Abstract

We study the three-dimensional forced–dissipated Gross–Pitaevskii equation. We force at relatively low wave numbers, expecting to observe a direct energy cascade and a consequent power-law spectrum of the form k − α . Our numerical results show that the exponent α strongly depends on how the inverse particle cascade is attenuated at k s lower than the forcing wave-number. If the inverse cascade is arrested by a friction at low k s, we observe an exponent which is in good agreement with the weak wave turbulence prediction k − 1 . For a hypo-viscosity, a k − 2 spectrum is observed which we explain using a critical balance argument. In simulations without any low k dissipation, a condensate at k = 0 is growing and the system goes through a strongly turbulent transition from a 4-wave to a 3-wave weak turbulence acoustic regime with evidence of k − 3 / 2 Zakharov–Sagdeev spectrum. In this regime, we also observe a spectrum for the incompressible kinetic energy which formally resembles the Kolmogorov k − 5 / 3 , but whose correct explanation should be in terms of the Kelvin wave turbulence. The probability density functions for the velocities and the densities are also discussed.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.