DETERMINATION OF ALCOHOL AND SUGAR CONTENT IN WINE BY MEANS OF MICROWAVES

DETERMINATION OF ALCOHOL AND SUGAR CONTENT IN WINE BY MEANS OF MICROWAVES

 

V. V. MERIAKRI, E. E. CHIGRAI

 

Institute of Radioengineering and Electronics, Russian Academy of Sciences

Vvedenski sq. 1, Fryazino Moscow Reg. 141190, RUSSIA

E-mail: meriakri@ms.ire.rssi.ru URL http://home.arcor.de/frank.vongratowski/ras.htm

 

1. INTRODUCTION

 

The monitoring of the composition of materials (including water solutions) is an important problem of applied spectroscopy in the optical, infrared, and microwave wavelength bands.

The aim of this paper is to examine the specific features of the application of electromagnetic microwaves (MW) (frequencies f = 3 - 30 GHz) and relatively new millimeter (MM) waves to the alcohol and sugar content determination in water and wines.

Presently, there is extensive literature devoted to the interaction between MW and MM waves and different liquids and water solutions [1 - 8]. The main conclusions in relation to these water-containing substances are as follows:

1. The sensitivity to the content of water and other dipole liquids in different media increases with frequency (e. g., a free space absorption of MM waves in water a > 40 1/cm is much greater than that in all monitored host materials; as wavelength l decreases, the absorption in water increases more rapidly than the absorption in these host materials).

2. Unlike low-frequency waves, MW and MM waves are practically not sensitive to conducting impurities in liquids.

3. MW and MM waves can be used for testing materials that are opaque for optical and infrared waves.

4. MW and MM waves allow one to realize non-destructive, real-time, in-flow measurement of the dielectric properties of media. These properties are closely related to the chemical composition of a substance under test.

 

2. PROPERTIES OF WATER SOLUTIONS

           

            The MW and MM wave dielectric properties (complex permittivity e = e+ ie, losses a, 1/cm) of water, alcohol, and sugar solutions in water (including wine) are practically independent of small mineral and conducting admixtures. Our measurements of e and a at frequencies 3, 10, and 30 GHz have shown that the dielectric properties of alcohol (CHO) and sugar in water and in wine are practically the same (the difference is less than 0.05- 0.1%).

            The dependence of e of water and water solutions in the MW and MM regions on frequency is well known [ ] and is described by the Debye–Cole-Cole law

 

       *        .

            Here, = 2f, = (f ® 0), = (f ® ), - relaxation time, and » 1. All these values are functions of temperature t and chemical composition of a liquid. For water and alcohol,  equals approximately 80 and 25, respectively,  equals approximately 5.0 and 3.3,

respectively, » 10sec, and 10sec (t = 15-25C). Due to the difference in  and for

 

 

water and alcohol, these liquids have essentially different () and losses () in the MW and MM wave range. For example, at frequencies of f» 10 GHz, losses in water are » 7 1/cm, losses in alcohol are » 2 1/cm; at frequencies of f» 3 GHz, » 0.7 1/cm and » 1.5 1/cm. Such difference in dielectric properties may be used for the determination of the alcohol content  % vol. in water. However,the dielectric properties (including losses) of alcohol in water solutions versus the alcohol content  do not obey a simple additive law. Therefore, we carried out the measurements of () and () at frequencies of interest. The measurements carried out in a rectangular metal waveguide of cross section 7.2 ´ 3.4 cm have shown that, at frequency of f, the transparency T of alcohol solution allows us to determine  20% with an accuracy of < 0.05 % vol. for given temperature.

            As for the sugar solutions in water, we also carried out the measurements of and  and T depending on the sugar concentration W g/litre at frequencies of f and f. It was found that it is possible to measure W < 300 g/litre with an accuracy of W/W  0.05 %.

            The results of the measurements of (,W), (,W), and T(,W) at frequencies of f and f in alcohol--sugar aqueous solutionshave shown that it is possible to determine the alcohol and sugar content in water for  20% and W 300 g/litre with practically the same accuracy as in the alcohol--water and sugar-in-water solutions if we measure T at two frequencies.

            The next step was the application of above-mentioned investigations to the method of determination of both alcohol and sugar content in wine.

 

3. A SET-UP FOR MEASURING ALCOHOL AND SUGAR CONTENT IN WINE

 

            An experimental set-up for measuring the alcohol and sugar content in wine was designed. The set-up consists of a metal coaxial line with a TEM mode operating at frequency f and a measuring cell (a section of a circular metal waveguide supporting a TM mode with liquid under test) of length 4 cm inserted into this coaxial line. The cell has dielectric matching windows on its both ends to avoid reflection from the boundaries. The cell has longitudinal slots in its walls and is inserted into a bath with liquid under test. These slots do not affect the propagation conditions for a TM mode and, at the same time, allow a liquid to flow through the cell. A section of a rectangular metal waveguide of cross section 2.3 ´ 0.5 cm supporting a TE mode at frequency f and with open ends and a matching window is inserted into a bath with a liquid. A second similar section is situated in the liquid along the same axis as the first section. The distance between these sections is of 0.45 cm.

            After the calibration of the set-up, the alcohol content  and sugar content W are determined from two measurements:

a)     The measurement of transparency T at frequency fallows one to find  independently of W;

b)     The measurement of transparency T at frequency f allows one to determine W using the known value of .

The measurements were carried out with five kinds of wines (white and red),  = 9 – 18 % vol., W 30 g/litre. The accuracy of determining  and W was about 0.1 % vol. and 0.3 g/litre, respectively.

 

4. CONCLUSION

 

The measurements of the transparency of a wine material at two frequencies (3 and 10 GHz) in the microwave region allow us to realize nondestructive, in-flow, and real-time method for determining the alcohol and sugar content in these liquids.

 

5. ACKNOWLEDGMENT

  

*   The authors wish to thank Prof. Guram Sh. Kevenishvili, Georgian State Polytechnical University, Tbilisi, Georgia, for his assistance in the measurements of wines.

 

REFERENCES

 

[1] Krazewski A.W.: "Microwave aquametry- needs and perspectives".

      IEEE Trans. MTT-39, (1991), Vol. 39, No. 5, pp. 828-835.

[2]. Apletalin V.N., Garin B.M.,. Meriakri V.V.: "Dielectric properties of liquids in the submillimeter band". Radio Engineering and Electronic Physics, (USSR), (1983), Vol. l28, No.1, pp.1-15.

[3]  Meriakri V.V., Chigrai E.E.: "Properties of materials for practical use at the MM and SMM wavelengths". Digest of the 18-th International. Conference on Infrared and Millimeter Waves,  (Colchester, UK), (1993), pp. 68-69.

[4] Meriakri V.V., Chigrai E.E., Nikitin I.P.: "Monitoring the water content of media and materials with millimeter waves". Radio and Communications Technology (Russia), (1996), Vol. 1, No 2, pp. 92-96.

[5] Liebe H.J., Hafford G.A., and Manabe T.: "A model for the complex permittivity of water at frequencies below 1 THz". International. Journal of Infrared and Millimeter Waves, (1991), Vol. 12, No 2, pp. 92-96.

[6] Meriakri V.V., Parkhomenko M.P.: "Application of dielectric waveguide for water control in alcohol". Electromagnetic Waves and Electronic Systems, (2000), Vol. 5, No 1, pp. 38-39, (in Russian).

 

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