Negative Temperature Coefficient Thermistors |
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Photo 1. NTC thermistors are manufactured in a variety of sizes and configurations. The chips in the center of the photo can be used as surface mount devices or attached to different types of insulated or uninsulated wire leads. The thermistor element is usually coated with a phenolic or epoxy material that provides protection from environmental conditions. For applications requiring sensing tip dimensions with part-to-part uniformity and/or smaller size, the devices can be encapsulated in PVC cups or polyimide tubes. |
NTC thermistors offer many desirable features for temperature measurement
and control within their operating temperature range. Although the word
thermistor is derived from THERMally sensitive resISTOR, the NTC thermistor
can be more accurately classified as a ceramic semiconductor. The most prevalent
types of thermistors are glass bead, disc, and chip configurations (see
Photo 1), and the following discussion focuses primarily on those technologies.
Temperature Ranges and Resistance Values. NTC thermistors exhibit a decrease
in electrical resistance with increasing temperature. Depending on the materials
and methods of fabrication, they are generally used in the temperature range
of -50°C to 150°C, and up to 300°C for some glass-encapsulated
units. The resistance value of a thermistor is typically referenced at 25°C
(abbreviated as R25). For most applications, the R25 values are between
100
and 100 k
. Other R25 values as low as 10
and as high as 40 M
can be produced, and resistance values at temperature points other than
25°C can be specified.
Accurate and Repeatable R/T Characteristic. The resistance vs. temperature
(R/T) characteristic (also known as R/T curve) of the NTC thermistor forms
the "scale" that allows its use as a temperature sensor. Although
this characteristic is a nonlinear, negative exponential function, several
interpolation equations are available that very accurately describe the
R/T curve [1,2,3]. The most well known is the Steinhart-Hart equation: 1/T
= A + B(lnR) + C(lnR)3
where: T = kelvin temperature R = resistance at temperature T
Coefficients A, B, and C are derived by calibrating at three temperature
points and then solving the three simultaneous equations. The uncertainty
associated with the use of the Steinhart-Hart equation is less than ±0.005°C
for 50°C temperature spans within the 0°C-260°C range,
so using the appropriate interpolation equation or lookup table in conjunction
with a microprocessor can eliminate the potential nonlinearity problem.
Sensitivity to Changes in Temperature. The
NTC thermistor's relatively large change in resistance vs. temperature,
typically on the order of -3%/°C to -6%/°C, provides an
order of magnitude greater sensitivity or signal response than other temperature
sensors such as thermocouples and RTDs. On the other hand, the less sensitive thermocouples and RTDs are a good choice for applications requiring temperature spans >260°C and/or operating temperatures beyond the limits for thermistors.
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| Figure 1. Over the range of -50°C to 150°C, NTC thermistors offer a distinct advantage in sensitivity to temperature changes compared to other temperature sensors. This graph illustrates the R/T characteristics of some typical NTC thermistors and a platinum RTD. |
Another important feature of the NTC thermistor is the degree of interchangeability
that can be offered at a relatively low cost, particularly for disc and
chip devices. Interchangeability describes the degree of accuracy or tolerance
to which a thermistor is specified and produced, and is normally expressed
as a temperature tolerance over a temperature range. For example, disc and
chip thermistors are commonly specified to tolerances of ±0.1°C
and ±0.2°C over the temperature ranges of 0°C to 70°C
and 0°C to 100°C. Interchangeability helps the systems manufacturer
or thermistor user reduce labor costs by not having to calibrate each instrument/system
with each thermistor during fabrication or while being used in the field.
A health care professional, for instance, can use a thermistor temperature
probe on one patient, discard it, and connect a new probe of the same specifications
for use on another patient--without recalibration. The same holds true for
other applications requiring reusable probes.
The small dimensions of most bead, disc, and chip thermistors used for
resistance thermometry make for a very rapid response to temperature changes.
This feature is particularly useful for temperature monitoring and control
systems requiring quick feedback.
