Turbulent gas motions in galaxy cluster simulations: the role of smoothed particle hydrodynamics viscosity

Smoothed particle hydrodynamics (SPH) employs an artificial viscosity to properly capture hydrodynamic shock waves. In its original formulation, the resulting numerical viscosity is large enough to suppress structure in the velocity field on scales well above the nominal resolution limit, and to damp the generation of turbulence by fluid instabilities. This could artificially suppress random gas motions in the intracluster medium (ICM), which are driven by infalling structures during the hierarchical structure formation process. We show that this is indeed the case by analysing results obtained with an SPH formulation where an individual, time-variable viscosity is used for each particle, following a suggestion by Morris & Monaghan. Using test calculations involving strong shocks, we demonstrate that this scheme captures shocks as well as the original formulation of SPH, but, in regions away from shocks, the numerical viscosity is much smaller. In a set of nine high-resolution simulations of cosmological galaxy cluster formation, we find that this low-viscosity formulation of SPH produces substantially higher levels of turbulent gas motions in the ICM, reaching a kinetic energy content in random gas motions (measured within a 1-Mpc cube) of up to 5‐30 per cent of the thermal energy content, depending on cluster mass. This also has significant effects on radial gas profiles and bulk cluster properties. We find a central flattening of the entropy profile and a reduction of the central gas density in the low-viscosity scheme. As a consequence, the bolometric X-ray luminosity is decreased by about a factor of 2. However, the cluster temperature profile remains essentially unchanged. Interestingly, this tends to reduce the differences seen in SPH and adaptive mesh refinement simulations of cluster formation. Finally, invoking a model for particle acceleration by magnetohydrodynamics waves driven by turbulence, we find that efficient electron acceleration and thus diffuse radio emission can be powered in the clusters simulated with the low-viscosity scheme provided that more than 5‐10 per cent of the turbulent energy density is associated with fast magneto-sonic modes.

[1]  G. Sod A survey of several finite difference methods for systems of nonlinear hyperbolic conservation laws , 1978 .

[2]  On the detectability of turbulence and bulk flows in X-ray clusters , 2003, astro-ph/0310041.

[3]  M. Steinmetz,et al.  The Santa Barbara Cluster Comparison Project: A Comparison of Cosmological Hydrodynamics Solutions , 1999, astro-ph/9906160.

[4]  D. Melrose The emission and absorption of waves by charged particles in magnetized plasmas , 1968 .

[5]  J. Burns,et al.  Numerical Simulations of Merging Clusters of Galaxies , 1997 .

[6]  R. Bender,et al.  New Light on Galaxy Evolution , 1996 .

[7]  Cluster mergers and non‐thermal phenomena: a statistical magneto‐turbulent model , 2005 .

[8]  G. Giovannini,et al.  Merging processes in galaxy clusters , 2002 .

[9]  Magnetic Field Evolution in Merging Clusters of Galaxies , 1999, astro-ph/9902105.

[10]  The structure and dynamical evolution of dark matter haloes , 1996, astro-ph/9603132.

[11]  Arnab Rai Choudhuri,et al.  The Physics of Fluids and Plasmas , 1998 .

[12]  J. Monaghan,et al.  A Switch to Reduce SPH Viscosity , 1997 .

[13]  S. White,et al.  X-ray archaeology in the coma cluster , 1993 .

[14]  Joseph John Monaghan,et al.  SPH and Riemann Solvers , 1997 .

[15]  Radio halo and relic candidates from the NRAO VLA Sky Survey , 1999, astro-ph/9904210.

[16]  S. Gabici,et al.  Alfvénic reacceleration of relativistic particles in galaxy clusters: MHD waves, leptons and hadrons , 2003, astro-ph/0312482.

[17]  J. Monaghan,et al.  Shock simulation by the particle method SPH , 1983 .

[18]  V. Springel,et al.  GADGET: a code for collisionless and gasdynamical cosmological simulations , 2000, astro-ph/0003162.

[19]  Jeffrey D. Scargle,et al.  Collisionless damping of hydromagnetic waves in relativistic plasma. I. Weak Landau damping: heating of the Crab Nebula , 1973 .

[20]  L. Moscardini,et al.  Comparing the temperatures of galaxy clusters from hydrodynamical N-body simulations to Chandra and XMM-Newton observations , 2004, astro-ph/0404425.

[21]  V. Springel,et al.  Cosmological smoothed particle hydrodynamics simulations: the entropy equation , 2001, astro-ph/0111016.

[22]  Non-Gaussian cosmic microwave background temperature fluctuations from peculiar velocities of clusters , 2001, astro-ph/0104332.

[23]  U. Virginia,et al.  Radio Halo Formation through Magnetoturbulent Particle Acceleration in Clusters of Galaxies , 2002, astro-ph/0206269.

[24]  A. Finoguenov,et al.  Probing turbulence in the Coma galaxy cluster , 2004 .

[25]  D. Buote On the Origin of Radio Halos in Galaxy Clusters , 2001, astro-ph/0104211.

[26]  Lars Hernquist,et al.  Comparing AMR and SPH Cosmological Simulations. I. Dark Matter and Adiabatic Simulations , 2003, astro-ph/0312651.

[27]  G. Bryan,et al.  Cluster Turbulence , 1998, astro-ph/9802335.

[28]  Evolution and structure of magnetic fields in simulated galaxy clusters , 2002, astro-ph/0202272.

[29]  H. Böhringer,et al.  A systematic study of X-ray substructure of galaxy clusters detected in the ROSAT All-Sky Survey ? , 2001, astro-ph/0109030.

[30]  E. Bertschinger The self-similar evolution of holes in an Einstein-de Sitter universe , 1985 .

[31]  G. Giovannini,et al.  Particle reacceleration in the Coma cluster: radio properties and hard X‐ray emission , 2000, astro-ph/0008518.

[32]  Hydrodynamic Simulations of a Moving Substructure in a Cluster of Galaxies: Cold Fronts and Turbulence Generation , 2005, astro-ph/0505274.

[33]  P. Ricker,et al.  Off-Axis Cluster Mergers: Effects of a Strongly Peaked Dark Matter Profile , 2001, astro-ph/0107210.

[34]  C. Sarazin The Energy Spectrum of Primary Cosmic-Ray Electrons in Clusters of Galaxies and Inverse Compton Emission , 1999, astro-ph/9901061.

[35]  Turbulence in clusters of galaxies and X-ray line profiles , 2003, astro-ph/0310737.

[36]  D. Balsara von Neumann stability analysis of smoothed particle hydrodynamics—suggestions for optimal algorithms , 1995 .

[37]  J. Eilek Particle reacceleration in radio galaxies , 1979 .

[38]  Volker Springel,et al.  Cosmological SPH simulations: The entropy equation , 2001 .

[39]  Simulating the metal enrichment of the intracluster medium , 2004, astro-ph/0401576.

[40]  M. Meneghetti,et al.  The impact of gas physics on strong cluster lensing , 2005, astro-ph/0504206.

[41]  L. Moscardini,et al.  Properties of cluster satellites in hydrodynamical simulations , 2003, astro-ph/0304375.

[42]  H. Böhringer,et al.  Matter and energy in clusters of galaxies as probes for galaxy and large-scale structure formation in the universe , 2003 .

[43]  R. Bender,et al.  IAU Symposium 171 New Light on Galaxy Evolution , 1996 .

[44]  Hydrodynamic Interaction of Strong Shocks with Inhomogeneous Media. I. Adiabatic Case , 2001, astro-ph/0109282.