Abstract
This work develops a new monolithic strategy for magnetohydrodynamics based on a continuous velocity–pressure formulation. The magnetic field is interpolated in the same way as the velocity field, and the entire formulation is within a nodal finite-element framework. The velocity and pressure interpolations are chosen so that they satisfy the Babuska–Brezzi (BB) conditions. In most of the existing formulations, a stabilized formulation is used that requires a stabilization term, and some associated mesh-dependent parameters that need to be adjusted. In contrast, no such parameters need to be adjusted in the current formulation, making it more user-friendly and robust. Both transient and steady-state formulations are developed for two- and three-dimensional geometries. An exact linearization of the monolithic strategy ensures that rapid (quadratic) convergence is achieved within each time (or load) step, while the stable nature of the interpolations used ensures that no instabilities arise in the solution. An existing analytical solution is corrected. The coarse mesh accuracy is shown to be better compared with other existing strategies in several benchmark problems, showing that the developed formulation is both robust and efficient.
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Abbreviations
- \(\alpha \) :
-
parameter in the generalized trapezoidal rule
- \({\varvec{b}}\) :
-
body force per unit mass
- \({{\varvec{B}}}\) :
-
magnetic induction
- \({\mathbb {C}}\) :
-
material constitutive tensor
- \({\varvec{D}}\) :
-
electric displacement
- \({\varvec{D}}_c\) :
-
rate of deformation tensor
- \({\varvec{E}}\) :
-
electric field
- \(\epsilon \) :
-
electric permittivity
- \(\epsilon _0, \epsilon _r\) :
-
\(\epsilon \) of vacuum, relative \(\epsilon \)
- \(\Gamma \) :
-
boundary
- \({{\mathrm{Ha}}}\) :
-
Hartman number
- \({\varvec{H}}\) :
-
magnetic field
- \({\varvec{j}}\) :
-
current density
- \(\mu \) :
-
magnetic permeability
- \(\mu _0\), \(\mu _r\) :
-
\(\mu \) of vacuum, relative \(\mu \)
- \(\mu _{\nu }\) :
-
fluid dynamic viscosity
- \({\varvec{n}}\) :
-
unit normal vector
- \(\nu \) :
-
kinematic viscosity
- \(\varOmega \) :
-
domain
- p :
-
fluid pressure
- \({\mathrm {Re}}\) :
-
Reynolds number
- \({\mathrm {Re}}_{\mathrm{m}}\) :
-
magnetic Reynolds number
- \(\rho \) :
-
fluid density
- \(\rho _c\) :
-
charge density
- \(\sigma \) :
-
conductivity
- t :
-
time
- \({\varvec{t}}\) :
-
traction vector acting on the surface
- \(t_{\Delta }\) :
-
time step in the transient strategy
- \({\varvec{\tau }}\) :
-
Cauchy stress tensor
- \({\varvec{u}}\) :
-
fluid velocity
- \(\dot{<\_>}\) :
-
Derivative of \(<\_>\) with respect to time
- \(\hat{<\_>}\) :
-
Discretized nodal values of \(<\_>\)
- \(<\_>_{\delta }\) :
-
Variation of \(<\_>\)
- \(<\_>_{\Delta }\) :
-
Increment of \(<\_>\)
- \(<\_>^{n}\) :
-
\(<\_>\) at time \(t_n\)
- \(<\_>^{k}\) :
-
\(<\_>\) at \(k^{\mathrm{th}}\) iteration at time \(t_{n+1}\)
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Nandy, A., Jog, C.S. A monolithic finite-element formulation for magnetohydrodynamics. Sādhanā 43, 151 (2018). https://doi.org/10.1007/s12046-018-0905-z
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DOI: https://doi.org/10.1007/s12046-018-0905-z