Master curves for the stress tensor invariants in stationary states of static granular beds. Implications for the thermodynamic phase space

We prepare static granular beds under gravity in different stationary states by tapping the system with pulsed excitations of controlled amplitude and duration. The macroscopic state-defined by the ensemble of static configurations explored by the system tap after tap-for a given tap intensity and d...

ver descrição completa

Detalhes bibliográficos
Autores: Pugnaloni, Luis Ariel, Damas, Jose, Zuriguel, Iker, Maza, Diego
Tipo de documento: artigo
Estado:Versão publicada
Data de publicação:2011
País:Argentina
Recursos:Consejo Nacional de Investigaciones Científicas y Técnicas
Repositório:CONICET Digital (CONICET)
Idioma:inglês
OAI Identifier:oai:ri.conicet.gov.ar:11336/102387
Acesso em linha:http://hdl.handle.net/11336/102387
Access Level:Acceso aberto
Palavra-chave:GRANULAR PACKINGS
https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
Descrição
Resumo:We prepare static granular beds under gravity in different stationary states by tapping the system with pulsed excitations of controlled amplitude and duration. The macroscopic state-defined by the ensemble of static configurations explored by the system tap after tap-for a given tap intensity and duration is studied in terms of volume, V, and force moment tensor, Sigma. In a previous paper [Pugnaloni et al., Phys. Rev. E 82, 050301(R) (2010)], we reported evidence supporting that such macroscopic states cannot be fully described by using only V or Sigma, apart from the number of particles N. In this work, we present an analysis of the fluctuations of these variables that indicates that V and Sigma may be sufficient to define the macroscopic states. Moreover, we show that only one of the invariants of Sigma is necessary, since each component of Sigma falls onto a master curve when plotted as a function of Tr(Sigma). This implies that these granular assemblies have a common shape for the stress tensor, even though it does not correspond to the hydrostatic type. Although most results are obtained by molecular dynamics simulations, we present supporting experimental results.