Abstract
A new formulation of the density of air-saturated water as a function of temperature on the 1990 International Temperature Scale (ITS-90) is presented. Also, a new equation for calculating isothermal compressibility as a function of temperature on ITS-90 was developed. The equations are to be used to calculate the density of water, in the temperature range 5 to 40 °C on ITS-90, used in the gravimetric determination of the volume of volumetric standards.
Keywords: air-saturated water, calibration, density of water, isothermal compressibility, ITS-90, volumetric standards
1. Introduction
In the gravimetric determination of the volume (calibration) of volumetric standards, water is used as the calibrating fluid. The volume is calculated from the mass and density of the water. In many quarters, the formulation of Wagenbreth and Blanke [1] is used to calculate the density of water. In this paper, a new formulation of the density of water (based primarily on the work of Kell [2]) as a function of temperature on the 1990 International Temperature Scale is presented.
2. Kelt’s Formulations
2.1 Density of Water
In 1975, Kell [2] published a new formulation for the density of air-free water at a pressure of 101.325 kPa (1 atmosphere) valid from 0 to 150 °C “that is in improved agreement with most data sets.” The Kell formulation is
(1) |
where t is temperature in °C on the 1968 International Practical Temperature Scale (IPTS-68).
2.2 Isothermal Compressibility
Kell also developed equations for calculation of the isothermal compressibility, κT, of air-free water [2]. In the temperature range 0 to 100 °C on IPTS-68, the equation can be expressed as
(2) |
where κT is isothermal compressibility in (kPa)−1.
3. New Formulations
3.1 Density of Air-Free Water
In the present work, the Kell calculated values of ρ were fitted over the temperature range 5 to 40 °C on the new 1990 International Temperature Scale (ITS-90) [3] to an equation quartic in temperature. The equation is
(3) |
In contrast with the Kell equation, a term in t5 is not necessary due at least in part to the fact that the 0 to 4 °C region, in which ρ increases with increasing temperature, has been excluded. Equation (3) applies to air-free water.
Values of the density of air-free water were calculated for temperatures (ITS-90, t90) between 4.999 and 39.990 °C using Eq. (3) and compared with corresponding Kell values. The estimate of the standard deviation (SD) of the difference was 0.00034 kg m−3. The ratio of SD to the mean value of density was 3.4 × 10−7, which is negligible.
3.2 Conversion of IPTS-68 to ITS-90
A very simple equation relating ITS-90 temperature, t90 to IPTS-68 temperature, t68, has been used in the present work to generate values of t90 for the development of Eq. (3). The equation for the temperature range 0 to 40 °C is
(4a) |
In the temperature range 0 to 100 °C the equation is
(4b) |
3.3 Change in Density of Water with Air Saturation
Bignell [4] measured the change in the density of water with air saturation for 80 points in the range of 4 to 20 °C. He fitted the points to develop the equation
(5) |
where Δρ is in kg m−3. There is no need to adjust for temperature scale. Bignell concluded that “there is probably not much need to extend the work to higher temperatures because the effect diminishes and the accuracy of density metrology at these temperatures would not warrant a more accurately known correction.”
3.4 Density of Air-Saturated Water on ITS-90
Equation (5) was added to Eq. (3) to produce an equation to be used to calculate the density, ρas, of air-saturated water in the temperature range 5 to 40 °C on ITS-90:
(6) |
The uncertainty in the density of air-saturated water for an uncertainty in temperature of 1 °C is approximately 210 ppm or 0.21 kg m−3 at 20 °C.
3.5 Isothermal Compressibility
The thermal compressibility data used by Kell have been fitted against temperature on ITS-90 for the temperature range 5 to 40 °C. The resulting equation is
(7) |
where κT is thermal compressibility in (kPa)−1.
The estimate of standard deviation (SD) of the residual, calculated κT–data κT, is 2.1 × l0−11 (kPa)−1; the ratio of SD to the midrange value of κT is 4.6 × l0−5, which is negligible for present purposes. It is not necessary to make a correction to κT for air saturation.
The value of the isothermal compressibility of water is approximately 46.5 parts per million (ppm)/atmosphere at 20 °C. At locations where the atmospheric pressure is significantly different from 1 atmosphere (101.325 kPa), a correction for compressibility calculated using Eq. (7) should be made. For example, at Boulder, CO, the correction for compressibility is approximately −8 ppm at 20 °C.
