2022
DOI: 10.1016/j.actamat.2022.118374
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A combined thermal desorption spectroscopy and internal friction study on the interaction of hydrogen with microstructural defects and the influence of carbon distribution

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Cited by 10 publications
(2 citation statements)
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“…2e, details in Supplementary Method section). These values correspond to the theoretically determined activation energies for (1) hydrogen desorbed from the body-centered cubic iron lattice 33,34 and hydrogen release from surface iron hydroxides; (2) high-angle grain boundaries and dislocations (constituting the low-angle grain boundaries) 35,36 ; (3) nano-pore and iron oxide (Fe 3 O 4 ) 28,37 ; and (4) remaining gangue inclusions (e.g. SiO 2 , Al 2 O 3 , etc.)…”
supporting
confidence: 71%
“…2e, details in Supplementary Method section). These values correspond to the theoretically determined activation energies for (1) hydrogen desorbed from the body-centered cubic iron lattice 33,34 and hydrogen release from surface iron hydroxides; (2) high-angle grain boundaries and dislocations (constituting the low-angle grain boundaries) 35,36 ; (3) nano-pore and iron oxide (Fe 3 O 4 ) 28,37 ; and (4) remaining gangue inclusions (e.g. SiO 2 , Al 2 O 3 , etc.)…”
supporting
confidence: 71%
“…They report activation energies up to 42 kJ/mol directly at the dislocation core. To release hydrogen trapped at grain boundaries, an activation energy very similar to dislocations, which is specified to lie between 17 and 33 kJ/mol [19,37,43,44], is needed. For the activation energy of hydrogen trapped at the ferrite/Fe 3 C interface, it has to be clearly distinguished between the level of strain which was applied to the material because, in unstrained pearlitic steels, the ferrite/Fe 3 C interface shows activation energies between 23.5 and 31 kJ/mol [40,45,46].…”
Section: Thermal Desorption Spectroscopymentioning
confidence: 99%