Observations from sonar data have suggested enhanced melting of thick, ridg
ed ice relative to level ice. There are several mechanisms that may account
for this intensified melting. In this paper, we examine the effects of two
-dimensional (2-D) heat conduction and enlarged basal surface area due to t
he sloping sides of the keel on heat conduction and melt rates. The cross s
ection of the 2-D ridge is taken to be an isosceles triangle with a rounded
crest. This is roughly the shape observed and allows a convenient numerica
l representation in polar coordinates; For comparison, ridges of similar sh
ape are also represented as a collection of 1-D columns of varying thicknes
s, similar to what is implicit in typical ice thickness distribution models
. The results show that 2-D ridges inhibit the heat conduction compared to
1-D ridges owing to the dominating effect of weaker temperature gradients.
The slope of the keel is the dominant factor in determining the temperature
gradient. A size distribution of 2-D ridges reduces heat transfer to the a
tmosphere by 3 W m(-2) compared to a similar distribution of 1-D ridges. Ov
er an annual cycle, basal ablation along the keel is insignificant for 2-D
ridges with small slopes, whereas ridges with large slopes show ablation ra
tes determined by the ice-ocean heat flux. These melt rates imply a transit
ion From a triangular to a more rounded shape. The I-D ridge geometry is no
t adequate to simulate the net melting at the keel base over an annual cycl
e. Melt rates are calculated along the ridge keel and for level ice over a
40 day period for comparison with observations. For 1-D ridges, all ice thi
cker than 5 m melts more slowly than the corresponding level ice. The inclu
sion of 2-D heat conduction increases the amount of ablation in the thicker
ice relative to the 5 m ice, especially for ridges with larger slopes. How
ever, this increase explains only a small fraction of the enhanced basal me
lting seen in the observations. These results suggest that other mechanisms
are important in determining the mass loss from thicker ice.