Resistance Temperature Detectors: Back to Basics
14 October 2011
Chris Chant, Business Development Manager at Okazaki Manufacturing Company (OMC), discusses the basic principles of a resistance temperature detector (RTD) and the technical advantages they offer in industrial applications.
Resistance Temperature Detectors or Resistive Thermal Devices (RTDs) are wire wound and thin film devices that incorporate pure metals or certain alloys that increase in resistance as the temperature increases, and conversely, decrease in resistance as the temperature decreases.
RTDs are similar to thermocouples in that they convert changes in temperature to voltage signals by the measurement of resistance. As an RTD becomes hotter, the resistance measured on its element becomes larger. As the RTD cools, the resistance becomes smaller.
The Platinum Element RTD
The most commonly used type of RTD element is Platinum. These versions are often referred to as PRTs or PRT100s. Platinum elements are popular because they can be used over a wide range of temperatures and also provide fast response times. Platinum’s coefficient of resistance is almost linear, which means that by using a platinum element, resolutions of +/- 0.1 deg C or better are possible.
PRTs are gradually replacing the use of thermocouples in many industrial applications below 600 deg C, due to their higher accuracy and repeatability.
The current international standard which specifies tolerance, and the temperature-to-electrical resistance relationship for platinum resistance thermometers is IEC 60751:2008. By far the most common devices used in industry have a nominal resistance of 100 ohms at 0 deg C, and are called Pt100 sensors ('Pt' is the symbol for platinum). The sensitivity of a standard 100 ohm sensor is a nominal 0.385 ohm/°C. RTDs with a sensitivity of 0.375 and 0.392 ohm/°C as well as a variety of others are also available.
Other more cost effective elements can be used in RTDs. The most common of these alternatives are copper and nickel. The advantage here is that the RTD will have a reduced manufacturing cost and will have a lower replacement value. However, the drawback is that these elements have more restrictions on the range over which they can be used due to non-linearities in the Resistance versus Voltage curve. Also, problems of wire oxidation are known to occur when copper is used as the element.
Why choose an RTD?
One of the technical advantages of using an RTD is that it provides a very stable output for long period of time. Other benefits include ease of recalibration and accuracy of readings over a relatively narrow temperature range. When compared to thermocouples, the disadvantages of using RTDs are: higher sensitivity to vibration, smaller overall temperature range, and a greater initial cost.
Prolonging Life and Eliminating Measurement Errors
To achieve the maximum life from a Resistance Temperature Detector, it is recommended that a protective well and terminal head be used. The well serves to protect the RTD from damage by the gas or liquid being measured. Protecting wells are typically manufactured in stainless steel, carbon steel, Inconel or cast iron. The wells are designed to operate in temperatures up to 1,100 deg C.
To eliminate measurement errors, it is necessary to compensate for the length of lead wire used to connect the RTD to the readout. The calculations to correct this are relatively straightforward. Three-wire and four-wire designs are also available that help to minimise these types of errors.
Laboratory Accuracy with Industrial Ruggedness
Platinum resistance temperature detectors are used for interpolation between the IPTS-68 fixed temperature points of ice and antimony (0 deg C to 630.74 deg C). They are generally used where accuracy and stability are most important. OMC’s approach to RTDs will bring +/- 0.05 degrees laboratory accuracy to the toughest industrial processes – without any special handling considerations.
OMC has combined the inherent accuracy of a precisely wound Platinum resistance element with AeroPak® compacted ceramic insulated cable. The result is a low cost yet rugged sensor that will withstand factory handling, whilst retaining the stability required for today’s precision process control environments.
Time response characteristics
The response of an OMC Resistance Temperature Detector is defined by two noticeable characteristics when exposed to an instantaneous (step) change in environment temperature. These are:
(a) Time Constant: The time to reach 63.2% of the complete step change in temperature.
(b) Response Time: Time to reach within 0.5% of the final temperature in a step change. This is approximately equal to 5 times the time constant.
The response of a temperature sensor to a step change in environment temperature tends to follow a second order differential equation. However, this is approximate, since if the mass of the sensor is small in relation to the mass of the fluid passing over it (as is the case with a liquid), the response may approach a first order differential equation.
Completed probes can be matched in pairs to the nearest 0.01 ohm at 0 deg C for differential temperature measurements to 0.05 deg C.
Completed probes can be supplied with selected ice point resistances within a narrow band to eliminate the need for compensation in indicating circuits.
In the last few months, OMC has completed the development of a brand new high temperature platinum resistance thermometer for industrial applications. The new Ceracoil W86 is able to measure very high temperatures of up to 660 deg C using a platinum RTD element.
For more information on OMC’s range of RTDs and thermowells, please visit the website at www.okazaki-mfg.co.uk or contact the sales department on 02920 814330 or email: email@example.com