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Simple analytical models of glacier-climate interactions - by Prof. J ...

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Problem West Antarcic ice sheet (P 3)<br />

The mass budget equation is obtained <strong>by</strong> setting the total accumulation equal to the total<br />

flux across the grounding line. This flux equals the ice velocity times the outlet cross<br />

section. Therefore<br />

π a R = 2 π R f * ρ w<br />

ρ i<br />

d 2 = 2 π R f d 2 (P 3.1)<br />

The water depth at the grounding line equals b 0 - s R, so we have<br />

d 2 = b 0<br />

2 + s<br />

2 R<br />

2 - 2 b0 s R (P 3.2)<br />

Combining yields<br />

2 f s 2 R 2 - (4 b 0 f s + a) R + 2 f b 0<br />

2 = 0 (P 3.3)<br />

Special case: b 0 = 0 (a purely marine ice sheet). So the highest point <strong>of</strong> the continent is<br />

just at sea level. Eq. (P 2.3) reduces to<br />

2 f s 2 R 2 - a R = 0 (P 3.4)<br />

→ R = a<br />

2 f s 2 (P 3.5)<br />

Application to the WAIS (R = 600 km, f = 1 yr -1 , a = 0.25 m yr -1 ):<br />

1/2<br />

→ s = a = 0.25<br />

1/2 = 0.00046 (P 3.6)<br />

2 f R 2 x 1 x 600,000<br />

Sensitivity to changes in accumulation rate:<br />

∂R<br />

∂a = 1<br />

2 f s 2 = 2.37x106 = 23.7 km/% (P 3.7)<br />

31

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