activity
20052007
most citedMorphology of flows and buoyant bubbles in the Virgo cluster

20 citations · 22 across the 3 of their papers we have counts for

collaborators

7 papers

astro-ph200720 cited

Morphology of flows and buoyant bubbles in the Virgo cluster

Georgi Pavlovski, Christian R. Kaiser, Edward C. D. Pope +1

There is growing evidence that the active galactic nuclei (AGN) associated with the central elliptical galaxy in clusters of galaxies are playing an important role in the evolution…

astro-ph20072 cited

Dynamics of buoyant bubbles in clusters of galaxies

Georgi Pavlovski, Christian R. Kaiser, Edward C. D. Pope

We present a phenomenological model of the dynamics of buoyant bubbles in the atmosphere of a cluster of galaxies. The derived equations describe velocity, size, mass, temperature…

astro-ph2007

Heating rate profiles in clusters of galaxies

Edward Pope, Christian Kaiser, Georgi Pavlovski +1

The results of hydrodynamic simulations of the Virgo and Perseus clusters suggest that thermal conduction is not responsible for the observed temperature and density profiles. As a…

astro-ph2006

Heating Rate Profiles in Galaxy Clusters

Edward C. D. Pope, Georgi Pavlovski, Christian R. Kaiser +1

In recent years evidence has accumulated suggesting that the gas in galaxy clusters is heated by non-gravitational processes. Here we calculate the heating rates required to mainta…

astro-ph2005

The Effect of Thermal Conduction on the Virgo Cluster

Edward C. D. Pope, Georgi Pavlovski, Christian R. Kaiser +1

Thermal conduction has been suggested as a possible mechanism by which sufficient energy is supplied to the central regions of galaxy clusters to balance the effect of radiative co…

astro-ph2005

Hydrodynamical simulations of the decay of high-speed molecular turbulence. II. Divergence from isothermality

G. Pavlovski, M. D. Smith, M. -M. Mac Low

A roughly constant temperature over a wide range of densities is maintained in molecular clouds through radiative heating and cooling. An isothermal equation of state is therefore…