On the algebraic structure of particle motion in a field of turbulence

Summary The motion of particles in a turbulent flow is described by means of algebraic physics. The initial concepts are structurally ordered groupoids, algebras of observables, logically dependent on them, with couplings and the non-canonic transition between two Hamiltonians. The non-canonic transition leads to the substitution of time t by a new parameter. Its real counterpart gives the lower limit of the size of the time step in the differential equation of transfer, based on the semi-empirical image of turbulent diffusion.

---

uu amu mm muu nua ¶rt;mau aau uuu. ¶rt;u nmuu m mm n¶rt;nnu¶rt;, uu m u auu a a¶rt;a u u auu n¶rt; ¶rt; ¶rt;aumuaau. auu n¶rt; nu¶rt;um a u t naam. ¶rt;mum aa n¶rt;m uau aa am au na, nua a nnuu au mm ¶rt;uuu.