Busca avançada
Ano de início
Entree
(Referência obtida automaticamente do Web of Science, por meio da informação sobre o financiamento pela FAPESP e o número do processo correspondente, incluída na publicação pelos autores.)

Hydrodynamics of two-dimensional compressible fluid with broken parity: Variational principle and free surface dynamics in the absence of dissipation

Texto completo
Autor(es):
Abanov, Alexander G. [1, 2] ; Can, Tankut [3] ; Ganeshan, Sriram [4] ; Monteiro, Gustavo M. [5, 6]
Número total de Autores: 4
Afiliação do(s) autor(es):
[1] SUNY Stony Brook, Dept Phys & Astron, Stony Brook, NY 11794 - USA
[2] Simons Ctr Geometry & Phys, Stony Brook, NY 11794 - USA
[3] CUNY, Grad Ctr, Initiat Theoret Sci, New York, NY 10012 - USA
[4] CUNY City Coll, Dept Phys, New York, NY 10031 - USA
[5] Univ Estadual Campinas, Inst Fis Gleb Wataghin, UNICAMP, BR-13083859 Campinas, SP - Brazil
[6] Int Inst Phys, Campus Univ Lagoa Nova, BR-59078970 Natal, RN - Brazil
Número total de Afiliações: 6
Tipo de documento: Artigo Científico
Fonte: PHYSICAL REVIEW FLUIDS; v. 5, n. 10 OCT 21 2020.
Citações Web of Science: 0
Resumo

We consider an isotropic compressible nondissipative fluid with broken parity subject to free surface boundary conditions in two spatial dimensions. The hydrodynamic equations describing the bulk dynamics of the fluid and the free surface boundary conditions depend explicitly on the parity-breaking nondissipative odd viscosity term. We construct an effective action which gives both bulk hydrodynamic equations and free surface boundary conditions. The free surface boundary conditions require an additional boundary term in the action which resembles a 1 + 1D chiral boson field coupled to the background geometry. We solve the linearized hydrodynamic equations for the deep water case and derive the dispersion of chiral surface waves. We show that in the long-wavelength limit the flow profile exhibits an oscillating vortical boundary layer near the free surface. The layer thickness is controlled by the ratio between the odd viscosity (nu(o)) and the sound velocity (c(s)), delta similar to nu(o)/c(s). In the incompressible limit, c(s) -> infinity, the vortical boundary layer becomes singular with the vorticity within the layer diverging as omega similar to c(s). The boundary layer is formed by odd viscosity coupling the divergence of velocity del center dot nu to vorticity del x nu. It results in nontrivial chiral free surface dynamics even in the absence of external forces. The structure of the odd-viscosity-induced boundary layer is very different from the conventional free surface boundary layer associated with dissipative shear viscosity. (AU)

Processo FAPESP: 16/13517-0 - Propriedades topológicas e de transporte em materiais quirais
Beneficiário:Gustavo Machado Monteiro
Modalidade de apoio: Bolsas no Brasil - Pós-Doutorado