Thermistors are well suited for sensing temperature at remote locations
via long, two-wire cable because the resistance of the long wires is insignificant
compared to the relatively high resistance of the thermistor.
As a result of improvements in technology, NTC bead, disc, and chip thermistor
configurations are typically more rugged and better able to handle mechanical
and thermal shock and vibration than other temperature sensors.
Most NTC thermistors are made from various compositions of the metal
oxides of manganese, nickel, cobalt, copper, and/or iron. A thermistor's
R/T characteristic and R25 value are determined by the particular formulation
of oxides. Over the past 10 years, better raw materials and advances in
ceramics processing technology have contributed to overall improvements
in the reliability, interchangeability, and cost-effectiveness of thermistors.
Of the thermistors shown in Figure 2, beads,
discs, and chips are the most widely used for precise temperature measurements.
Although each configuration is produced by a unique method, some general
ceramics processing techniques apply to most thermistors: formulation and
preparation of the metal oxide powders; milling and blending with a binder;
forming into a "green" body; heat-treating to produce a ceramic
material; addition of electrical contacts (for discs and chips); and, for
discrete components, assembly into a usable device with wire leads and a
protective coating.
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| Figure 2. A variety of manufacturing processes are used to make NTC thermistors configured as beads (A), chips (B), discs (C), rods (D), and washers (E). |
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Historical Note on the Thermistor
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Bead thermistors, which have lead wires that are embedded in the ceramic
material, are made by combining the metal oxide powders with a suitable
binder to form a slurry. A small amount of slurry is applied to a pair of
platinum alloy wires held parallel in a fixture. Several beads can be spaced
evenly along the wires, depending on wire length. After the beads have been
dried, the strand is fired in a furnace at 1100°C-1400°C to
initiate sintering. During sintering, the ceramic body becomes denser as
the metal oxide particles bond together and shrink down around the platinum
alloy leads to form an intimate physical and electrical bond. After sintering,
the wires are cut to create individual devices. A glass coating is applied
to provide strain relief to the lead-ceramic interface and to give the
device a protective hermetic seal for long-term stability. Typical glass
bead thermistors range from 0.01 in. to 0.06 in. (0.25 mm to 1.5 mm) in
dia.
Disc thermistors are made by preparing the various metal oxide powders,
blending them with a suitable binder, and then compressing small amounts
of the mixture in a die under several tons of pressure. The discs are then
fired at high temperatures to form solid ceramic bodies. A thick film electrode
material, typically silver, is applied to the opposite sides of the disc
to provide the contacts for the attachment of lead wires. A coating of epoxy,
phenolic, or glass is applied to each device to provide protection from
mechanical and environmental stresses. Typical uncoated disc sizes range
from 0.05 in. to 0.10 in. (1.3 mm to 2.5 mm) in dia.; coated disc thermistors
generally measure 0.10 in. to 0.15 in. (2.5 mm to 3.8 mm) in dia.
Chip thermistors are manufactured by tape casting, a more recent technique
borrowed from the ceramic chip capacitor and ceramic substrate industries.
An oxide-binder slurry similar to that used in making bead thermistors is
poured into a fixture that allows a very tightly controlled thickness of
material to be cast onto a belt or movable carrier. The cast material is
allowed to dry into a flexible ceramic tape, which is cut into smaller sections
and sintered at high temperatures into wafers 0.01 in. to 0.03 in. (0.25
mm to 0.80 mm) thick. After a thick film electrode material is applied,
the wafers are diced into chips. The chips can be used as surface mount
devices or made into discrete units by attaching leads and applying a protective
coating of epoxy, phenolic, or glass. Typical chip sizes range from 0.04
in. by 0.04 in. (1 mm by 1 mm) to 0.10 in. by 0.10 in. (2.5 mm by 2.5 mm)
in square or rectangular shapes. Coated chip thermistors commonly measure
from 0.08 in. to 0.10 in. (2.0 mm to 2.5 mm) in diameter. Very small coated
chip thermistors 0.02 in. to 0.06 in. (0.5 mm to 1.5 mm) in dia. are available
for applications requiring small size, fast response, tight tolerance, and
interchangeability.
