2+1 dimensional hydrodynamics including bulk viscosity: a systematics study
arXiv:1109.1630 · doi:10.1103/PhysRevC.85.024909
Abstract
We have studied the effect of nonzero bulk viscosity with peak near the lattice QCD predicted crossover temperature on charged particle transverse momentum spectra and elliptic flow. The Israel-Stewart theory of 2nd order causal dissipative relativistic fluid dynamics is used to simulate the space time evolution of the matter formed in Au-Au collisions at =200 GeV assuming longitudinal boost invariance. A systematic comparison of temperature, transverse velocity, spatial and momentum anisotropy evolution of the ideal, bulk and shear viscous fluid has been carried out. Two different temperature dependent forms of and a constant was used. Both the bulk and shear viscous correction to the ideal freezeout distribution function are included. The dissipative correction to the freezeout distribution for bulk viscosity was calculated using Grad's fourteen moment method. From our simulation we show that the method is applicable only for for freezeout temperatures 130 and 160 MeV.
14pages, 26 figures, accepted for publication in Phys. Rev. C
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Cited by in corpus (12)
- Bulk Viscosity Effects in Event-by-Event Relativistic Hydrodynamics
- Relativistic hydrodynamics in heavy-ion collisions: general aspects and recent developments
- Relativistic second-order dissipative hydrodynamics at finite chemical potential
- Investigation of Heat Conductivity in Relativistic Systems using a Partonic Cascade
- Comparison of results from a 2+1D relativistic viscous hydrodynamic model to elliptic and hexadecapole flow of charged hadrons measured in Au-Au collisions at = 200 GeV
- A new scheme of causal viscous hydrodynamics for relativistic heavy-ion collisions: A Riemann solver for quark-gluon plasma
- A new relativistic viscous hydrodynamics code and its application to the Kelvin-Helmholtz instability in high-energy heavy-ion collisions
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- Formulation of relativistic dissipative fluid dynamics and its applications in heavy-ion collisions