Idealizing matter as a pressureless fluid and representing its motion
by a peculiar-velocity field superimposed on a homogeneous and isotrop
ic Hubble expansion, we apply (Lagrangian) spatial averaging on an arb
itrary domain D to the (nonlinear) equations of Newtonian cosmology an
d derive an exact, general equation for the evolution of the (domain d
ependent) scale factor a(D)/(t). We consider the effect of inhomogenei
ties on the average expansion and discuss under which circumstances th
e standard description of the average motion in terms of Friedmann's e
quation holds. We find that this effect vanishes for spatially compact
models if one averages over the whole space. For spatially infinite i
nhomogeneous models obeying the cosmological principle of large-scale
isotropy and homogeneity, Friedmann models may provide an approximatio
n to the average motion on the largest scales, whereas for hierarchica
l (Charlier-type) models the general expansion equation shows how inho
mogeneities might appreciably affect the expansion at all scales. An a
veraged vorticity evolution law is also given. Since we employ spatial
averaging, the problem of justifying ensemble averaging does not aris
e. A generalization of the expansion law to general relativity is stra
ightforward for the case of irrotational flows and will be discussed.
The effect may have important consequences for a variety of problems i
n large-scale structure modeling as well as for the interpretation of
observations.