Washer-shaped thermistors are essentially a variation of the disc type
except for having a hole in the middle, and are usually leadless for use
as surface mount devices or as part of an assembly. Rod-shaped thermistors
are made by extruding a viscous oxide-binder mixture through a die, heat-treating
it to form a ceramic material, applying electrodes, and attaching leads.
Rod thermistors are used primarily for applications requiring very high
resistance and/or high power dissipation.
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Photo 2. NTC thermistors can be attached to extension leads or jacketed cable and assembled into various types of housings. The optimum materials, dimensions, and configuration for a probe assembly are determined by careful review of the application requirements. |
One of the problems the thermistor industry has faced over the years
is that some manufacturers have claimed their particular style or configuration
of thermistor is better than other configurations made by their competitors,
without regard to other, more pertinent factors. These thermistor "politics,"
more harmful than beneficial to the industry, can confuse engineers and
purchasing agents who are looking for reliable information to help them
choose the appropriate product for their application. Although some thermistor
qualities or capabilities, including interchangeability, repeatability,
size, responsiveness, and stability, can either be enhanced or limited by
style or geometry, these characteristics are much more dependent on a manufacturer's
ability to understand the ceramics technology being used and to maintain
control of the manufacturing process.
Glass-coated beads feature excellent long-term stability and reliability
for operation at temperatures up to 300°C. Studies at the National
Institute of Standards and Technology (NIST) and other laboratories indicate
that some special bead-in-glass probes have measurement uncertainties and
stabilities (better than ± 0.003°C for temperatures between
0°C and 100°C) that approach those of some standard platinum resistance thermometers [3,4,5]. The relatively small size of glass bead thermistors gives them a quick response to temperature changes, but for some applications this small size can make the devices hard to handle during assembly and have the effect of limiting their power dissipation. It is also more difficult and more expensive to produce glass beads with close tolerances and interchangeability.
Individual calibration and R/T characterization, resistor network padding,
or use of matched pairs are among the methods used to achieve interchangeability.
Chip and disc thermistors are noted for their tight tolerances and interchangeability
at a relatively low cost compared to bead thermistors. These qualities are
inherent in the manufacturing processes. The thermistors' larger size permits
power dissipation higher than that of beads, although at some expense of
response times. Larger size can be a disadvantage in some applications.
Because of their geometry, disc thermistors normally have larger coated
diameters and higher power dissipation capabilities than chip thermistors.
On the other hand, chip thermistors typically can be produced to smaller
coated diameters and are better suited for applications requiring smaller
size and faster response times. More recent designs of chip thermistors
allow the production of sizes and response times approaching those of glass
beads. In some cases, chip and disc thermistors with equivalent physical
and electrical characteristics can be used in the same applications without
any noticeable difference in performance.
Thermistors, thermocouples, RTDs, and other sensors and electronic components
exhibit a phenomenon called drift, a gradual, predictable change in certain
properties over time. For a thermistor, drift results in a change in resistance
from its initial value, typically after being continuously exposed to or
cycled to an elevated temperature. Thermistor drift is expressed as a percent
change in resistance and/or as a change in temperature that occurs at a
given exposure temperature for a certain length of time. As the exposure
temperature increases, so do the drift and the drift rate [4,5,6].
Chip and disc thermistors with soldered leads and an epoxy or phenolic
coating have potential limitations in their maximum operating temperatures,
typically 150° C for short-term exposures (1-24 hours) and 105°C
for long-term exposures (1-12 months). When subjected to environmental
conditions above their recommended maximum operating temperatures, epoxy-
or phenolic-coated chips and discs can begin to exhibit an undesirable,
excessive amount of drift. When such thermistors are used at temperatures
below the specified maximum operating temperatures, drift is minimal, on
the order of 0.02°C to 0.15°C after 12 months of continuous exposure
to temperatures between 25°C and 100°C, respectively. Recent advances
in the techniques used to manufacture chip and disc thermistors with a glass
coating have produced devices that combine the interchangeability advantage
of chips and discs with the stability of glass beads [5,6]. For applications
that require operating temperatures up to 200°C, these new devices
offer a lower cost alternative to the conventional glass bead thermistors.
