“…The Ross Sea ice drainage basin is divided into east antarctic and west antarctic portions by the Transantarctic Mountains, and the latter portion has several features which suggest nonequilibrium flow conditions; specifically, (1) the ice surface is generally concave whereas an equilibrium ice sheet has a convex surface [Nye, 1959[Nye, , 1967Hae[eli, 1961;Weertman, 1961], (2) evidence of extensive past glaciation• is preserved in bordering unglaciated areas and on •he Ross Sea floor [Wade, 1937;Douma•i, 1964;Mercer, 1968aMercer, , 1972Calkin eta/., 1970;Denton et al, 1970;Houtz and Meijer, 1970;LeMasurier, 1972;Mayewski, 1972;Fillon, 1972], (3) the floating ice cover and possibly the grounded ice cover overlies bedrock that is apparently in isostatic uplift, presumably due to partial reduction of a heavier former ice cover [Bennett, 1964;Robinson, 1964;Bentley, 1964], (4) ice elevations formerly were several hundred meters higher than at present according to oxygen isotope analyses of ice cores at Byrd Station and Little America 5 [Johnsen et al, 1972;Dansgaard, personal communication, 1972], (5) between Byrd Station and the ice divide, downstream ice output quite possibly exceeds the precipitation ice input, suggesting a negative ice budget in this region [Whillans, 1973a, b;Brecher, 1973], (6) a wet base underlies most or all of the grounded ice sheet, which is a neces•ry but not sufficient condition for a surge of the ice sheet [Zotikov, 1963a;Gow et al, 1968;Weertman, 1969;Robin et al, 1970b;Budd et al, 1970;Dewart, 1973], and (7) thermal instability may be widespread in the grounded ice cover and might-lead to thermal convection [Hughes, 1971[Hughes, , 1972aBentley, 1971] and perhaps surges …”