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Past Climate Variability and Change in the Arctic and at High Latitudes

Past Climate Variability and Change in the Arctic and at High Latitudes

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Although l<strong>in</strong>ked to site temper<strong>at</strong>ure, δ 18O can<br />

be affected by many factors (Jouzel et al., 1997;<br />

Alley <strong>and</strong> Cuffey, 2001), such as change <strong>in</strong> <strong>the</strong><br />

r<strong>at</strong>io of summertime to w<strong>in</strong>tertime precipit<strong>at</strong>ion.<br />

Hence, additional means of determ<strong>in</strong><strong>in</strong>g<br />

past temper<strong>at</strong>ures are required. One of <strong>the</strong> most<br />

reliable is based on <strong>the</strong> physical temper<strong>at</strong>ure of<br />

<strong>the</strong> ice. Just as a frozen turkey takes a long time<br />

<strong>in</strong> a hot oven to warm <strong>in</strong> <strong>the</strong> middle, <strong>in</strong>termedi<strong>at</strong>e<br />

depths of <strong>the</strong> central GreenlAnd ice Sheet<br />

are colder than ice above or below. Surface ice<br />

temper<strong>at</strong>ures equilibr<strong>at</strong>e with air temper<strong>at</strong>ure,<br />

<strong>and</strong> basal ice receives some warmth from Earth’s<br />

he<strong>at</strong> flow, but <strong>the</strong> center of <strong>the</strong> ice sheet has not<br />

f<strong>in</strong>ished warm<strong>in</strong>g from <strong>the</strong> ice-age cold. If ice<br />

flow is understood well <strong>at</strong> a site, <strong>the</strong> modern<br />

profile of <strong>the</strong> physical temper<strong>at</strong>ure of <strong>the</strong> ice with<br />

<strong>in</strong>creas<strong>in</strong>g depth provides a low-time-resolution<br />

history of <strong>the</strong> surface temper<strong>at</strong>ure with <strong>in</strong>creas<strong>in</strong>g<br />

time. Jo<strong>in</strong>t <strong>in</strong>terpret<strong>at</strong>ion of <strong>the</strong> isotopic<br />

r<strong>at</strong>ios <strong>and</strong> temper<strong>at</strong>ures measured <strong>in</strong> boreholes<br />

(Cuffey et al., 1995; Cuffey <strong>and</strong> Clow, 1997),<br />

or <strong>in</strong>dependent <strong>in</strong>terpret<strong>at</strong>ion of <strong>the</strong> borehole<br />

temper<strong>at</strong>ures <strong>and</strong> <strong>the</strong>n comparison with <strong>the</strong><br />

isotopic r<strong>at</strong>ios (Dahl-Jensen et al., 1998), helps<br />

to outl<strong>in</strong>e <strong>the</strong> history of surface air temper<strong>at</strong>ure.<br />

Fur<strong>the</strong>rmore, <strong>the</strong> rel<strong>at</strong>ion between isotopic r<strong>at</strong>io<br />

<strong>and</strong> temper<strong>at</strong>ure (α ‰ per °C) becomes a useful<br />

paleoclim<strong>at</strong>ic <strong>in</strong>dic<strong>at</strong>or, <strong>and</strong> changes <strong>in</strong> this r<strong>at</strong>io<br />

α with time can be used to test hypo<strong>the</strong>ses about<br />

<strong>the</strong> overall changes <strong>in</strong> seasonality of snowfall<br />

<strong>and</strong> o<strong>the</strong>r factors.<br />

The isotopic composition of gases trapped <strong>in</strong><br />

bubbles <strong>in</strong> <strong>the</strong> ice sheet provides an additional <strong>in</strong>dic<strong>at</strong>or<br />

of temper<strong>at</strong>ure. New-fallen snow conta<strong>in</strong>s<br />

many <strong>in</strong>terconnected air spaces. Snow turns to<br />

ice without melt<strong>in</strong>g <strong>in</strong> central regions of cold<br />

ice sheets through solid-st<strong>at</strong>e mechanisms th<strong>at</strong><br />

oper<strong>at</strong>e more rapidly under higher temper<strong>at</strong>ure<br />

or higher pressure. Snow <strong>in</strong> an ice sheet usually<br />

transforms to ice with<strong>in</strong> <strong>the</strong> top few tens of<br />

meters. The <strong>in</strong>termedi<strong>at</strong>e m<strong>at</strong>erial is called firn,<br />

