Abstract
Abstract
This paper exposes how to obtain a relation that have to be hold for all free-divergence velocity fields that evolve according to Navier–Stokes equations. However, checking the violation of this relation requires a huge computational effort. To circumvent this problem it is proposed an additional ansatz to free-divergence Navier–Stokes fields. This makes available six degrees of freedom which can be tuned. When they are tuned adequately, it is possible to find finite L
2 norms of the velocity field for volumes of
R
3
and for
t
∈
[
t
0
,
∞
)
. In particular, the kinetic energy of the system is bounded when the field components u
i
are class C
3 functions on
R
3
×
[
t
0
,
∞
)
that hold Dirichlet boundary conditions. This additional relation lets us conclude that Navier–Stokes equations with no-slip boundary conditions have not unique solution. Moreover, under a given external force the kinetic energy can be computed exactly as a funtion of time.
Subject
General Physics and Astronomy
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