
Keywords: dataacquisition systems (DAS), precision deltasigma ADCs, highresolution thermocouples
Related Parts


HighPerformance Temperature Measurement Using Thermocouples and Precision DeltaSigma ADCs, Part 2
By: 
Joseph Shtargot, Strategic Applications Engineer 

Mohammad Qazi, Applications Engineer 

Abstract: Many industrial and medical applications require temperature measurements with accuracies of ±1°C or better, performed with reasonable cost over a wide range of temperatures (270°C to +1750°C) and often with low power consumption. This article describes design of the costefficient, portable, highresolution dataacquisition systems (DAS) based on precision deltasigma analogtodigital converters (ADCs). It also presents formulas and software for implementation of standardized linearization calculation algorithms to accurately cover this wide temperature range while ensuring reproducible measurements.
A similar version of this article appears on
EDN, October 18, 2013.
Introduction
This twopart series presents the design of a costeffective, portable, highresolution dataacquisition system (DAS) based on a precision deltasigma analogtodigital converter (ADC). The
Part 1 article reviewed the history of thermocouple technology and the principal of the operation. It described a thermocouple interface with the
MAX11200 ADC evaluation (EV) kit.
^{1}
This Part 2 of the series presents a dedicated reference design (RD) in which the MAX11200 ADC interfaces with a thermocouple and platinum resistance temperature detector (PRTD) using a simple multiplexor. No additional instrumentation amplifiers, lownoise references, and optical isolation are needed for precise temperature measurement. The new RD is cost effective, compact, and low power. We also describe the highresolution thermocouple’s DAS and the software required to achieve accuracies of ±1°C, or better, using standardized linearization calculation algorithms.
Thermocouple Calculation Overview
In Part 1 of this series^{2} we explained that thermocouples generate a voltage/charge (V_{OUT}) and do not require any voltage or current excitation. Readers familiar with the technology can jump to the next section.
V_{OUT} is the function of the temperature differential,  (T_{JUNC}  T_{COLD}), produced by two dissimilar metals. The differential is due to the different electric potentials for the Metal 1 and Metal 2 and the temperature gradient applied to them.^{3} The NIST ITS90 Thermocouple Database^{4} defines this V_{OUT} function for most practical Metal 1 and Metal 2 combinations and enables the calculation of relative temperature T_{JUNC} based on the V_{OUT} measurements. It is important to emphasize that T_{JUNC} is only a relative temperature in relation to the cold junction (T_{COLD}). To find the absolute temperature (in °C, °F, or K), T_{COLD} temperature must be independently measured:
Tabs = T_{JUNC} + T_{COLD} 
(Eq. 1) 
where:
Tabs is the absolute temperature of the hot junction;
T_{JUNC} is the relative temperature of the hot junction versus the cold reference junction;
T_{COLD} is the absolute temperature of the reference cold junction.
Note that the T_{JUNC} and T_{COLD} temperature measurements must be produced in the same units (i.e., in °C, °F, or K).
Equation 1 dictates that the thermocouple measurement requires V_{OUT} precision measurements for the hot junction, as well as an accurate complimentary sensor^{5} for the coldjunction temperature measurements.
Accuracy and Resolution
Thermocouple temperature calculation can be done using simplified linearization algorithms. The approximate absolute temperature is calculated as:
Tabs = (E + Ecj)/k 
(Eq. 2) 
where:
E is the measured thermocouple output in mV;
Tabs are the absolute temperature of the thermocouples in °C;
Ecj is the coldjunction thermocouple equivalent output in mV, calculated by using the cold junction temperature, measured independently, and the ITS90 Thermocouple Database tables;
k is the thermocouple average sensitivity.
While a linearization approach could substantially reduce the calculation volume and complexity, it can also produce large temperaturemeasurement errors. For example, in a Ktype thermocouple linear approximation by Equation 2 allows only a 1°C to 4°C degree of precision in the narrower 50°C to +350°C temperature range. At +1000°C the calculation errors could reach around 7°C, while at 100°C the error would be around 13°C. (See Table 2.) The root cause of the large errors can be traced to nonlinearity, as shown in Figure 1.
Figure 1. Ktype thermocouple nonlinearity. The data show the output voltage vs. temperature for a Ktype thermocouple. The curve is reasonably linear in the range of 50°C to +350°C, and it clearly has significant deviations from absolute linearity at the “ends,” below 50°C and above +350°C.^{6}
Output voltages from the most common thermocouples,^{7, 8} as a function of temperature, are highly nonlinear. This nonlinearity can produce large errors in the extended temperature ranges as shown in the Ktype thermocouple example in Figure 1.
Errors in the extended temperature ranges are also common for applicationspecific ICs (ASICs) like the
MAX31855 thermocoupletodigital converter. For example, if an extended 270°C to +1372°C temperature range is needed for Ktype thermocouples, then the MAX31855 thermocouple’s overall accuracy will be ±6°C. A similar situation exists for other popular thermocouples.
Consequently, Figure 1 and Equation 2 demonstrate that rather complex nonlinear compensation is needed to further improve the accuracy of a popular industrial thermocouple.
