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Potential of mean force for electrical conductivity of dense plasmas

Journal Article · · High Energy Density Physics
The electrical conductivity in dense plasmas can be calculated with the relaxation-time approximation provided that the interaction potential between the scattering electron and the ion is known. To date there has been considerable uncertainty as to the best way to define this interaction potential so that it correctly includes the effects of ionic structure, screening by electrons and partial ionization. The current approximations lead to significantly different results with varying levels of agreement when compared to bench-mark calculations and experiments. Here, we present a new way to define this potential, drawing on ideas from classical fluid theory to define a potential of mean force. This new potential results in significantly improved agreement with experiments and bench-mark calculations, and includes all the aforementioned physics self-consistently.
Research Organization:
Los Alamos National Laboratory (LANL)
Sponsoring Organization:
USDOE
Grant/Contract Number:
AC52-06NA25396
OSTI ID:
1396133
Alternate ID(s):
OSTI ID: 1549230
Report Number(s):
LA-UR-17-26365
Journal Information:
High Energy Density Physics, Journal Name: High Energy Density Physics Vol. 25; ISSN 1574-1818
Publisher:
ElsevierCopyright Statement
Country of Publication:
United States
Language:
English

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Cited By (4)

Model for the electrical conductivity in dense plasma mixtures journal August 2020
Coulomb log for conductivity of dense plasmas journal September 2018
Theory of the electron-ion temperature relaxation rate spanning the hot solid metals and plasma phases journal October 2019
Correlations between conduction electrons in dense plasmas journal January 2020

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