1982
DOI: 10.1103/physrevc.26.149
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Three-component fluid dynamics for the description of energetic heavy-ion reactions

Abstract: The nucleons taking part in heavy ion reaction are considered as a three-component fluid. The first and second components correspond to the nucleons of the target and the projectile, while the thermalized nucleons produced in the Course of the collision belong to the third component. Making use of the Boltzmann equation, hydrodynamical equations are derived. An equation of state for anisotropic nuclear matter obtained from a field theoretical model in mean field approximation is applied in a one dimensional ve… Show more

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Cited by 37 publications
(15 citation statements)
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“…The inclusion of dissipative processes between the components in the three component model allows to give up the simplifying assumption of former three component models [17,18] where it is assumed that a nucleon of component one or two populating the thermalized matter component carries off all its energy and momentum 9 As a consequence of the above assumption the components of projectile and target in the earlier three component model moved with constant velocity and fixed temperature disregarding recoil effects due to the interpenetration of the nuclei 9…”
Section: (47)mentioning
confidence: 99%
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“…The inclusion of dissipative processes between the components in the three component model allows to give up the simplifying assumption of former three component models [17,18] where it is assumed that a nucleon of component one or two populating the thermalized matter component carries off all its energy and momentum 9 As a consequence of the above assumption the components of projectile and target in the earlier three component model moved with constant velocity and fixed temperature disregarding recoil effects due to the interpenetration of the nuclei 9…”
Section: (47)mentioning
confidence: 99%
“…These components can be arbitrarily defined, but their sum should yield the total momentum distribution of a particle species [17] N f(x, p)= ~ fk(x, Pk). (13 k=l Thus conservation laws are in general not existing for the components separately.…”
Section: Basic Equations Of the Multicomponent Transport Theorymentioning
confidence: 99%
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“…This idea was further developed in [3,7,15]. In [16] a non-relativistic three-fluid model was developed, introducing a third thermalized fluid of stopped baryons. Depending on the strength of the interaction between the target and projectile fluids this model contains the one-fluid model (strong coupling) as well as the two-fluid model (weak coupling) as limiting cases.…”
Section: Introductionmentioning
confidence: 99%