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An improved temperature-jump apparatus

โœ Scribed by A.S. Verkman; A.A. Pandiscio; M. Jennings; A.K. Solomon


Publisher
Elsevier Science
Year
1980
Tongue
English
Weight
552 KB
Volume
102
Category
Article
ISSN
0003-2697

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โœฆ Synopsis


A temperature-jump device of the type devised by M. Eigen (1954, Discuss. Furaduy Sot. 17, 194-210) was built using an 8000-to 40,000-V capacitor discharge to raise the temperature of a conductive sample as much as 25ยฐC within 5 ps. The temperature-jump cell design, which differs from that of previously built cells, consists of cylindrical electrodes fitted into a quartz cylindrical observation cell. This allowed for variable electrode spacing and eliminated high-voltage arcing as well as the need to degas samples to prevent solution cavitation. The temperature of a 0.3-to 3.0-ml sample volume could be adjusted over a -20 to 60ยฐC temperature range by circulating 20% glycerol in water through the hollow, stainless-steel electrodes. Absorption, fluorescence, and scattering measurements could be made over the wavelength range 220 to 750 nm with signal to noise ratios generally exceeding 1000: 1. A battery-driven, high-intensity mercury arc lamp provided stable. ripple-free light. The optical signal was amplified, digitized by a waveform recorder, transferred to a computer, and analyzed numerically to resolve multipleexponential decay processes. The performance of this apparatus is illustrated by several membrane-substrate interactions.


๐Ÿ“œ SIMILAR VOLUMES


A simple stopped-flow temperature-jump a
โœ A.S. Verkman; James A. Dix; A.A. Pandiscio ๐Ÿ“‚ Article ๐Ÿ“… 1981 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 430 KB

A stopped-flow temperature-jump apparatus that has been used to extend the capabilities of a temperature-jump apparatus described previously (Verkman et al., Anal. Biochem. 102, 189-195, 1980) is described. The observation cell is a single cylinder made from ultraviolettransmitting Lucite. Stainless

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A fast up-and-down temperature-jump apparatus whose dead time is about 60 ms was constructed. The principle of the method is to let the sample solution flow to the observation cell through a capillary in a heat-exchange chamber. Bubbling and cavitation effects in the observation cell at large up or