3.6 Compressibility-Corrected Water Density Equation
The expression for the density of air-saturated water, ρasc, at an ambient pressure of P kPa is
(8) |
where ρas is calculated using Eq. (6) and κT is calculated using Eq. (7).
4. Tables
Table 1 is a tabulation of values of the density of air-saturated water using Eq. (6). Table 2 is a tabulation of the values of the density of air-free water calculated using Eq. (3). Table 3 is a tabulation of values of air-free water calculated using the formulation of Wagenbreth and Blanke [1], this table has been included in this paper for purposes of comparison.
Table 1.
t(°C) | 0.0 | 0.1 | 0.2 | 0.3 | 0.4 | 0.5 | 0.6 | 0.7 | 0.8 | 0.9 |
---|---|---|---|---|---|---|---|---|---|---|
5 | 0.999961 | 0.999959 | 0.999957 | 0.999955 | 0.999953 | 0.999950 | 0.999948 | 0.999945 | 0.999942 | 0.999939 |
6 | 0.999936 | 0.999933 | 0.999930 | 0.999926 | 0.999922 | 0.999919 | 0.999915 | 0.999911 | 0.999906 | 0.999902 |
7 | 0.999897 | 0.999893 | 0.999888 | 0.999883 | 0.999878 | 0.999872 | 0.999867 | 0.999861 | 0.999856 | 0.999850 |
8 | 0.999844 | 0.999838 | 0.999832 | 0.999825 | 0.999819 | 0.999812 | 0.999805 | 0.999798 | 0.999791 | 0.999784 |
9 | 0.999777 | 0.999769 | 0.999761 | 0.999754 | 0.999746 | 0.999738 | 0.999730 | 0.999721 | 0.999713 | 0.999704 |
10 | 0.999695 | 0.999687 | 0.999678 | 0.999669 | 0.999659 | 0.999650 | 0.999640 | 0.999631 | 0.999621 | 0.999611 |
11 | 0.999601 | 0.999591 | 0.999581 | 0.999570 | 0.999560 | 0.999549 | 0.999538 | 0.999527 | 0.999516 | 0.999505 |
12 | 0.999494 | 0.999482 | 0.999471 | 0.999459 | 0.999447 | 0.999435 | 0.999423 | 0.999411 | 0.999398 | 0.999386 |
13 | 0.999373 | 0.999361 | 0.999348 | 0.999335 | 0.999322 | 0.999309 | 0.999295 | 0.999282 | 0.999268 | 0.999255 |
14 | 0.999241 | 0.999227 | 0.999213 | 0.999199 | 0.999184 | 0.999170 | 0.999156 | 0.999141 | 0.999126 | 0.999111 |
15 | 0.999096 | 0.999081 | 0.999066 | 0.999051 | 0.999035 | 0.999019 | 0.999004 | 0.998988 | 0.998972 | 0.998956 |
16 | 0.998940 | 0.998923 | 0.998907 | 0.998891 | 0.998874 | 0.998857 | 0.998840 | 0.998823 | 0.998806 | 0.998789 |
17 | 0.998772 | 0.998754 | 0.998737 | 0.998719 | 0.998701 | 0.998683 | 0.998665 | 0.998647 | 0.998629 | 0.998611 |
18 | 0.998592 | 0.998574 | 0.998555 | 0.998536 | 0.998517 | 0.998499 | 0.998479 | 0.998460 | 0.998441 | 0.998421 |
19 | 0.998402 | 0.998382 | 0.998363 | 0.998343 | 0.998323 | 0.998303 | 0.998283 | 0.998262 | 0.998242 | 0.998221 |
20 | 0.998201 | 0.998180 | 0.998159 | 0.998138 | 0.998117 | 0.998096 | 0.998075 | 0.998054 | 0.998032 | 0.998011 |
21 | 0.997989 | 0.997967 | 0.997945 | 0.997924 | 0.997901 | 0.997879 | 0.997857 | 0.997835 | 0.997812 | 0.997790 |
22 | 0.997767 | 0.997744 | 0.997721 | 0.997698 | 0.997675 | 0.997652 | 0.997629 | 0.997606 | 0.997582 | 0.997559 |
23 | 0.997535 | 0.997511 | 0.997487 | 0.997463 | 0.997439 | 0.997415 | 0.997391 | 0.997366 | 0.997342 | 0.997317 |
