-temperature
sensor at its maximum operating temperature to be sure of consistency
and quality.

Successful
measurements
Successful high-temperature measurements require more than just
good sensor design. Cabling and electrical connections are critical
to the acquisition of good quality data. A loose connector can
result in the generation of a high-level, low frequency signal
that is not related to the measurement. Over time, the reliability
of connectors can degrade at temperatures above 900°F (482°C)
due to oxide formation on the pin-to-socket contacts and potential
loss of pin retention. The result can show up as a roll-off in
the output of the sensor at higher frequencies.
Sensors designed for temperatures up to 1,200°F (649°C)
are therefore fitted with integral cables, which are mechanically
isolated from the seismic system to avoid base and cable strain
effects. Cables provided might use magnesium oxide or silicone
dioxide insulation. The latter is preferred since it is non-hydroscopic
and exhibits excellent high-temperature electrical characteristics.
Careful selection of the cable material and use of protective
over-braid facilitates handling and allows bend forming during
installation while maintaining cable integrity. The braid provides
flex to rigid cables and protects it from getting nicked or damaged.
Cables should not be bent under two-and-a-half times the diameter
of the cable as it may damage internal insulation or affect dielectric
properties. Cables on accelerometers should be clamped at approximately
8in (20 cm) intervals to prevent excessive flexing during vibration.
It's important to provide clearance between cables and other
components on the structure to prevent abrasion during vibration.
An accelerometer must be coupled with the surface it is measuring.
As a result, bending of the structure or mounting bracket can
cause distortion, producing unwanted output called base-strain
sensitivity. If brackets have to be used, care must be taken
to avoid introducing dynamic response problems due to bracket
resonances within or near the operational frequency range. A
thorough understanding of the modes of mounting brackets and
adaptors is important for good data and it must be verified that
engine resonance, bracket resonances, and sensor resonances do
not overlap.
Piezoelectric sensors will operate normally when subjected to
radiation-rich
environments.

Pyroelectric outputs will be produced when transient radiation
produces significant temperature changes, but this is no greater
than that produced within the standard temperature range. The
magnitude of pyroelectric output depends on the type of piezoelectric
ceramic used as well as the design. There should only be small
errors produced as a result of temperature changes present in
nuclear shock, with typical vibration applications resulting
from Gamma radiation. Neutron radiation could cause changes in
the molecular structure but only at extraordinary levels. Adverse
reactions to radiation include a reduction of piezoelectric material
output and the deterioration of various materials that are intolerant
to radiation such as Teflon. Generally, higher temperature crystals
are more resistant to the effects of radiation.
High-temperature sensor design is driven by their possible applications.
In test and measurement applications, single-ended designs are
used to minimize mass and size. Because of the wide array of
test and measurement environ-ments and associated conditions,
high-temperature sensors feature numerous mounting and cable/connector
configurations. With a singleended system, the accelerometer
has an inherent capacitance between the case and the signal side
of the crystal. It would normally be susceptible to electrostatic
pick-up without the use of an insulating base.
A general high-temperature category is used in permanently-mounted
monitoring applications. This type of accelerometer is often
referred to as a bill of material or OEM sensor because it is
integrated into a customer's product line. These accelerometers
are almost exclusively designed for each application. Unlike
their test and measurement counterparts, the housings for these
sensors are almost always electrically isolated from the measurement
circuit and the charge output of the sensor is differential.
Differential signal output is used where the capacitance balance
between signals is important because the structure on which it
is mounted is used as an electrical ground return. Capacitance
balance allows differential charge amplifiers to distinguish
between common mode signal (noise) and differential signal, which
is the true measure of dynamic acceleration. Differential output
is preferred when signals must be routed through multipin connectors
where the individual shielding of conductors is not feasible.
Whether they are used in aircraft engines, space vehicles, or
power generation stations, these sensors must provide high levels
of accuracy, stability, and reliability. Therefore, the instruments
used in extreme environments such as cryogens and high-temperature
sensors require special consideration during the design and manufacturing
process. I
Article
by Margie Mattingly