Electrostatic Shock Structures in a Magnetized Plasma Having Non-Thermal Particles
Abstract
:1. Introduction
2. Governing Equations
3. Derivation of Burgers’ Equation
4. Numerical Analysis and Discussion
5. Conclusions
- The negative (positive) shock profile can exist for the value of ().
- The steepness of both positive and negative shock profiles declines with the increase of without affecting the height.
- The increase in oblique angle raises the height of the positive shock profile.
- The height of the positive shock wave increases with the number density of positron.
- The amplitude of the positive shock profile increases (decreases) with increasing the value of positive (negative) ion mass.
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Acknowledgments
Conflicts of Interest
References
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Jahan, S.; Banik, S.; Chowdhury, N.A.; Mannan, A.; Mamun, A.A. Electrostatic Shock Structures in a Magnetized Plasma Having Non-Thermal Particles. Gases 2022, 2, 22-32. https://doi.org/10.3390/gases2020002
Jahan S, Banik S, Chowdhury NA, Mannan A, Mamun AA. Electrostatic Shock Structures in a Magnetized Plasma Having Non-Thermal Particles. Gases. 2022; 2(2):22-32. https://doi.org/10.3390/gases2020002
Chicago/Turabian StyleJahan, Sharmin, Subrata Banik, Nure Alam Chowdhury, Abdul Mannan, and A A Mamun. 2022. "Electrostatic Shock Structures in a Magnetized Plasma Having Non-Thermal Particles" Gases 2, no. 2: 22-32. https://doi.org/10.3390/gases2020002