24 | 0.997293 | 0.997268 | 0.997243 | 0.997218 | 0.997193 | 0.997168 | 0.997143 | 0.997118 | 0.997092 | 0.997067 |
25 | 0.997041 | 0.997015 | 0.996990 | 0.996964 | 0.996938 | 0.996912 | 0.996885 | 0.996859 | 0.996833 | 0.996806 |
26 | 0.996780 | 0.996753 | 0.996726 | 0.996700 | 0.996673 | 0.996646 | 0.996619 | 0.996591 | 0.996564 | 0.996537 |
27 | 0.996509 | 0.996482 | 0.996454 | 0.996426 | 0.996399 | 0.996371 | 0.996343 | 0.996314 | 0.996286 | 0.996258 |
28 | 0.996230 | 0.996201 | 0.996173 | 0.996144 | 0.996115 | 0.996086 | 0.996057 | 0.996028 | 0.995999 | 0.995970 |
29 | 0.995941 | 0.995912 | 0.995882 | 0.995853 | 0.995823 | 0.995793 | 0.995764 | 0.995734 | 0.995704 | 0.995674 |
30 | 0.995643 | 0.995613 | 0.995583 | 0.995553 | 0.995522 | 0.995491 | 0.995461 | 0.995430 | 0.995399 | 0.995368 |
31 | 0.995337 | 0.995306 | 0.995275 | 0.995244 | 0.995212 | 0.995181 | 0.995149 | 0.995118 | 0.995086 | 0.995054 |
32 | 0.995023 | 0.994991 | 0.994959 | 0.994927 | 0.994894 | 0.994862 | 0.994830 | 0.994797 | 0.994765 | 0.994732 |
33 | 0.994699 | 0.994667 | 0.994634 | 0.994601 | 0.994568 | 0.994535 | 0.994502 | 0.994468 | 0.994435 | 0.994402 |
34 | 0.994368 | 0.994334 | 0.994301 | 0.994267 | 0.994233 | 0.994199 | 0.994165 | 0.994131 | 0.994097 | 0.994063 |
35 | 0.994028 | 0.993994 | 0.993960 | 0.993925 | 0.993890 | 0.993856 | 0.993821 | 0.993786 | 0.993751 | 0.993716 |
36 | 0.993681 | 0.993646 | 0.993610 | 0.993575 | 0.993539 | 0.993504 | 0.993468 | 0.993433 | 0.993397 | 0.993361 |
37 | 0.993325 | 0.993289 | 0.993253 | 0.993217 | 0.993181 | 0.993144 | 0.993108 | 0.993071 | 0.993035 | 0.992998 |
38 | 0.992962 | 0.992925 | 0.992888 | 0.992851 | 0.992814 | 0.992777 | 0.992740 | 0.992702 | 0.992665 | 0.992628 |
39 | 0.992590 | 0.992553 | 0.992515 | 0.992477 | 0.992439 | 0.992401 | 0.992363 | 0.992325 | 0.992287 | 0.992249 |
Table 2.
t(°C) | 0.0 | 0.1 | 0.2 | 0.3 | 0.4 | 0.5 | 0.6 | 0.7 | 0.8 | 0.9 |
---|---|---|---|---|---|---|---|---|---|---|
5 | 0.999965 | 0.999963 | 0.999961 | 0.999959 | 0.999957 | 0.999954 | 0.999952 | 0.999949 | 0.999946 | 0.999943 |
6 | 0.999940 | 0.999937 | 0.999934 | 0.999930 | 0.999926 | 0.999923 | 0.999919 | 0.999914 | 0.999910 | 0.999906 |
7 | 0.999901 | 0.999896 | 0.999892 | 0.999887 | 0.999881 | 0.999876 | 0.999871 | 0.999865 | 0.999860 | 0.999854 |
8 | 0.999848 | 0.999842 | 0.999835 | 0.999829 | 0.999822 | 0.999816 | 0.999809 | 0.999802 | 0.999795 | 0.999788 |
9 | 0.999780 | 0.999773 | 0.999765 | 0.999757 | 0.999749 | 0.999741 | 0.999733 | 0.999725 | 0.999716 | 0.999708 |
10 | 0.999699 | 0.999690 | 0.999681 | 0.999672 | 0.999663 | 0.999653 | 0.999644 | 0.999634 | 0.999624 | 0.999615 |
11 | 0.999604 | 0.999594 | 0.999584 | 0.999574 | 0.999563 | 0.999552 | 0.999541 | 0.999531 | 0.999519 | 0.999508 |
12 | 0.999497 | 0.999485 | 0.999474 | 0.999462 | 0.999450 | 0.999438 | 0.999426 | 0.999414 | 0.999402 | 0.999389 |
13 | 0.999377 | 0.999364 | 0.999351 | 0.999338 | 0.999325 | 0.999312 | 0.999299 | 0.999285 | 0.999272 | 0.999258 |