Improving the Accuracy
We return now to the NIST ITS90 database cited above. Substantial accuracy improvement (in the order of magnitude versus linearization algorithms) can be achieved with the modern NIST ITS90 Thermocouple Database, which allows the polynomial equation to be used to convert thermocouple voltage to temperature (°C) over a wide temperature range using standardized polynomial coefficients.^{9} New contemporary NIST ITS90 coefficients are provided for the temperature intervals (versus single intervals in the previous standards), and they allow temperatures to be calculated with good accuracy (around ±0.1°C)—more than sufficient for most industrial applications.
Improving Resolution
The MAX11200 used in this RD is a lowpower, 24bit, deltasigma ADC. It has an extremely low inputreferred RMS noise of 570nV at 10sps. The noisefree resolution (NFR) is around 6.6 × RMS noise and represents a value of 3.762µV. (This is called flickerfree code.) The NFR represents the minimum values that can be reliably differentiated by the ADC in voltage in the measurement range.
Table 1 provides more precise NFR resolution values than in Part 1 of this series^{10} where the assumption was that NFR = V_{REF}/2^{20}. Therefore, a detailed calculation for a 0°C to 500°C range is:
Noise free codes = V_{INT}/Input referred noise
Noise free codes = 20.644mV/3.762µV_{PP}
Noise free codes = 5487.5 codes
Temp (resolution) = 500°C/5487.5
Temp (resolution) = 0.0911°C
Table 1 provides the calculated values of °C/NFR error for three temperature ranges. For all the temperature ranges the NFR values are below 0.15°C, which is better than for ASICs and more than sufficient for most thermocouples in industrial and medical applications.
Table 1. °C/NFR Error for Defined Temp Ranges 
Temperature Range (°C) 
200 to 0 
0 to 500 
500 to 1372 
Voltage Range (V_{INT}, mV) 
5.891 
20.644 
34.242 
Resolution (°C/NFR) 
0.1277 
0.0911 
0.0871 
Electronic Design
Interfacing a Thermocouple with the MAX11200based DAS Board
Part 1 of this article described the thermocouple interface with the MAX11200 EV kit. That design produces very good results, but includes many components, optical isolation, and features intended for general applications. Figure 2 shows a simplified schematic for the MAX11200based DAS board, here optimized for costeffective portable thermocouple measurements applications. Included on board is the PRTD.^{11}
High resolution is achieved by using the MAX11200 fully differential capability. A ratiometric approach utilizes the ADC’s excellent commonmode rejection (100dB or better) and, therefore, allows the design to achieve a desirable signaltonoise ratio (SNR) without optical isolation and dedicated reference.
Figure 2. Block diagram of the MAX11200 DASbased temperature measurement system. Design allows dynamic measurement of either the thermocouple or PRTD.
In Figure 2 the MAX11200’s GPIO is set to control the precision multiplexer, the
MAX4782, which selects either the thermocouple or the PRTD. This approach allows dynamic measurement of either the thermocouple or PRTD using a single MAX11200; it improves system precision and reduces the requirements for calibration. The PRTD is a PT1000 (PTS 1206, 1000Ω) used for temperature measurement of the cold junction. The
MAX8511 precision LDO powers the system and provides a reference voltage for the MAX11200.
The Algorithms
The algorithms selected for this design are similar to those presented in Part 1 of this article and can be used for any type of the thermocouple. The NIST ITS90 provides different sets of the coefficients for specific temperature intervals: 200°C to 0°C, 0°C to +500°C, and +500°C to +1372°CKtype thermocouples. Each temperature interval must be preselected for use in Equation 3.
T = d_{0} + d_{1} × E^{1} + d_{2} × E^{2} + ... d_{N} × E^{N} 
(Eq. 3) 
where:
T is the temperature in °C;
E is the V_{OUT} thermocouple output in mV;
dN is the polynomial coefficients unique to each thermocouple;
N is the maximum order of the polynomial.
The simplified linearization algorithm in equation 3 allows the designer to select temperature intervals based on Table 1 with sufficient accuracy.
Processing the Data
The firmware in the
MAXQ622 microcontroller (Figure 2) provides datareading capability to the software through USB. The software implements algorithms based on Equations 2 and 3. Raw measurement data is processed inside the PC. The software manages the following major functions which are charted in
Figure 3:
 Initializes the MAX11200 ADC
 Collects and processes the ADC's output data
 Calculates the temperature using Equations 2 and 3
During initialization, the MAX11200 ADC goes through the selfcalibration process, enables the input signal buffers, and disables both system gain calibration and system offset calibration. This DAS allows reasonably fast data acquisition with excellent (100dB or better) normalmode powerline 50Hz/60Hz rejection. Selection of the sample rates is very important for reducing noise and interference in the industrial measurements.
The recommended external clock for 60Hz linefrequency rejection is 2.4576MHz, which is effective for data rates of 1, 2, 5, 10, and 15sps. For 50Hz linefrequency rejection, the recommended external clock is 2.048MHz, which is effective for data rates of 0.83, 2.08, 4.17, 8.33, and 12.5sps.
