The Effect of Changing the Applied Sequence Using the TVC on the Accuracy of the AC Signal Calibration

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Sensors & Transducers 2013 by IFSA http://www.sensorsportal.com The Effect of Changing the Sequence Using the TVC on the Accuracy of the AC Signal Calibration Rasha S. M. Ali National Institute for Standards (NIS), Tersa Street-Elharam, Giza, 12211, Egypt Tel.: 0201003342242, fax: 0020233867451 E-mail: rasha_sama79@hotmail.com Received: 31 January 2013 /Accepted: 14 June 2013 /Published: 25 June 2013 Abstract: Ac signals are accurately measured by using Thermal Converters (TCs). In this paper, ac voltages are automatically calibrated as an example by the Thermal Voltage Converter (TVC) with changing the sequence of the applied signals. 1 V, 10 V, and 100 V at different frequencies from 50 Hz to 100 khz are measured. The three different sequences are sequence #1 which is (+dc, ac, -dc), sequence #2 which is (ac, +dc, -dc, ac), and sequence #3 which is (ac, +dc, ac, -dc, ac). The effect of changing the applied sequence is studied to have the more precise and accurate performance. In order to achieve switching between ac and dc at regular and precise intervals and the comparison is made sequentially, a LabVIEW program is especially built for this study. The uncertainty budgets for the different ac voltages are also evaluated. Copyright 2013 IFSA. Keywords: ac metrology, Thermal-element, Thermal voltage converter, Range resistors, Temperature coefficient, Uncertainty. 1. Introduction TCs are the most accurate true root-mean-square (rms) measuring devices available. They are employed as ac-dc transfer standards in National Metrology Institutes (NMIs) [1]. In primary laboratories, the use of TCs has been preferred to other methods for the accurate measurement of ac signal because they are static, easily transportable, and less difficult to handle [2]. These consist mainly of a resistor operating as a heater thermal-element (TE) to which a voltage or a current signal is applied. In close contact with the heater, but galvanically insulated from it, a temperature sensor measures the temperature rise above ambient and thus the energy content of the signal [1]. These temperature sensors, thermocouples are used to monitor the temperature along the heater structure while applying a timed sequence of an ac signal and both polarities of a dc signal. By comparing the output of the TE with ac applied to the average output of the TE when both polarities of dc are applied, the unknown ac quantity may be determined in terms of the known dc quantity [3]. This ac-dc difference is calculated from [4, 5]. Accurate and consistent measurements can be made under these circumstances, if readings are taken at time intervals that are about equal and in a sequence which tends to average out the effect of drift. For example, some NMIs are making their measurements according to the sequence (+dc, ac, - dc), and other NMI are applying the ac and the polarities of the dc signals according to the sequence (ac, +dc, -dc, ac), furthermore others according to the Article number P_1233 155

sequence (ac, +dc, ac, -dc, ac). The effect of changing the applied sequence on the precision and accuracy of the ac signal measurement is practically studied in this work through a practical comparison is done between them. It is advantageous to avoid as much as possible any variation of the thermal conditions [6] and switching between ac and dc with the shortest possible interruption of the input voltage is a prerequisite to achieve constant heating conditions in the TCs. Short means here that the switching time must be small compared to the thermal time constant of the TCs [6]. The short switching time can be achieved by automatically calibrating these TCs rather than manually. Thus, a LabVIEW program is especially designed to achieve this purpose. 