14 | 0.999244 | 0.999230 | 0.999216 | 0.999202 | 0.999188 | 0.999173 | 0.999159 | 0.999144 | 0.999129 | 0.999114 |
15 | 0.999099 | 0.999084 | 0.999069 | 0.999053 | 0.999038 | 0.999022 | 0.999007 | 0.998991 | 0.998975 | 0.998959 |
16 | 0.998943 | 0.998926 | 0.998910 | 0.998893 | 0.998877 | 0.998860 | 0.998843 | 0.998826 | 0.998809 | 0.998792 |
17 | 0.998774 | 0.998757 | 0.998739 | 0.998722 | 0.998704 | 0.998686 | 0.998668 | 0.998650 | 0.998632 | 0.998613 |
18 | 0.998595 | 0.998576 | 0.998558 | 0.998539 | 0.998520 | 0.998501 | 0.998482 | 0.998463 | 0.998444 | 0.998424 |
19 | 0.998405 | 0.998385 | 0.998365 | 0.998345 | 0.998325 | 0.998305 | 0.998285 | 0.998265 | 0.998244 | 0.998224 |
20 | 0.998203 | 0.998183 | 0.998162 | 0.998141 | 0.998120 | 0.998099 | 0.998077 | 0.998056 | 0.998035 | 0.998013 |
21 | 0.997991 | 0.997970 | 0.997948 | 0.997926 | 0.997904 | 0.997882 | 0.997859 | 0.997837 | 0.997815 | 0.997792 |
22 | 0.997769 | 0.997746 | 0.997724 | 0.997701 | 0.997678 | 0.997654 | 0.997631 | 0.997608 | 0.997584 | 0.997561 |
23 | 0.997537 | 0.997513 | 0.997489 | 0.997465 | 0.997441 | 0.997417 | 0.997393 | 0.997369 | 0.997344 | 0.997320 |
24 | 0.997295 | 0.997270 | 0.997245 | 0.997220 | 0.997195 | 0.997170 | 0.997145 | 0.997120 | 0.997094 | 0.997069 |
25 | 0.997043 | 0.997017 | 0.996992 | 0.996966 | 0.996940 | 0.996914 | 0.996887 | 0.996861 | 0.996835 | 0.996808 |
26 | 0.996782 | 0.996755 | 0.996728 | 0.996701 | 0.996675 | 0.996648 | 0.996620 | 0.996593 | 0.996566 | 0.996539 |
27 | 0.996511 | 0.996483 | 0.996456 | 0.996428 | 0.996400 | 0.996372 | 0.996344 | 0.996316 | 0.996288 | 0.996260 |
28 | 0.996231 | 0.996203 | 0.996174 | 0.996146 | 0.996117 | 0.996088 | 0.996059 | 0.996030 | 0.996001 | 0.995972 |
29 | 0.995942 | 0.995913 | 0.995884 | 0.995854 | 0.995824 | 0.995795 | 0.995765 | 0.995735 | 0.995705 | 0.995675 |
30 | 0.995645 | 0.995615 | 0.995584 | 0.995554 | 0.995523 | 0.995493 | 0.995462 | 0.995431 | 0.995401 | 0.995370 |
31 | 0.995339 | 0.995307 | 0.995276 | 0.995245 | 0.995214 | 0.995182 | 0.995151 | 0.995119 | 0.995087 | 0.995056 |
32 | 0.995024 | 0.994992 | 0.994960 | 0.994928 | 0.994895 | 0.994863 | 0.994831 | 0.994798 | 0.994766 | 0.994733 |
33 | 0.994701 | 0.994668 | 0.994635 | 0.994602 | 0.994569 | 0.994536 | 0.994503 | 0.994469 | 0.994436 | 0.994403 |
34 | 0.994369 | 0.994335 | 0.994302 | 0.994268 | 0.994234 | 0.994200 | 0.994166 | 0.994132 | 0.994098 | 0.994064 |
35 | 0.994029 | 0.993995 | 0.993960 | 0.993926 | 0.993891 | 0.993856 | 0.993822 | 0.993787 | 0.993752 | 0.993717 |
36 | 0.993682 | 0.993646 | 0.993611 | 0.993576 | 0.993540 | 0.993505 | 0.993469 | 0.993433 | 0.993398 | 0.993362 |
37 | 0.993326 | 0.993290 | 0.993254 | 0.993217 | 0.993181 | 0.993145 | 0.993108 | 0.993072 | 0.993035 | 0.992999 |
38 | 0.992962 | 0.992925 | 0.992888 | 0.992851 | 0.992814 | 0.992777 | 0.992740 | 0.992703 | 0.992665 | 0.992628 |
39 | 0.992590 | 0.992553 | 0.992515 | 0.992478 | 0.992440 | 0.992402 | 0.992364 | 0.992326 | 0.992288 | 0.992249 |
Table 3.
