Simple analytical models of glacier-climate interactions - by Prof. J ...
Simple analytical models of glacier-climate interactions - by Prof. J ...
Simple analytical models of glacier-climate interactions - by Prof. J ...
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5. A volume time scale for valley <strong>glacier</strong>s<br />
A time scale for the adjustment <strong>of</strong> <strong>glacier</strong>s to <strong>climate</strong> change can be derived from the<br />
requirement <strong>of</strong> mass continuity (Jóhanesson et al, 1989; Haeberli and Hoelzle, 1995).<br />
We perform a linear perturbation analysis. Conservation <strong>of</strong> ice volume V can be<br />
expressed as<br />
d V<br />
d t<br />
= d A H m<br />
d t<br />
= H m d A<br />
d t<br />
+ A dH m<br />
d t<br />
. (5.1)<br />
Here A is the <strong>glacier</strong> area and H m the mean ice thickness. Now we write<br />
V = V 0 + V', A = A 0 +A' and H m = H m,0 + H m ', where the reference state is defined<br />
as (V 0 , A 0 , H m,0 ). By substitution in eq. (5.1) and <strong>by</strong> neglecting higher-order terms we<br />
then obtain the perturbation equation<br />
d V'<br />
d t<br />
= H m,0 d A'<br />
d t<br />
+ A 0 dH m '<br />
d t<br />
. (5.2)<br />
Next we assume (see Fig. 7.1):<br />
A' = w f L' , (5.3)<br />
Here w f is the characteristic width <strong>of</strong> the <strong>glacier</strong> tongue.<br />
Fig. 6.1.<br />
L'<br />
total <strong>glacier</strong><br />
area A<br />
w f<br />
flowline<br />
If the mean thickness <strong>of</strong> the <strong>glacier</strong> does not change we have for the change <strong>of</strong> ice volume<br />
with time<br />
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