Paley–Zygmund inequality: Difference between revisions
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'''Computational magnetohydrodynamics (CMHD)''' is a rapidly developing branch of [[magnetohydrodynamics]] that uses [[numerical method]]s and algorithms to solve and analyze problems that involve electrically conducting fluids. Most of the methods used in CMHD are borrowed from the well established techniques employed in [[Computational fluid dynamics]]. The complexity mainly arises due to the presence of a [[magnetic field]] and its coupling with the fluid. One of the important issues is to numerically maintain the <math> \nabla \cdot {\mathbf B} = 0</math> (conservation of magnetic flux) condition, from [[Maxwell's equations]], to avoid any unphysical effects. | |||
==See also== | |||
* [[Magnetohydrodynamic turbulence]] | |||
* [[Magnetic flow meter]] | |||
==References== | |||
* Brio, M., Wu, C. C.(1988), "An upwind differencing scheme for the equations of ideal magnetohydrodynamics", ''Journal of Computational Physics'', '''75''', 400–422. | |||
* Henri-Marie Damevin and Klaus A. Hoffmann(2002), "Development of a Runge-Kutta Scheme with TVD for Magnetogasdynamics", ''Journal of Spacecraft and Rockets'', '''34''',No.4, 624–632. | |||
* Robert W. MacCormack(1999), "An upwind conservation form method for ideal magnetohydrodynamics equations", ''AIAA-99-3609''. | |||
* Robert W. MacCormack(2001), "A conservation form method for magneto-fluid dynamics", ''AIAA-2001-0195''. | |||
==Further reading== | |||
* Toro, E. F. (1999), ''Riemann Solvers and Numerical Methods for Fluid Dynamics'', Springer-Verlag. | |||
==External links== | |||
[http://www.ncbi.nlm.nih.gov/pmc/articles/PMC392293/ NCBI] | |||
{{fluiddynamics-stub}} | |||
[[Category:Numerical analysis]] | |||
Revision as of 22:11, 1 January 2014
Computational magnetohydrodynamics (CMHD) is a rapidly developing branch of magnetohydrodynamics that uses numerical methods and algorithms to solve and analyze problems that involve electrically conducting fluids. Most of the methods used in CMHD are borrowed from the well established techniques employed in Computational fluid dynamics. The complexity mainly arises due to the presence of a magnetic field and its coupling with the fluid. One of the important issues is to numerically maintain the (conservation of magnetic flux) condition, from Maxwell's equations, to avoid any unphysical effects.
See also
References
- Brio, M., Wu, C. C.(1988), "An upwind differencing scheme for the equations of ideal magnetohydrodynamics", Journal of Computational Physics, 75, 400–422.
- Henri-Marie Damevin and Klaus A. Hoffmann(2002), "Development of a Runge-Kutta Scheme with TVD for Magnetogasdynamics", Journal of Spacecraft and Rockets, 34,No.4, 624–632.
- Robert W. MacCormack(1999), "An upwind conservation form method for ideal magnetohydrodynamics equations", AIAA-99-3609.
- Robert W. MacCormack(2001), "A conservation form method for magneto-fluid dynamics", AIAA-2001-0195.
Further reading
- Toro, E. F. (1999), Riemann Solvers and Numerical Methods for Fluid Dynamics, Springer-Verlag.