The pressure candidate for a Leray–Hopf solution #
The velocity tensor, extended by zero outside the time interval, defines the
whole-space Riesz pressure used in thm:assoc-pressure.
The zero extension of the velocity tensor on the finite time slab,
used by thm:assoc-pressure.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Every component of the zero-extended velocity tensor belongs to
space-time L^(5/3), by lem:u-ten-thirds.
Every component of the zero-extended velocity tensor belongs to
space-time L^(3/2), by the finite-time L^3 energy interpolation.
The jointly measurable Riesz pressure selected for thm:assoc-pressure.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The associated pressure candidate belongs to space-time L^(5/3), as in
thm:assoc-pressure.
The pressure candidate has the global L^(5/3) membership required by
thm:assoc-pressure on the finite time slab.
The pressure selected from a Leray–Hopf solution's velocity tensor.
Equations
Instances For
The pressure selected for thm:assoc-pressure has the required
space-time L^(5/3) membership.