FORCE STANDARDS COMPARISON BETWEEN PTB (GERMANY) AND CENAM (MEXICO).

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FORCE STANDARDS COMPARISON BETWEEN PTB (GERMANY) AND CENAM (MEXICO). Jorge C. Torres-Guzmán*, Amritlal Sawla**, Daniel Ramírez-Ahedo* * Centro Nacional de Metrología, México. **Physikalisch-Technische Bundesanstalt, Germany. Abstract. A force comparison was carried out between the Centro Nacional de Metrología, CENAM (in Mexico) and the Physikalisch-Technische Bundesanstalt, PTB (in Germany), in order to estimate the level of agreement for the realization of the quantity and the uncertainty associated to its measurement. The comparison was carried out in a range starting at kn and up to 150 kn. In order to achieve best accuracy of the force transducers used was made of 5 sub ranges (5 kn, 0 kn, 50 kn, 100 kn and 150 kn). The results obtained, the deviations graphs that include the uncertainty for each laboratory are presented in this document. 1. Introduction Within the frame of the Physikalisch-Technische Bundesanstalt (PTB, Germany) - Centro Nacional de Metrología (CENAM, Mexico) collaboration, a force comparison was carried out in order to estimate the level of agreement for the realization of the quantity, and the uncertainty associated to its measurement. This constitutes the first force comparison between the two institutions. 1.1 Scope of work The ISO publication "International Vocabulary of Basic and General Terms of Metrology" (VIM), and the International System of Units, SI, were used for the comparison and for the writing of this document. The recommendations in the Guide to the Expression of Uncertainty in Measurement and the Guidelines for key comparison carried out by Consultative Committees were followed [1,, 3, 4]. 1. Program objectives To compare force measurement in the range of kn to 150 kn. Comparison.1 Comparison standards In order to achieve best accuracy of the comparison force transducers used, the range was divided in 5 sub ranges, as shown below. Instrument Make Comparison Sub Ranges Force Steps Digital Amplifier (PTB) HBM - - Digital Amplifier (CENAM) HBM - - Force Transducer up to 5 kn HBM kn to 5 kn kn, 3 kn, 4 kn and 5 kn Force Transducer up to 0 kn GTM 10 kn to 0 kn 10 kn, 1 kn, 16 kn, and 0 kn Force Transducer up to 50 kn GTM 0 kn to 50 kn 0 kn, 30 kn, 40 kn, and 50 kn Force Transducer up to 100 kn GTM 50 kn to 100kN 50 kn, 60 kn, 80 kn, and 100 kn Force Transducer up to 150 kn GTM 100 kn to 150 kn 100 kn, 10kN, 140 kn and 150 kn Table 1. Comparison general information.

. Comparison round The comparison was performed including initial measurements at the PTB force laboratory, measurements at CENAM and final measurements at PTB..3 General guidelines and procedure The most relevant aspects of the measurements procedure and comparison conditions are included in tables 1 and. Readings positions 0, 90, 180, 70 and 360 Readings cycles cycles in each position and 1 cycle at 360 Force application time 180 s Preloads application time 180 s with 180 s resting time between preloads Number of preloads (at maximum force) 3 at 0, at 90, 180, 70 and 360 Temperature during measurements C ± 0,3 K Table. Comparison procedure. 3. Laboratories' standards Both laboratories used dead weight machines (DWM) as their standards for the comparison. The information of the standards used by each laboratory is presented in table 3. Sub Range PTB CENAM kn to 5 kn DWM-00k DWM-CNM-150 kn 10 kn to 0 kn DWM-00k DWM-CNM-150 kn 0 kn to 50 kn DWM-100k DWM-CNM-150 kn 50 kn to 100 kn DWM-100k DWM-CNM-150 kn 100 kn to 150 kn DWM-001M DWM-CNM-150 kn Table 3. Dead weight machines (DWM) used for the comparison by the laboratories. 4. Results As PTB made two full measurements, these were analyzed to assess the stability of the force transducers. The two measurement results for each force transducer are presented in graphs, including deviation and uncertainty for each measurement and its mean value. To increase clarity in the figures, a line is shown connecting the points of measurement. -,0E-04 -,5E-04-3,5E-04 3 4 5 Nom inal Force, kn -,0E-04 -,5E-04 10 1 16 0 Nom inal Force, kn PTB-f inal Figure 1. PTB measurements to the force Figure. PTB measurements to the force transducer for the kn to 5 kn sub range. transducer for the 10 kn to 0 kn sub range.

-,0E-04 -,5E-04 0 30 40 50 Nominal Force, kn -,0E-04 -,5E-04 50 60 80 100 Nom inal Force, kn Figure 3. PTB measurements to the force Figure 4. PTB measurements to the force transducer for the 0 kn to 50 kn sub range. transducer for 50 kn to 100 kn sub range.,0e-05 -,0E-05-4,0E-05-6,0E-05-8,0E-05 100 10 140 150 Nominal Force, kn Figure 5. PTB measurements to the force transducer for the 100 kn to 150 kn sub range. As it is shown in the previous figures, a very small time dependant variation on the instrument's response was detected. This small drift seems to be force dependent too. To compensate this effect, a no linear correction would have to be made; as the maximum drift during the period of the comparison is less than 50 10-6 relative to the applied force (only for one of the force transducers, figure ), the correction of this effect seems to be unnecessary. The results of the measurements made are here presented for each sub range. The results are shown in figures, one figure for each sub range. The figures 6 to 10, include the deviation and uncertainty calculated for the force transducer. In each figure, the points represent the results obtained by CENAM and the mean of PTB initial and final measurements. Similarly, the uncertainties presented for PTB are the mean value of their initial and final measurements. To calculate the deviations and the uncertainties from the measured data, the following considerations were made: The uncertainties calculated were based mainly, on three contributing elements; the standard used by the laboratory, reproducibility of the results (which includes repeatability) and resolution of the comparison standard (force transducer and digital amplifier). The laboratories deviation was calculated respect to an ideal transducer response. The ideal transducer response used was to assume that the last preload applied to each force transducer represented its constant response behavior. Then, the laboratories measurement results were compared to this transducer response.