t(°C) | 0.0 | 0.1 | 0.2 | 0.3 | 0.4 | 0.5 | 0.6 | 0.7 | 0.8 | 0.9 |
---|---|---|---|---|---|---|---|---|---|---|
5 | 0.999964 | 0.999962 | 0.999960 | 0.999958 | 0.999956 | 0.999954 | 0.999951 | 0.999949 | 0.999946 | 0.999943 |
6 | 0.999940 | 0.999937 | 0.999933 | 0.999930 | 0.999926 | 0.999922 | 0.999918 | 0.999914 | 0.999910 | 0.999906 |
7 | 0.999901 | 0.999896 | 0.999892 | 0.999887 | 0.999881 | 0.999876 | 0.999871 | 0.999865 | 0.999860 | 0.999854 |
8 | 0.999848 | 0.999842 | 0.999835 | 0.999829 | 0.999822 | 0.999816 | 0.999809 | 0.999802 | 0.999795 | 0.999787 |
9 | 0.999780 | 0.999773 | 0.999765 | 0.999757 | 0.999749 | 0.999741 | 0.999733 | 0.999725 | 0.999716 | 0.999707 |
10 | 0.999699 | 0.999690 | 0.999681 | 0.999672 | 0.999662 | 0.999653 | 0.999643 | 0.999634 | 0.999624 | 0.999614 |
11 | 0.999604 | 0.999594 | 0.999583 | 0.999573 | 0.999562 | 0.999552 | 0.999541 | 0.999530 | 0.999519 | 0.999507 |
12 | 0.999496 | 0.999485 | 0.999473 | 0.999461 | 0.999449 | 0.999437 | 0.999425 | 0.999413 | 0.999401 | 0.999388 |
13 | 0.999376 | 0.999363 | 0.999350 | 0.999337 | 0.999324 | 0.999311 | 0.999297 | 0.999284 | 0.999270 | 0.999256 |
14 | 0.999243 | 0.999229 | 0.999215 | 0.999200 | 0.999186 | 0.999172 | 0.999157 | 0.999142 | 0.999128 | 0.999113 |
15 | 0.999098 | 0.999083 | 0.999067 | 0.999052 | 0.999036 | 0.999021 | 0.999005 | 0.998989 | 0.998973 | 0.998957 |
16 | 0.998941 | 0.998925 | 0.998908 | 0.998892 | 0.998875 | 0.998858 | 0.998841 | 0.998824 | 0.998807 | 0.998790 |
17 | 0.998773 | 0.998755 | 0.998738 | 0.998720 | 0.998702 | 0.998684 | 0.998666 | 0.998648 | 0.998630 | 0.998612 |
18 | 0.998593 | 0.998575 | 0.998556 | 0.998537 | 0.998519 | 0.998500 | 0.998480 | 0.998461 | 0.998442 | 0.998422 |
19 | 0.998403 | 0.998383 | 0.998364 | 0.998344 | 0.998324 | 0.998304 | 0.998284 | 0.998263 | 0.998243 | 0.998222 |
20 | 0.998202 | 0.998181 | 0.998160 | 0.998139 | 0.998118 | 0.998097 | 0.998076 | 0.998055 | 0.998033 | 0.998012 |
21 | 0.997990 | 0.997968 | 0.997947 | 0.997925 | 0.997903 | 0.997881 | 0.997858 | 0.997836 | 0.997814 | 0.997791 |
22 | 0.997768 | 0.997746 | 0.997723 | 0.997700 | 0.997677 | 0.997654 | 0.997630 | 0.997607 | 0.997584 | 0.997560 |
23 | 0.997536 | 0.997513 | 0.997489 | 0.997465 | 0.997441 | 0.997417 | 0.997392 | 0.997368 | 0.997344 | 0.997319 |
24 | 0.997294 | 0.997270 | 0.997245 | 0.997220 | 0.997195 | 0.997170 | 0.997145 | 0.997119 | 0.997094 | 0.997068 |
25 | 0.997043 | 0.997017 | 0.996991 | 0.996966 | 0.996940 | 0.996913 | 0.996887 | 0.996861 | 0.996835 | 0.996808 |
26 | 0.996782 | 0.996755 | 0.996723 | 0.996702 | 0.996675 | 0.996648 | 0.996621 | 0.996593 | 0.996566 | 0.996539 |
