THE 9.355 GHZ COMPLEX PERMITTIVITY OF LIGHT AND HEAVY-WATER FROM 1 TO90-DEGREES-C USING AN IMPROVED HIGH-PRECISION INSTRUMENTATION SYSTEM

Citation
Xp. Hu et al., THE 9.355 GHZ COMPLEX PERMITTIVITY OF LIGHT AND HEAVY-WATER FROM 1 TO90-DEGREES-C USING AN IMPROVED HIGH-PRECISION INSTRUMENTATION SYSTEM, Journal of chemical and engineering data, 39(4), 1994, pp. 625-638
Citations number
29
Categorie Soggetti
Engineering, Chemical",Chemistry
ISSN journal
00219568
Volume
39
Issue
4
Year of publication
1994
Pages
625 - 638
Database
ISI
SICI code
0021-9568(1994)39:4<625:T9GCPO>2.0.ZU;2-5
Abstract
Recent improvements to a high-precision instrumentation system for mea suring the complex permittivity of high loss liquids using a variable- length transmission sample cell at microwave frequencies are described . An error analysis for this system is given. These improvements have enabled the complex permittivity of heavy water and of double-distille d, deionized light water to be measured with a typical accuracy of +/- 0.1% for epsilon' and +/-0.2% for epsilon'' and a precision of about 0 .02% at 9.355 GHz in the temperature interval from approximately 1 to 90-degrees-C in increments of about 2.5-degrees-C. The values of epsil on'(t) and epsilon''(t) have been fitted to empirical quintic polynomi als in the temperature t(degrees-C). For light water epsilon'(t) = 44. 628(3) + (13.929(8) x 10(-1)t - (3.222(6) x 10(-2)t2 + (3.165(17) x 10 (-4)t3 - (1.503(21) x 10(-6)t4 + (2.67(9) x 10(-9)t5 and epsilon''(t) = 40.573(3) - (1.475(6) x 10(-1)t - (2.477(4) x 10(-2)t2 + (6.092(12) x 10(-4)t3 - (6.000(15) x 10(-6)t4 + (2.213(7) x 10(-8)t5 and for heav y water epsilon'(t) = 31.452(17) + (16.630(28) x 10(-1)t - (2.796(17) x 10(-2)t2 + (1.141(45) x 10(-4)t3 + (0.920(54) x 10(-6)t4 - (7.16(23) x 10(-9)t5 and epsilon''(t) = 37.610(9) + (4.952(16) x 10(-1)t - (4.7 49(10) x 10(-2)t2 + (9.659(26) x 10(-4)t3 - (8.609(30) x 10(-6)t4 + (2 .913(13) x 10(-8)t5. The temperature dependences of the Gibbs free ene rgy, enthalpy, and entropy of activation parameters for the relaxation process as well as the relaxation time have been calculated from both the epsilon'(t) and epsilon''(t) data sets for both light and heavy w ater.