,0E-04 E-04 -,0E-04-4,0E-04-5,0E-04 3 4 5 -,0E-04 -,5E-04 10 1 16 0 Figure 6. Relative deviation PTB-CENAM for Figure 7. Relative deviation PTB-CENAM for the sub range kn to 5 kn. the sub range 10 kn to 0 kn. E-04 -,0E-04 -,5E-04-3,5E-04 0 30 40 50 -,0E-04 -,5E-04 Figure 8. Relative deviation PTB-CENAM for Figure 9. Relative deviation PTB-CENAM for the sub range 0 kn to 50 kn. the sub range 50 kn to 100 kn. 4,0E-05,0E-05 -,0E-05-4,0E-05-6,0E-05-8,0E-05 Figure 10. Relative deviation PTB-CENAM for the sub range 100 kn to 150 kn. 5. Discussion From the five figures (figures 6 to 10), it can be observed that the laboratories uncertainties calculated for each force transducer are similar except for kn to 5 kn where the uncertainty calculated by CENAM was higher (due to reproducibility). Also, the biggest difference between the results of the two laboratories occurred in figure 7 at 10 kn, where the uncertainties of the laboratories barely overlap each other. In order to compare in a better way the measurement results, a normalized error graph can be used. A modified equation of the one described in NORAMET s document 8 [5] and EAL- P7 [6] is proposed. The equation used here (equation 1) takes into account the initial and final readings performed at PTB. As readings were made in mv/v, the calculated deviation is considered instead of using a force lecture. 100 10 140 150 50 60 80 100

e n e U lab lab e = (1) + U Where, e n - normalized error e lab - laboratory s estimated deviation (e CENAM or e ) e - average estimated deviation = (e CENAM + e ) / U lab - laboratory s expanded uncertainty (U CENAM or U ) U - average expanded uncertainty (three options were used, see equation, 3 and 4) In all calculations, the average from the PTB measurements was used to represent PTB, as: U = (U + U ) / And, e = (e + e )/ The three options for the erence uncertainty values used are: 1) Average. U = ( U CENAM + U PTB mean )/ () ) Combined uncertainty of the two laboratories. U ( U + U )/ = CENAM PTB mean (3) 3) Combined and including the comparison s standard time stability. Where, ( U + U ) 4 S U + = (4) CENAM PTB mean / stability eptb initial eptb final S stability = (5) 3 The force transducer that presented the greatest drift is the one used for the sub range covering from 10 kn to 0 kn (figure ). The variability range for its lower force point (figure 7), is a 0,5 10-4 ; then, the estimated standard deviation, in relative terms from the mean for 10 kn, is obtained as: = S stability 6 50 10 6 ( 3) = 144, 10 The normalized error equation presented here, is used to obtain a new set of graphs for all the sub ranges. It is important to point out that the values should be between and + if equivalence of measurements is to be achieved [5, 6]. In order to provide a better view of the comparison results and of the equivalence of measurement, the next graphs present the most critical results (larger normalized error) from the three options for U, option. 0, -0, 3 4 5 Figure 11. Normalized error, (option ), for Figure 1. Normalized error, (option ), for kn to 5 kn. 10 kn to 0 kn. 0, -0, 10 1 16 0

Norm alized Error 0, -0, 0 30 40 50 Figure 13. Normalized error, (option ), for Figure 14. Normalized error, (option ), for 0 kn to 50 kn. 50 kn to 100 kn. 0, -0, Figure 15. Normalized error, (option ), for 100 kn to 150 kn. 6. Conclusion PTB and CENAM compared their force standards by means of 5 force transducers without performing preliminary measurements prior to the reported data. The transducers response was such as to facilitate the comparison. The results demonstrated agreement between the two laboratories with negligible differences observed. The normalized error equation employed has been proposed as means of assessing comparability between the two laboratories, and its use facilitated the visualization of compatibility of force measurement. The values obtained by means of the normalized error equation were, for almost all cases, below 0,5; only one point was (10 kn, figure 1) and in many points below 0,. References [1] International Vocabulary of Basic and General Terms in Metrology; BIPM, IEC, IFCC, ISO, IUPAC, IUPAP, OIML; 1993. [] The International System of Units (SI); Bureau International des Poids et Mesures. BIPM; 1998. [3] Guide To The Expression Of Uncertainty In Measurement; ISO TAG 4 WG 3. BIPM, IEC, IFCC, ISO, IUPAC, IUPAP, OIML; 1995. [4] Quinn T. J. Guidelines for key comparison carried out by Consultative Committees. 1997. [5] Document No. 8. Noramet. 1998. [6] EAL-P7, EAL Interlaboratory Comparisons. 1996. Contact Points Dr. Jorge C. Torres-Guzmán Dr. Amritlal Sawla Centro Nacional de Metrología (CENAM) Physikalisch-Technische Bundesanstalt (PTB) km 4,5 carretera a Los Cués, El Marqués, Querétaro Bundesallee 100 D-38116, Braunschweig C.P. 76 41, Mexico Germany Tel: (44) 11 057, fax: (44) 11 0578 Tel: (531) 59 110, fax: (531) 59 105 e-mail jtorres@cenam.mx. e-mail Amritlal.Sawla@ptb.de 0, -0, 100 10 140 150 50 60 80 100