27 | 0.996511 | 0.996484 | 0.996456 | 0.996428 | 0.996401 | 0.996373 | 0.996345 | 0.996316 | 0.996288 | 0.996260 |
28 | 0.996232 | 0.996203 | 0.996175 | 0.996146 | 0.996117 | 0.996088 | 0.996060 | 0.996031 | 0.996001 | 0.995972 |
29 | 0.996943 | 0.995914 | 0.995884 | 0.995855 | 0.995825 | 0.995795 | 0.995765 | 0.995736 | 0.995706 | 0.995676 |
30 | 0.995645 | 0.995615 | 0.995585 | 0.995554 | 0.995524 | 0.995493 | 0.995463 | 0.995432 | 0.995401 | 0.995370 |
31 | 0.995339 | 0.995308 | 0.995277 | 0.995246 | 0.995214 | 0.995183 | 0.995151 | 0.995120 | 0.995088 | 0.995056 |
32 | 0.995024 | 0.994992 | 0.994960 | 0.994928 | 0.994896 | 0.994864 | 0.994831 | 0.994799 | 0.994766 | 0.994734 |
33 | 0.994701 | 0.994668 | 0.994635 | 0.994602 | 0.994569 | 0.994536 | 0.994503 | 0.994470 | 0.994436 | 0.994403 |
34 | 0.994369 | 0.994336 | 0.994302 | 0.994268 | 0.994234 | 0.994201 | 0.994167 | 0.994132 | 0.994098 | 0.994064 |
35 | 0.994030 | 0.993995 | 0.993961 | 0.993926 | 0.993891 | 0.993857 | 0.993822 | 0.993787 | 0.993752 | 0.993717 |
36 | 0.993682 | 0.993647 | 0.993611 | 0.993576 | 0.993541 | 0.993505 | 0.993469 | 0.993434 | 0.993398 | 0.993362 |
37 | 0.993326 | 0.993290 | 0.993254 | 0.993218 | 0.993182 | 0.993146 | 0.993109 | 0.993073 | 0.993036 | 0.993000 |
38 | 0.992963 | 0.992926 | 0.992889 | 0.992852 | 0.992815 | 0.992778 | 0.992741 | 0.992704 | 0.992667 | 0.992629 |
39 | 0.992592 | 0.992554 | 0.992517 | 0.992479 | 0.992442 | 0.992404 | 0.992366 | 0.992328 | 0.992290 | 0.992252 |
The units for water density in these tables are g/cm3, as a convenience to those who routinely use these units.
5. Summary
Equation (3) can be used to calculate the density of air-free water in the temperature range of 5 to 40 °C in ITS-90 at one atmosphere.
Equation (6) can be used to calculate the density of air-saturated water in the same temperature range at one atmosphere.
Equation (8) can be used to calculate the density of air-saturated water in the same temperature range at an ambient pressure of P kPa.
The use of Eq. (6) for air-saturated water, and Eq. (8) where appropriate, is recommended for calculation of water density.
Biography
About the authors: Frank E. Jones is a physicist and an independent consultant who retired from the National Bureau of Standards (now NIST) in 1987. Georgia L. Harris is a physical scientist with the Office of Weights and Measures at NIST. The National Institute of Standards and Technology is an agency of the Technology Administration, U.S. Department of Commerce.
6. References
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