These comparisons can help determine whether a thermistor supplier is
objectively evaluating an application in terms of the appropriate thermistor,
or simply promoting the configuration it manufactures. For an example of
the latter approach, see [7], where a manufacturer of disc thermistors stated
that "Loose-tolerance thermistors are usually mass-produced by tape
casting," and that "These devices . . . are designed for applications
requiring neither interchangeability nor a high degree of accuracy,"
implying that all chip thermistors are loose tolerance. On the contrary,
millions of precision chip thermistors with superior long-term stability
are produced annually to an interchangeable tolerance of ±0.1°C,
and they are available with an interchangeability of ±0.05°C.
In reality, broad-tolerance and tight-tolerance thermistors are available
in each of the three major thermistor configurations discussed above.
After determining the appropriate specifications, the engineer and purchasing
agent need to evaluate which configuration and supplier will best meet the
requirements for process control, quality, on-time delivery, and value at
a reasonable price. An important part of the evaluation process is to perform
some basic tests on the design and quality of the thermistor and, wherever
possible, include simulation of the actual environmental conditions of the
intended application. To achieve optimum performance, thermistors are usually
mounted into protective housings or probe assemblies (see Photo 2). For additional information on sensor assembly design, see [8]. An informed
decision can then be made as to which product and supplier will provide
the best value for the application requirement. Part II of this article
will examine the ways to perform these tests.
The full five-part article on Negative Temperature Coefficient
Thermistors can be found at the Sensors Magazine web site..
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References 1. J.S. Steinhart and S.R. Hart. 1968. "Calibration Curves for Thermistors," Deep Sea Research 15:497. 2. M. Sapoff et al. 1982. "The Exactness of Fit of Resistance-Temperature Data of Thermistors with Third-Degree Polynomials," Temperature, Its Measurement and Control in Science and Industry, Vol. 5, James F. Schooley, ed., American Institute of Physics, New York, NY:875. 3. W.R. Siwek et al. 1992. "A Precision Temperature Standard Based on the Exactness of Fit of Thermistor Resistance-Temperature Data Using Third Degree Polynomials," Temperature, Its Measurement and Control in Science and Industry, Vol. 6, James F. Schooley, ed., American Institute of Physics, New York, NY:491. 4. S.D. Wood et al. 1978. "An Investigation of the Stability of Thermistors," J Res of the Nat Bur of Stds:83, 247. 5. W.R. Siwek et al. 1992. "Stability of NTC Thermistors," Temperature, Its Measurements and Control in Science and Industry, Vol. 6, James F. Schooley, ed., American Institute of Physics, New York, NY:497. 6. J.A. Wise. 1992. "Stability of Glass-Encapsulated Disc-Type Thermistors," Temperature, Its Measurement and Control in Science and Industry, Vol. 6, James F. Schooley, ed., American Institute of Physics, New York, NY:481. 7. C. Faller and F. Arment. Jun. 1996. "NTC Thermistor Update," Sensors:22. 8. D. McGillicuddy. Dec. 1993. "NTC Thermistor Basics and Principles of Operation," Sensors:42. 9. D. Hill and H. Tuller. 1991. "Ceramic Sensors: Theory and Practice," Ceramic Materials for Electronics, R. Buchanan, ed., Marcel Dekker, Inc., New York, NY:272. 10. U.S. Patent No. 2,258,646, 14 Oct. 1941. 11. R.L. Winter, former chairman and CEO, Western Thermistor Corp., private communication. Jul. 1996. |
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