On \(q\)-Gaussian integrable Hamiltonian reductions in anisentropic magneto-gasdynamics
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Publication:404888
DOI10.1007/s10440-014-9926-8zbMath1304.76050OpenAlexW1978746733MaRDI QIDQ404888
Colin Rogers, Wolfgang K. Schief
Publication date: 4 September 2014
Published in: Acta Applicandae Mathematicae (Search for Journal in Brave)
Full work available at URL: https://doi.org/10.1007/s10440-014-9926-8
PDEs in connection with fluid mechanics (35Q35) Gas dynamics (general theory) (76N15) Magnetohydrodynamics and electrohydrodynamics (76W05)
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Cites Work
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- Multi-component Ermakov systems: Structure and linearization
- The pulsrodon in 2+1-dimensional magneto-gasdynamics: Hamiltonian structure and integrability
- Ermakov-Ray-Reid Systems in (2+1)-Dimensional Rotating Shallow Water Theory
- Ermakov–Ray–Reid systems in nonlinear optics
- Generalised Thermostatistics
- On the integrability of a Hamiltonian reduction of a 2+1-dimensional non-isothermal rotating gas cloud system
- Group theoretical analysis of a rotating shallow liquid in a rigid container
- Introduction to Nonextensive Statistical Mechanics
- Spinning gas clouds with precession: a new formulation
- Ermakov systems, nonlinear superposition, and solutions of nonlinear equations of motion
- Ermakov systems of arbitrary order and dimension: structure and linearization
- On (2+1)-dimensional Ermakov systems
- A class of accelerated solutions of the two–dimensional ideal magnetohydrodynamic equations
- Elliptical vortices and integrable Hamiltonian dynamics of the rotating shallow-water equations
- Ermakov–Ray–Reid Reductions of Variational Approximations in Nonlinear Optics
- Universal and Integrable Aspects of an Elliptic Vortex Representation in 2+1‐Dimensional Magneto‐Gasdynamics
- Some general theorems concerning the finite motion of a shallow rotating liquid lying on a paraboloid
- The nonlinear differential equation 𝑦”+𝑝(𝑥)𝑦+𝑐𝑦⁻³=0
