Dry snow an the surface of polar ice ice sheets is first densified and
metamorphosed to produce firn. Bubbly ice is the nest stage of the tr
ansformation process which takes place below the depth of pore closure
. This stage extends to the transition zone where, due to high pressur
es and low temperatures, air trapped in bubbles and ice begins to form
the mixed air clathrate hydrates, while the gas phase progressively d
isappears. Here we develop a model of bubbly-ice rheology and ice-shee
t dynamics taking into account glacier-ice compressibility. The intera
ction between hydrostatic compression of air bubbles, deviatoric (unia
xial) compressive deformation of the ice matrix and global deformation
s of the glacier body is considered. The ice-matrix pressure and the a
bsolute-load pressure are distinguished. Similarity theory and scale a
nalysis are used to examine the resultant mathematical model of bubbly
-ice densification. The initial rate of bubble compression in ice shee
ts appears to be relatively high, so that the pressure (density) relax
ation process takes place only 150-200 m in depth (below pore close-of
f) to reach its asymptotic phase, wherein the minimal drop between bub
ble and ice pressures is governed by the rate of loading (ice accumula
tion). This makes it possible to consider densification under stationa
ry (present-day) conditions of ice formation as a special case of prim
ary interest. The computational tests performed with the model indicat
e that both ice-porosity and bubble-pressure profiles in ice sheets ar
e sensitive to variations of the rheological parameters of pure ice. H
owever, only the bubble-pressure profile distinguishes between the rhe
ological properties at low and high stresses. The porosity profile at
the asymptotic phase is mostly determined by the air content in the ic
e. In the companion paper (Lipenkov and others, 1997), we apply the mo
del to experimental data from polar ice cores and deduce, through an i
nverse procedure, the rheological properties of pure ice as well as th
e mean air content in Holocene and glacial ice sediments at Vostok Sta
tion (Antarctica).