Statement

Let (u1,p1,f1)(u_1,p_1,f_1) solve the with viscosity 11. For ν>0\nu>0, set

uν(t,x)=νu1(t,x/ν),pν(t,x)=νp1(t,x/ν),fν(t,x)=νf1(t,x/ν).u_\nu(t,x)=\sqrt\nu\,u_1(t,x/\sqrt\nu),\quad p_\nu(t,x)=\nu p_1(t,x/\sqrt\nu),\quad f_\nu(t,x)=\sqrt\nu\,f_1(t,x/\sqrt\nu).

Then (uν,pν,fν)(u_\nu,p_\nu,f_\nu) solves the equations with viscosity ν\nu.

Verification and energy

The time, advection, pressure, and viscous terms all become ν\sqrt\nu times their unit-viscosity versions. Divergence remains zero. By change of variables, the kinetic energy in dimension dd is Eν(t)=ν1+d/2E1(t)E_\nu(t)=\nu^{1+d/2}E_1(t), whenever finite. The spatial domain is also dilated by ν\sqrt\nu; on a torus this changes its periods.

References