Input signal buffers increase the input impedance to the high megohms range. This improves measurement precision because it practically eliminates the shunting effect of the input dynamic current.
Figure 3. Chart outlines the toplevel actions of the DAS firmware and software.
Design Implementation
Figure 4 shows the implementation of the costeffective, compact highresolution DAS shown in Figure 2. The DAS was designed and tested with the popular Ktype OMEGA^{®} thermocouple KTSS116^{12} and verified with the Fluke^{®} 724 temperature calibrator. The DAS board dimensions are only 2in × 1.5in and overall Bill of the Materials cost is below $10 (U.S.), depending on the quantity. The current design is powered through a laptop USB port. The batterybased power consumption could be reduced to below around 3mA by reducing the clock frequency and removing the status LEDs.
Figure 4. The setup for the temperature measurement system featuring the MAX11200 ADC.
A Fluke 724 temperature calibrator supplies precision voltage that corresponds to the Ktype thermocouple’s output in the 200°C to +1300°C range to the MAX4782 X1 and Y1 inputs. An onboard PT1000based circuit connected to the MAX4782 X0 and Y0 inputs provides the cold junction compensation module.
The software collects and processes data generated by thermocouple and PT1000 outputs. The MAX11200’s GPIOs allow dynamic control of the MAX4782 for selecting either the thermocouple or the PRTD. The MAXQ622 microcontroller manages the MAX11200 measurement and transmits data though a USB port to the laptop computer.
The laptop display (Figure 3) shows a traditional analog thermometer with fullscale approximate measurements, as well as a precise digital thermometer reflecting final temperature calculations (in °C or °F).
Table 2 lists measurements and calculations using Equations 2 and 3 for the 200°C to +1300°C temperature range.
Table 2. Measurements for the 200°C to +1300°C Temperature Range 
Temperature—Fluke 724 (°C) 
Temperature—Thermocouple GUI (°C) 
Temperature Error vs. Calibrator (°C) 
Temperature Calculated by Linear Equation (°C) 
200 
200.2 
0.2 
143.6 
100 
100.4 
0.4 
86.62 
50 
50.4 
0.4 
46.01 
0 
0.3 
0.3 
0.05 
20 
19.7 
0.3 
19.68 
100 
99.7 
0.3 
99.96 
200 
199.8 
0.2 
198.69 
500 
499.9 
0.1 
503.7 
1000 
1000.4 
0.4 
1006.92 
1300 
1300.9 
0.9 
1278.4 
Table 2 shows that with use of Equation 2, the MAX11200based DAS achieves precise temperature measurement in the order of ±0.5°C over a very wide temperature range with about 0.9°C accuracy at +1300°C. Linear approximation by Equation 2 allows the selection of temperature intervals quickly and efficiently. Using Equation 2 required relatively complex calculations with polynomial calculation algorithms. Modern processors like MAXQ622, in conjunction with portable personal computers, process complex calculations efficiently and in a costeffective manner.
Detailed schematics, a bill of materials (BOM), and application software for this design are available to all qualified customers .
Conclusion
In recent years we have seen the development of costeffective, thermocouplebased temperaturesensing measurement across very wide temperature ranges. In fact, a range of 270°C to +1750°C is quite doable at a reasonable cost and often with very low power consumption.
In this RD, the MAX11200 lowpower ADC interfaces with a thermocouple and PRTD using a simple multiplexor. No additional instrumentation amplifiers, low noise references, and optical isolation are needed. Using a microcontroller and standard personal computer, the MAX11200based DAS achieves precision on the order of ±0.5° from 200°C to +1000°C. This temperaturemeasurement RD offers high performance, yet it is compact and cost effective. It is ideal for portable sensing applications and compares favorably with more precise, but more expensive and complex designs discussed in the Part 1 article.
References
 Mirza, Sohail, Shtargot, Joseph , “Modern thermocouples and a highresolution deltasigma ADC enable highprecision temperature measurement”, EE Times, 6/22/2011, and Reference Schematic 5032
 Ibid.
 Using Thermocouples, Thermocouple Introduction and Theory (PDF),
 See the NIST online databases
 For more details about highaccuracy temperature measurements using a PRTD, see Maxim Integrated application note 5244, “Modern PRTD Temperature Sensors and HighAccuracy DeltaSigma ADCs Enable Wide Range Highaccuracy Temperature Measurements”. Equation 4 from this application note is used for RTD temperature measurement.
 Ibid.
 NIST online databases, op. cit.
 For more information see Maxim Integrated application note 4679, “Thermal Management Handbook”.
 NIST online databases, op. cit.
 See reference 1.
 For more details of highaccuracy temperature measurements using PRTD, see the application note cited in reference 8.
 For information on the Ktype OMEGA thermocouple KTSS116 (PDF), go to “Molded Transition Joint Probes,” OMEGA.
Fluke is a registered trademark of Fluke Corporation.
OMEGA is a registered trademark of Omega Engineering, Inc.
© Nov 22, 2013, Maxim Integrated Products, Inc.

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