2. Automatic Measurement System Set-Up To study the effect of changing the applied sequences on the ac voltages measurement as an example, a comparison is done between the three different applied sequences using TVC. They are sequence #1 which is (+dc, ac, -dc), sequence #2 which is (ac, +dc, -dc, ac), and sequence #3 which is (ac, +dc, ac, -dc, ac). 1 V, 10 V, and 100 V ac voltages at different frequencies from 50 Hz to 100 khz are accurately calibrated according to the three different sequences. The TVC ratings are 1 V, 90. For voltages above 1 V, range resistors are used. They are connected coaxially with the TVC. The measurement system as shown in Fig. 1 contains a calibration system, Fluke model 5720A which is the source of the ac voltage and the stable and reference dc, TVC connected in series with the range resistor for the 10 V and 100V ranges to calibrate the ac voltage, DMM, Fluke model 8508A; 8.5 digits; which measures the e.m.f from the TVC output, and a computer programmed with the suitable software (LabVIEW). The calibration system and the DMM are connected to the computer through GPIB cables. This calibration of the ac voltages is done automatically by using a LabVIEW program. This software controls the measurements of the ac voltages through GPIB card and GPIB cables. In this way switching between ac and dc takes place at constant intervals. Fig. 2 shows the Front panel of the LabVIEW program. It consists of controls and indicators. Each icon controls the system performance. Such as, the "Warming-Up Time" controls the time of the "Warming-Up Voltage" and the "Delay" controls the time waiting before recording the values from the DMM after the TVC reaches to its steady-state. The icons of "Rating Voltage" and "Frequencies" identify the values of the voltage and the frequency required for the measurement. The calibration of each ac voltage at the different frequencies according to the three applied sequences is done sequentially as shown in Fig. 2. This is done in the same environmental conditions. Fig. 2. Front panel of the designed LabVIEW program. 3. Measurement Results and Uncertainty Evaluation Fig. 1. Measurement System set-up. The results of the ac voltages obtained by applying the three different sequencies on the TVC input are compared to the actual values of the ac voltages. Table 1 shows the measured values of the ac voltages for the ranges 1 V, 10 V, 100 V at frequencies 50 Hz, 100 Hz, 1 khz, 10 khz and 100 khz. It is found from the table that the measurement results of the 1 V at the different 156

frequencies obtained by sequence #1, sequence #2, and sequence #3 are very close to the actual values. For the calibration of the higher voltages such as 10 V and 100 V, It's shown that the results obtained from sequence #2 and sequence #3 are very closed to the actual values but sequence #1 is far from them. Each result in Table 1 is calculated from [4, 5]. The uncertainty for the ac voltages measurements, 1 V, 10 V, and 100 V at the frequencies from 50 Hz to 100 khz is evaluated with 95 % confidence level using a (coverage factor k=2) according to the ISO GUM [7]. All components of the combined standard uncertainty (Type A, and Type B) are taken into consideration. Table 2 illustrates the uncertainty budget for the 10 V at 50 Hz by applying sequence #3 as an example. Table 3 shows Type A, Type B and expanded uncertainties associated with the measurement of the 1 V at frequencies 50 Hz, 100 Hz, 1 khz, 10 khz, and 100 khz by applying the three different sequences. It's shown from Table 3 that the Type A and the expanded uncertainty of the measurand 1 V at the different frequencies by sequence #1 is slightly high than sequence #2 and sequence #3. Table 4 shows Type A, Type B and expanded uncertainties associated with the measurement of the 10 V at frequencies 50 Hz, 100 Hz, 1 khz, 10 khz, and 100 khz by applying the three different sequences. Table 5 shows Type A, Type B and expanded uncertainties associated with the measurement of the 100 V at frequencies 50 Hz, 100 Hz, 1 khz, 10 khz, and 100 khz by applying the three different sequences. It can be noticed from Table 4 and Table 5 that the Type A and the expanded uncertainty of the measurands 10 V and 100 V at the different frequencies by applying sequence #1 is much higher than sequence #2 and sequence #3. This indicates that sequence #2 and sequence #3 is more precise than sequence #1 in the higher ranges of the ac voltages measurement. Table 1. 