Abstract
Data on the hydrogen isotopes (H, D) yield of Pd with linear heating: a) by the accelerated electrons beam with energy up to 35 KeV, b) by joule heat of AC (50 Hz) through samples, c) by external coaxial metal furnace (stainless steel), d) in quartz vacuum cell are presented and e) UV stimulation during thermal heating (the research article [2]).The highest temperature position of the maximum hydrogen isotopes intensity release corresponds to the samples heating in a metal vacuum cell by external coaxial furnace. The lowest temperature position of the maximum intensity hydrogen isotopes release corresponds to the heating by accelerated electrons beam. The difference in these positions of the maximum is ΔТ ≈ 300°С. Shift of maxima position in the hydrogen and deuterium release into the low-temperature region is significant (ΔТ ≈ 50–100°С) for the Pd sample when metal are heated by electric current or in a quartz vacuum cell compared to their heating in a metal vacuum cell and under UV stimulation during thermal heating.
Highlights
Data on the hydrogen isotopes (H, D) yield of Pd with linear heating: a) by the accelerated electrons beam with energy up to 35 KeV, b) by joule heat of AC (50 Hz) through samples, c) by external coaxial metal furnace, d) in quartz vacuum cell are presented and e) ultraviolet light (UV) stimulation during thermal heating
For the Pd sample when metal are heated by electric current or in a quartz vacuum cell compared to their heating in a metal vacuum cell and under UV stimulation during thermal heating
It is important to create hydrogen storage devices and develop methods for accelerating physical processes at interphase boundaries in metal e hydrogen systems [1]. This brief article describes the data upon the stimulation hydrogen isotopes (H,D) yield from Pd at equilibrium and non-equilibrium heating of the samples with help: a) external coaxial furnace, b) the Joule's heat of electric current, c) accelerated electrons beam, d) weak electromagnetic fields and e) UV stimulation during thermal heating
Summary
Physics Hydrogenesolid state matter systems under external influence text file, graph A plant for studying radiation and thermal desorption of gases from inorganic materials. It is important to create hydrogen storage devices and develop methods for accelerating physical processes at interphase boundaries in metal e hydrogen systems [1] This brief article describes the data upon the stimulation hydrogen isotopes (H,D) yield from Pd at equilibrium and non-equilibrium heating of the samples with help: a) external coaxial furnace, b) the Joule's heat of electric current, c) accelerated electrons beam, d) weak electromagnetic fields and e) UV stimulation during thermal heating. Analytical approximations indicate possible mechanisms for stimulating radiation, UV and dynamic electromagnetic processes (curve 40, Fig. 1a) [2]
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