Neutron Yield Enhancement Through Gas Admixture and Cathode Radius Variation in a Plasma Focus Device

This study investigates the complex relationship between different cathode radii (<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</i>) and neutron yield (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula>), for the 2.73-kJ United Nations University/International Centre for Theoretical Physics Plasma Fusion Facility (UNU/ICTP PFF) plasma focus (PF) device when gas admixtures are introduced. The Lee model code is applied to characterize the UNU/ICTP PFF and for optimizing deuterium and argon (D:Ar) neutron production. The latest codes revealed how varying cathode radii and gas admixtures affect <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula> and plasma dynamics. The maximum computed <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula> generated per shot is <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$2.42\times 10^{7}$</tex-math> </inline-formula> n with beam energy of 80.7 kJ at a gas admixture weight ratio of ca. 19% and the pure D counterpart produced <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$9.57\times 10^{6}$</tex-math> </inline-formula> n with a beam energy of 68.97 kJ, both corresponding to 2.0-cm cathode radii. This shows a significant increase of ca. 153%. The study revealed that <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{\mathrm {th}}$</tex-math> </inline-formula> made a negligible contribution to the total <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula>. The pinch lifetime increases with increasing proportion of Ar gas. As the Ar weight ratio increases, the overall mass of the plasma increases, due to heavier Ar atoms.

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Journal
IEEE Transactions on Plasma Science
Published
2025-05-19
DOI
https://doi.org/10.1109/tps.2025.3565331
Primary Topic
Laser-Plasma Interactions and Diagnostics
Type
article
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article

Neutron Yield Enhancement Through Gas Admixture and Cathode Radius Variation in a Plasma Focus Device

S. L. Yap, Haiyun Tan, L. MUHAMMAD, Haruna P. Wante et al.
IEEE Transactions on Plasma Science
Laser-Plasma Interactions and Diagnostics
article

Neutron Yield Enhancement Through Gas Admixture and Cathode Radius Variation in a Plasma Focus Device

S. L. Yap, Haiyun Tan, L. MUHAMMAD, Haruna P. Wante, S. Lee, L. K. Lim
article en

Abstract

This study investigates the complex relationship between different cathode radii (<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">b</i>) and neutron yield (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula>), for the 2.73-kJ United Nations University/International Centre for Theoretical Physics Plasma Fusion Facility (UNU/ICTP PFF) plasma focus (PF) device when gas admixtures are introduced. The Lee model code is applied to characterize the UNU/ICTP PFF and for optimizing deuterium and argon (D:Ar) neutron production. The latest codes revealed how varying cathode radii and gas admixtures affect <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula> and plasma dynamics. The maximum computed <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula> generated per shot is <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$2.42\times 10^{7}$</tex-math> </inline-formula> n with beam energy of 80.7 kJ at a gas admixture weight ratio of ca. 19% and the pure D counterpart produced <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$9.57\times 10^{6}$</tex-math> </inline-formula> n with a beam energy of 68.97 kJ, both corresponding to 2.0-cm cathode radii. This shows a significant increase of ca. 153%. The study revealed that <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{\mathrm {th}}$</tex-math> </inline-formula> made a negligible contribution to the total <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$Y_{n}$</tex-math> </inline-formula>. The pinch lifetime increases with increasing proportion of Ar gas. As the Ar weight ratio increases, the overall mass of the plasma increases, due to heavier Ar atoms.

IEEE Transactions on Plasma ScienceVol. 53(7)
University of Malaya (MY)
Ministry of Higher Education, Malaysia
Affordable and clean energy
Openalex Percentile: Top 95%
Laser-Plasma Interactions and Diagnostics
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