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Journal ArticleDOI

Flow behind magnetogasdynamic exponential shock wave in self-gravitating gas

TLDR
In this article, the effects of variation of ambient magnetic field, gravitational parameter and adiabatic exponent on the propagation of a cylindrical (or spherical) shock wave driven out by a piston moving with time according to an exponential law, in a self-gravitating ideal gas with azimuthal magnetic field is investigated.
Abstract
The propagation of a cylindrical (or spherical) shock wave driven out by a piston moving with time according to an exponential law, in a self-gravitating ideal gas with azimuthal magnetic field is investigated. The initial magnetic field is assumed to be varying according to an exponential law. Solutions are obtained for both the cases of isothermal and adiabatic flows. The effects of variation of ambient magnetic field, gravitational parameter and adiabatic exponent are worked out in detail. It is manifested that the increase in strength of ambient magnetic field has decaying effect on the shock wave however increase in the value of gravitational parameter has reverse effect on the shock strength. The compressibility of the medium is increased in the presence of gravitational field. Also, a comparison between the solutions obtained in the case of isothermal and adiabatic flows is done. Density, pressure, velocity and magnetic field increases, however mass decreases as we move inward from the shock front towards the piston.

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Citations
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Similarity solutions for unsteady flow behind an exponential shock in a self-gravitating non-ideal gas with azimuthal magnetic field

TL;DR: In this paper, the effects of variation of ambient magnetic field, non-idealness of the gas, adiabatic exponent and gravitational parameter are worked out in detail, in both the cases, when the flow between the shock and the piston is isothermal or adiabaatic.
Journal ArticleDOI

Shock wave driven out by a piston in a mixture of a non-ideal gas and small solid particles under the influence of the gravitation field with monochromatic radiation

TL;DR: In this article, similar solutions for a spherical shock wave in a mixture of small solid particles of micro size and a non-ideal gas are discussed under the influence of the gravitational field with monochromatic radiation.
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Approximate analytical solution for shock wave in rotational axisymmetric perfect gas with azimuthal magnetic field: Isothermal flow

TL;DR: In this paper, the propagation of cylindrical shock wave in rotational axisymmetric perfect gas under isothermal flow condition with azimuthal magnetic field is investigated.
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Flow behind an exponential shock in a rotational axisymmetric mixture of non-ideal gas and small solid particles with heat conduction and radiation heat flux

TL;DR: In this paper, a rotational axisymmetric dusty gas with heat conduction and radiation heat flux, which has variable azimuthal and axial fluid velocities, is studied.
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Self-similar solutions of cylindrical shock wave in a dusty gas

TL;DR: In this article, self-similar solutions for one-dimensional unsteady and cylindrically symmetric flow driven by a moving piston in a dusty gas are determined for both types of flows, i.e. isothermal flow and adiabatic flow.
References
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Journal ArticleDOI

Accretion processes in star formation

TL;DR: In this article, the authors provide a comprehensive view of the formation of stars and planetary systems, from their beginnings in cold clouds of molecular gas to their emergence as new suns with planet-forming disks.
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On the propagation of shock waves through regions of non-uniform area or flow

TL;DR: In this paper, it is shown that the results of Moeckel and Chisnell's work can be obtained by the application of a simple rule, which must be satisfied by flow quantities along a characteristic to the flow quantities just behind the shock wave.
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Cylindrical Shock Waves Produced by Instantaneous Energy Release

TL;DR: In this paper, Taylor's analysis of the intense spherical explosion has been extended to the cylindrical case, and it is shown that the radius R of a strong cylinrical shock wave produced by a sudden release of energy E per unit length grows with time t according to the equation R=S(γ)(E/ρ0)1/4t1/2, where ρ0 is the atmospheric density and S(γ) is a calculated function of the specific heat ratio γ.