Reference Frames

Mesh motion is defined with respect to a reference frame, which can be stationary (laboratory reference frame) or rotating and translating relative to the laboratory frame. In steady simulations, or in transient simulations that do not require a time-accurate solution, moving reference frames provide a way of modeling rotations and translations as a steady-state problem, while leaving the mesh stationary.

Consider a moving reference frame that is rotating and translating with constant velocity:

The velocity of a material point P with respect to the moving reference frame (also called the relative velocity) can be written as:

Figure 1. EQUATION_DISPLAY
vr=vvMRF,tωMRF×rP,MRF
(4860)

where v is the velocity in the laboratory reference frame (also called the absolute velocity), vMRF,t is the moving reference frame translation velocity, that is, the velocity of its origin with respect to the laboratory frame, ωMRF is the angular velocity of the moving reference frame with respect to the laboratory frame, and rP,MRF is the position vector of the material point with respect to the moving reference frame.

You can define the rotation of a moving reference frame with respect to a parent reference frame that can be both rotating and translating.

The resulting relative velocity is:
Figure 2. EQUATION_DISPLAY
vr=v(vp+ve)
(4861)

with

vp=vt+ωp×rpve=ωe×re

where ωp is the angular velocity of the parent reference frame, as measured in the laboratory reference frame, ωe is the angular velocity of the embedded reference frame, as measured in the parent reference frame, rp is the position vector with respect to the parent reference frame, and re is the position vector with respect to the embedded reference frame.