1 V, 10 V and 100 V results at different frequencies. Voltage 1 V 10 V 100 V Measured Values, V Freq. (Hz) Sequence#1 Sequence#2 Sequence#3 Actual Value 50 0.9999885 0.9999826 0.9999820 0.999981 100 0.9999745 0.9999855 0.9999866 0.999981 1000 1.0000036 0.9999804 0.9999866 0.999984 10000 0.9999771 0.9999844 0.9999805 0.999981 100000 0.9999954 1.0000160 1.0000060 0.999988 50 10.001281 9.9999441 9.9999441 10.00002 100 10.002297 0.9999441 9.9999441 10.00002 1000 10.000688 10.000088 10.000062 10.00003 10000 10.001239 9.9999591 9.9999591 9.99999 100000 10.001570 9.9998101 9.9998701 9.99980 50 100.01795 100.00008 99.999111 99.9987 100 100.01483 99.998899 99.998773 99.9987 1000 99.985441 99.998302 99.998793 99.9985 10000 100.01774 99.995246 99.995107 99.9981 100000 100.02469 100.00218 100.00220 99.9926 Uncertainty Sources Table 2. Uncertainty budget for 10 V at 50 Hz by sequence #3. Standard Uncertainty Probability distribution Divider C i Uncertainty contribution, ppm Type A 0.31 ppm Normal 1 1 0.3 DVM accuracy 3.3 ppm Normal 2 1 1.7 TVC Calibration 15 ppm Normal 2 1 7.5 DC Voltage Calibration 0.42 ppm Normal 2 1 0.2 Thermal e.m.f 7.45 ppm Rectangular 3 1 4.3 Resolution 0.07 ppm Rectangular 3 1 0.04 Combined standard uncertainty: Effective degrees of freedom: Expanded Uncertainty at confidence level 95%, (k = 2): ±8.8 ppm ±18 ppm 157

Table 3. Type A, Type B and Exp. Uncertainties of 1 V. Sequences Sequence #1 Sequence #2 Sequence #3 Relative Uncertainties, Nominal Frequency ppm 50 Hz 100 Hz 1 khz 10 khz 100 khz Type A 2.6 4 7 11.2 12.4 Type B 5.34 5.34 5.1 5.1 5.9 Exp. Uncertainty (k=2) 12 16 17 25 28 Type A 1.14 1.7 2.6 8.1 9.3 Type B 5.34 5.34 5.1 5.1 5.9 Exp. Uncertainty (k=2) 11 11 12 19 22 Type A 1.24 1.02 1.3 7.5 7.2 Type B 5.34 5.34 5.1 5.1 5.9 Exp. Uncertainty (k=2) 11 11 11 18 19 Table 4. Type A, Type B and Exp. Uncertainties of 10 V. Sequences Sequence #1 Sequence #2 Sequence #3 Relative Uncertainties, Nominal Frequency ppm 50 Hz 100 Hz 1 khz 10 khz 100 khz Type A 11 17.2 13.3 8 13.3 Type B 8.8 8.8 8.8 8.8 8.8 Exp. Uncertainty (k=2) 28 39 32 24 32 Type A 0.8 0.6 1.6 2 6.5 Type B 8.8 8.8 8.8 8.8 8.8 Exp. Uncertainty (k=2) 18 18 18 18 22 Type A 0.3 0.33 2.2 2.3 7 Type B 8.8 8.8 8.8 8.8 8.8 Exp. Uncertainty (k=2) 18 18 18 18 23 Table 5. Type A, Type B and Exp. Uncertainties of 100 V. Sequences Sequence #1 Sequence #2 Sequence #3 Relative Uncertainties, Nominal Frequency ppm 50 Hz 100 Hz 1 khz 10 khz 100 khz Type A 3.54 11.2 6.23 9.7 13.8 Type B 11 11 11 11 11 Exp. Uncertainty (k=2) 23 32 26 30 36 Type A 1 1.13 1.9 3.7 7.8 Type B 11 11 11 11 11 Exp. Uncertainty (k=2) 22 22 22 23 23 Type A 1 0.93 0.84 2.8 3 Type B 11 11 11 11 11 Exp. Uncertainty (k=2) 22 22 22 23 23 Fig. 3, Fig. 4, and Fig. 5 show the visual charts of the measured values, 1 V, 10 V, and 100 V at the different frequencies and their uncertainties for the different applying sequences. These visual charts present a quick comparison on the effect of changing the different applied sequences on the accuracy and the uncertainty of the ac voltage measurements. Each visual chart at each frequency is represented with the three error bars. The midpoint in each bar represents the value of the measurand. The lower limit and the upper limit represent the uncertainty limits. The shortness of the error bar denotes the lower uncertainty. It is found from Fig. 3 that the measured values, obtained by applying the three different sequences are very near to each other and also, their