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Featured researches published by G. Jakli.


FEBS Letters | 1993

Naturally occurring deuterium is essential for the normal growth rate of cells

Gábor Somlyai; Gábor Jancsó; G. Jakli; Kornélia Vass; Balázs Barna; Viktor Lakics; Tamás Gaál

The role of naturally occurring D in living organisms has been examined by using deuterium‐depleted water (30–40 ppm D) instead of water containing the natural abundance of D (150 ppm). The deuterium‐depleted water significantly decreased the growth rate of the L929 fibroblast cell line, and also inhibited the tumor growth in xenotransplanted mice. Eighty days after transplantation in 10 (59%) out of 17 tumorous mice the tumor, after having grown, regressed and then disappeared. We suggest that the naturally occurring D has a central role in signal transduction involved in cell cycle regulation.


The Journal of Chemical Thermodynamics | 1972

The vapor pressures of dimethyl sulfoxide and hexadeuterodimethyl sulfoxide from about 313 to 453 K

G. Jakli; W. Alexander Van Hook

Abstract The vapor pressure of (CH3)2SO has been determined from 323 to 443 K by mercury manometry thereby extending the older (293 to 323 K) results of Douglas. A least-squares fit was made to the available data and is suitable from approximately 291. 7 K (the melting temperature) to 463 K, and is ln ( p Torr ) = 17.4922 – 4517.79 ( T K − 47.2583) . The vapor pressure difference, [ p“( CD 3 ) 2 SO ’ − p“ (CH 3 ) 2 SO ’ ], was measured by differential capacitance manometry between 323 and 368 K, and by mercury manometry between 383 and 463 K. The vapor pressure isotope effects derived from the results may be expressed by the equation: ln ( p D p H ) = −43454.6( K T ) 2 + 219.449( K T ) − 0.25996 . The isotope effect on the melting temperature Tm was determined as T m “(CD 3 ) 2 SO’ − T m “(CH 3 ) 2 SO’ = (2.30 ± 0.02) K , substantiating the prediction (above) of a change in sign of the isotope effect around 313 to 318 K.


The Journal of Physical Chemistry | 1972

The vapor pressure isotope effect in aqueous systems. I. H2O-D2O (-64° to 100°) and H216O-H218O (-17° to 16°); Ice and Liquid. II. Alkali metal chloride solution in H2O and D2O (-5° to 100°)

Jovan Pupezin; G. Jakli; Gábor Jancsó; W. Van Alexander Hook


The Journal of Physical Chemistry | 1981

Isotope effects in aqueous systems. 12. Thermodynamics of urea-h4/water and urea-d4/water-d2 solutions

G. Jakli; W. Alexander Van Hook


Journal of Chemical & Engineering Data | 1972

Osmotic coefficients of aqueous solutions of sodium bromide, sodium iodide, potassium fluoride, and calcium chloride between o.deg. and 90.deg.

G. Jakli; W. Alexander Van Hook


The Journal of Physical Chemistry | 1989

Sodium alkyl sulfate apparent molar volumes in normal and heavy water: connection with micellar structure

Szabolcs Vass; Tamás I. Török; G. Jakli; Endre Berecz


Journal of Chemical & Engineering Data | 2001

Excess Thermodynamic Properties of H2O and D2O Solutions of Tetramethylurea, an Azeotropic System. Vapor Pressures, Excess Vapor Pressures, and Vapor Pressure Isotope Effects

G. Jakli; W. Alexander Van Hook


Journal of Chemical & Engineering Data | 1997

Isotope effects in aqueous systems. Excess thermodynamic properties of 1,3-dimethylurea solutions in H2O and D2O

G. Jakli; W. A. Van Hook


Bulletin of the Chemical Society of Japan | 2012

Molar Volumes of Ethoxylated Nonylphenols in Micellar Solutions

Szabolcs Vass; István Lakatos; G. Jakli; István Nagy


The Journal of Physical Chemistry | 1981

Isotope effects in aqueous systems. 12. Thermodynamics of urea-h/sub 4//H/sub 2/O and urea-d/sub 4//D/sub 2/O solutions

G. Jakli; W. A. Van Hook

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T. C. Chan

University of Tennessee

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