The target of this paper is a discussion of the meaning of the Newtoni
an concept of a reference frame showing no rotation with respect to a
set of distant celestial objects in the framework of general relativit
y. Because of the properties of Newtonian absolute space and time and
the existence of global inertial reference systems in Newton's theory
the theoretical construction of such a globally nonrotating reference
frame is obvious. This definitively no longer is the case in a relativ
istic framework. There exist no global inertial reference systems and
one faces the necessity to give the notion of nonrotating frames a rig
orous meaning. Considering possible definitions of nonrotating referen
ce frames in both Newtonian and relativistic physics, we conclude that
the concept of relative spatial rotation between reference systems pl
ays a fundamental role in defining nonrotating astronomical reference
frames. It turns out that the property of two relativistic reference s
ystems to show no spatial rotation relative to each other, being a coo
rdinate-dependent concept, has some properties which cannot be interpr
eted within our ''Newtonian common sense''. As an example, we discuss
two versions of a geocentric reference system, both of which can be co
nsidered to show no rotation relative to distant celestial objects at
the present level of observational accuracy, but differing by a time-d
ependent rotation of considerable amplitude. Applying the obtained res
ults to the recently elaborated formalisms for constructing relativist
ic astronomical reference systems, we describe relative spatial rotati
ons between the galactic, barycentric, geocentric reference systems an
d the reference system of an observer. We find a certain parallel betw
een the concept of simultaneity (synchronization of clocks) and the co
ncept of reference system showing no rotation relative to distant cele
stial objects. Both notions are absolute in Newtonian physics and beco
me coordinate-dependent in the relativistic framework, representing, t
herefore, a mathematical convention rather than a physically meaningfu
l phenomena.