expanded uncertainties. This means that the applied sequences have not a great effect on the low ac voltages measurement. In Fig. 4 and Fig. 5, they are illustrated that the results and the expanded uncertainties which are obtained by applying sequence #2 and sequence #3 are close to each other, but sequence #1 is greatly different from them. This reflects that the applied sequences #2 and #3 have a great effect on the accuracy of the higher ranges of the ac voltages measurement. That is due to the thermoelectric effects and the temperature coefficient of the TVC which is connected in series with the range resistors which need to apply ac signal again to avoid the drift and take the average of them. 158

AC Voltage (Volt) 1.00006 1.00004 1.00002 1 0.99998 0.99996 0.99994 0.99992 0.9999 1 V at Different Frequencies 1 2 3 4 5 55 Hz 100 Hz 1 khz 10 khz 100 khz Fig. 3. Visual chart of 1 V results at different frequencies. AC Voltage (Volt) 10.002 10.0015 10.001 10.0005 10 9.9995 9.999 9.9985 10 V at Different Frequencies 1 2 3 4 5 55 Hz 100 Hz 1 khz 10 khz 100 khz Fig. 4. Visual chart of 10 V results at different frequencies. AC Voltage (Volt) 100.04 100.03 100.02 100.01 100 99.99 99.98 99.97 99.96 100 V at Different Frequencies 1 2 3 4 5 55 Hz 100 Hz 1 khz 10 khz 100 khz Fig. 5. Visual chart of 100 V results at different frequencies. 4. Conclusion The effect of changing the applied sequence on the accuracy and the precision of the ac voltage calibrations by using the TCs is made. A practical comparison is done between the three different applied sequences to study the effect. It is found that the low ac voltage such as 1 V measured by applying the different three sequences is not changed greatly. So, they have not a great effect on the precision and the accuracy of the low ac voltages measurement. On the other hand, the measurement of the higher voltages as 10 V and 100 V which are obtained by applying sequence #2 and sequence #3 are close to each other, but sequence #1 is greatly different from them. This indicates that the applied sequences #2 and #3 have a great effect on the accuracy and the precision of the higher ranges of the ac voltages measurement. Thus, this paper proves that sequence #1 is not recommended to be applied in the higher ranges and sequence #2 is enough to have accurate and precise ac voltage measurements without the need to apply ac voltage again between the both polarities of the dc signal as in sequence #3. This is also saving more time in the measurement of the ac signals by using the TCs. 159

References [1]. Waldemar Guilherme, Kurten Ihlenfeld, Field-effect transistor thermal converters: a promising device for ac-dc transfer and ac power measurements at higher frequencies, Sensors and Actuators A, Vol. 115, 2004, pp. 1-7. [2]. Umberto Pogliano, Gian Carlo Bosco, and Danilo Serazio, Development of a New Type of Electrometic AC-DC Transfer Standard, IEEE Trans. Instrum. Meas., Vol. 49, No. 4, August 2000, pp. 896-900. [3]. Thomas E. Lipe, A Reevaluation of the NIST Low- Frequency Standards for AC-DC Difference in the Voltage Range 0.6-100 V, IEEE Trans. Instrum. Meas., Vol. 74, No. 6, December 1996, pp. 913-917. [4]. Rasha S. M. Ali, Comparison between Two Different Designs in the AC Voltage Measurement, Measurement Journal, Vol. 44, Issue 9, Nov. 2011, pp. 1539-1542. [5]. Joseph R. Kinard, Earl S. Williams and Thomas E. Lipe, Automated Thermal Voltage Converter Intercomparisons, IEEE Transaction on Instrumentation and Measurement, Vol. 74, No. 1, January 1986, pp. 105-107. [6]. M. Flueli and W. Fasel, A Fast Switching System for AC-DC Transfer Measurements, CPEM, 6-10 July 1998, pp. 27-28. [7]. Uncertainty Guide to the expression of uncertainty in measurement, JCGM 100: September 2008, http://www.bipm.org/utils/common/documents/jcgm/ JCGM_100_2008_E.pdf 2013 Copyright, International Frequency Sensor Association (IFSA). All rights reserved. (http://www.sensorsportal.com 160