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Ya.B. Zel’dovich and Yu.P. Raizer, The Physics of Shock Waves and High Temperature Hydrodynamic Phenomena (Academic, New York, 1967).
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Bufetov, I.A.1
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10
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85036146032
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Alternatively, one obtains a nonlinear diffusion equation for the gas density, (Formula presented), with the effective diffusion coefficient decreasing with (Formula presented). This equation appeared in a number of nonlinear diffusion problems where (Formula presented) decays at (Formula presented) 17. In the hot bubble problem (Formula presented) at (Formula presented), and this difference results in quite a different dynamics
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Alternatively, one obtains a nonlinear diffusion equation for the gas density, (Formula presented), with the effective diffusion coefficient decreasing with (Formula presented). This equation appeared in a number of nonlinear diffusion problems where (Formula presented) decays at (Formula presented) 17. In the hot bubble problem (Formula presented) at (Formula presented), and this difference results in quite a different dynamics.
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12
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85036269777
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The heat flux (Formula presented) should be continuous. For (Formula presented) it implies (Formula presented)
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The heat flux (Formula presented) should be continuous. For (Formula presented) it implies (Formula presented).
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13
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85036325554
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Shrinking is possible when a cold “cloud” is heated by a hot and underdense peripheral gas. A problem mathematically equivalent to this one was considered in Ref. 17
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Shrinking is possible when a cold “cloud” is heated by a hot and underdense peripheral gas. A problem mathematically equivalent to this one was considered in Ref. 17.
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14
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85036187702
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reality, the temperature should approach a finite value at large distances. Correspondingly, the solution we are interested in represents an intermediate asymptotics 2
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In reality, the temperature should approach a finite value at large distances. Correspondingly, the solution we are interested in represents an intermediate asymptotics 2.
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15
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85036266985
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If (Formula presented) is a solution of Eq. (3), then (Formula presented) is also a solution for any (Formula presented). This property enables one to restore the k dependence in the final results
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If (Formula presented) is a solution of Eq. (3), then (Formula presented) is also a solution for any (Formula presented). This property enables one to restore the k dependence in the final results.
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16
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0004149831
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Cambridge University Press, Cambridge, England
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S. Wolfram, The Mathematica Book, 3rd ed. (Cambridge University Press, Cambridge, England, 1996).
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The Mathematica Book, 3rd ed.
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Wolfram, S.1
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