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At least 19 recordsLinked to original sources

Diacridines: bifunctional intercalators. I. Chemistry, physical chemistry and growth inhibitory properties.

The synthesis, as well as the rationale for synthesis of diacridines, double intercalators, as potential inhibitors of nucleic acid synthesis is presented. The syntheses of (9-acridyl)-putrescine and -spermine, and bis(-9-acridyl)-putrescine, -spermidine, -spermine diamines and of bis(6-chloro-2-methoxy-9-acridyl)-putrescine and -spermine diamines, all substituted on the terminal NH2 groups are described. In addition, the homologous series of diacridines connected by the amino groups of the diamines NH2(CH2)nNH2 (where n = 2,3,4,6,8,10,12,14,16,18) to the C-9 of the diacridines has been synthesized. The chemical properties of these compounds as well as their molecular relationship to DNA are presented. The effect of the double intercalators on the Tm of DNA and of (A)n - (U)n, (dA)n - (dT)n, (G)n - (C)n and on (dG)n - (dC)n have been determined. The double acridine intercalators produce a much greater increase of the Tm of these nucleic acids than do the single acridine intercalators. They also profoundly affect the Tm of DNA in physiological salt concentrations; under these latter conditions the single intercalators have no effect. The relationship between the length of the chain connecting the two acridine rings and the inhibition of the growth of P-388 cells in vitro and vivo is presented. Their growth inhibitory properties appear, in general, to parallel their intercalative abilities.

Acridines↗

The physical chemistry of biological membranes.

Physical chemistry explains the principles of self-organization of lipids into bilayers that form the matrix of biological membranes, and continuum theory of membrane energetics is successful in explaining many biological processes. With increasing sophistication of investigative tools, there is now a growing appreciation for lipid diversity and for the role of individual lipids and specific lipid-protein interactions in membrane structure and function.

Animals↗

Applied physical chemistry for clinical anaesthetists.

Physical chemistry is applicable to many aspects of both clinical anaesthesia and research. This review includes applications in: (a) the supply of gases and vapours; (b) some drug interactions, particularly at the site of absorption; (c) the uptake and distribution of the agents; and (d) mechanisms of anaesthesia based on correlations with physical properties.

Anesthesiology↗

Air and water stable ionic liquids in physical chemistry.

Ionic liquids are defined today as liquids which solely consist of cations and anions and which by definition must have a melting point of 100 degrees C or below. Originating from electrochemistry in AlCl(3) based liquids an enormous progress was made during the recent 10 years to synthesize ionic liquids that can be handled under ambient conditions, and today about 300 ionic liquids are already commercially available. Whereas the main interest is still focussed on organic and technical chemistry, various aspects of physical chemistry in ionic liquids are discussed now in literature. In this review article we give a short overview on physicochemical aspects of ionic liquids, such as physical properties of ionic liquids, nanoparticles, nanotubes, batteries, spectroscopy, thermodynamics and catalysis of/in ionic liquids. The focus is set on air and water stable ionic liquids as they will presumably dominate various fields of chemistry in future.

Air↗

Physical chemistry of freeze-drying: measurement of sublimation rates for frozen aqueous solutions by a microbalance technique.

The sublimation rate of frozen solutions was studied as a function of freezing rate, thickness of dried product (l), temperature, residual air pressure, and solute concentration. Data are presented for pure water, aqueous potassium chloride, aqueous povidone, and aqueous dobutamine hydrochloride-mannitol (System I). The resistance of the dried product to water vapor flow (Rp) was evaluated from the sublimation rate and the sample temperature. The primary experimental technique was based on freeze-drying a cylindrical microsample isothermally, with the sample suspended from one arm of a vacuum microbalance. Methodology to evaluate resistance data from vial freeze-drying experiments is also described. In separate experiments, samples in the form of a thin (15-microns) film were visually observed through a microscope during freeze-drying. Freeze-drying of most samples appeared to occur by water vapor escaping through open channels created by prior sublimation of ice. Contrary to the usual theoretical model, Rp is neither independent of temperature nor directly proportional to l. Rather, Rp decreases with increasing temperature and the l dependence is normally of the form Rp = (A0 + A1l)/(1 + A2l), where Ai (i = 0, 1, 2) are constants. In several cases, Rp is very large near l = 0, decreases sharply at l congruent to 0.1 cm, and obeys the above equation where l greater than 0.2 cm, a result suggesting an amorphous surface skin which cracks on desorption of water. The temperature dependence of Rp suggests that, as the sample temperature approaches the eutectic (or collapse) temperature, hydrodynamic surface flow of adsorbed water is an important flow mechanism.

Air Pressure↗