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After withdrawing the tube from liquid N2 the hermetic cup of the tube 1 was opened and a needle thermo-sensor of the measuring device Biophys-TT (produced by Electronic Engineering department of LSIEPC, Yerevan) was placed into the tube. Then 1 ml. of DW treated by any of the above mentioned factors was poured in the plastic tube (2) and frozen until – 550C. After which the tube 1 with the frozen DW and thermo-sensor in it was withdrawn from the tube 1 and placed at room temperature for melting.

Scaiano, F. L. Cozens, and L. McLean, Model for the rationalization of magnetic field effects in vivo. Application of the radical-pair mechanism to biological systems, Photochem. Photobiol. 59(6), 585-589, (1994). 14. B. Brocklehurst and K. A. McLauchlan, Free radical mechanism for the effects of environmental electromagnetic fields on biological systems, Int. J. Radiat. Biol. 69(1),3-24 (1996). 15. A. R. Liboff, R. J. Rozek, M. J. Sherman, B. R. McLeod, and S. D. Smith, Ca-45 cyclotron resonance in human lymphocytes, J.

After which the tube 1 with the frozen DW and thermo-sensor in it was withdrawn from the tube 1 and placed at room temperature for melting. The temperature changes were continuously recorded by personal computer through Digidata 1322A (production of “Axon Instruments” USA). 34 BIOELECTROMAGNETICS Figure 2. 5 mT) (A), MV (B) and MV (30 dB) after 30 min pre-treated by SMF (12 mT) (C). Initial temperature - 11,90C. As it can be seen from the presented data, the character of frequencydependence of heat release is changed during EMF and MV exposure, and is modulated by preliminary SMF exposure.

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