<strong>and</strong> <strong>the</strong> transform<strong>at</strong>ion is complete when bubbles<br />

are isol<strong>at</strong>ed so th<strong>at</strong> <strong>the</strong> air spaces are no longer<br />

<strong>in</strong>terconnected to <strong>the</strong> surface. W<strong>in</strong>d mov<strong>in</strong>g<br />

over <strong>the</strong> ice sheet typically mixes gases <strong>in</strong> <strong>the</strong><br />

pore spaces of <strong>the</strong> firn only <strong>in</strong> <strong>the</strong> uppermost<br />

few meters or less. Diffusion mixes <strong>the</strong> gases<br />

deeper than this. Gases are slightly separ<strong>at</strong>ed by<br />

gravity (Sowers et al., 1992), with <strong>the</strong> air trapped<br />

<strong>in</strong> bubbles slightly isotopically heavier than <strong>in</strong> <strong>the</strong><br />

free <strong>at</strong>mosphere, proportional to <strong>the</strong> thickness<br />

of <strong>the</strong> air column <strong>in</strong> which diffusion dom<strong>in</strong><strong>at</strong>es.<br />

<strong>Past</strong> <strong>Clim<strong>at</strong>e</strong> <strong>Variability</strong> <strong>and</strong> <strong>Change</strong> <strong>in</strong> <strong>the</strong> <strong>Arctic</strong> <strong>and</strong> <strong>at</strong> <strong>High</strong> L<strong>at</strong>itudes<br />

If a sudden temper<strong>at</strong>ure change occurs <strong>at</strong> <strong>the</strong><br />

surface, <strong>the</strong> result<strong>in</strong>g temper<strong>at</strong>ure change of <strong>the</strong><br />

firn bene<strong>at</strong>h requires typically about 100 years<br />

to penetr<strong>at</strong>e to <strong>the</strong> depth of bubble trapp<strong>in</strong>g.<br />

However, when a temper<strong>at</strong>ure gradient is applied<br />

across gases <strong>in</strong> diffusive equilibrium, <strong>the</strong><br />

gases are separ<strong>at</strong>ed by <strong>the</strong>rmal fraction<strong>at</strong>ion as<br />

well as by gravity, with <strong>the</strong> heavier gases mov<strong>in</strong>g<br />

<strong>the</strong>rmally to <strong>the</strong> colder end (Sever<strong>in</strong>ghaus et al.,<br />

1998). Equilibrium of gases is obta<strong>in</strong>ed <strong>in</strong> a few<br />

years, far faster than <strong>the</strong> time for he<strong>at</strong> flow to<br />

remove <strong>the</strong> temper<strong>at</strong>ure gradient across <strong>the</strong> firn.<br />

With<strong>in</strong> a few years after an abrupt temper<strong>at</strong>ure<br />

change <strong>at</strong> <strong>the</strong> surface, newly form<strong>in</strong>g bubbles<br />

will beg<strong>in</strong> to trap air with very slight (but easily<br />

measured) anomalies <strong>in</strong> gas-isotope compositions,<br />

<strong>and</strong> this trapp<strong>in</strong>g of slightly anomalous<br />

air will cont<strong>in</strong>ue for a century or so. Because<br />

different gases have different sensitivities to<br />

temper<strong>at</strong>ure gradients <strong>and</strong> to gravity, measur<strong>in</strong>g<br />

isotopic r<strong>at</strong>ios of several gases (such as argon<br />

<strong>and</strong> nitrogen) allows researchers to determ<strong>in</strong>e<br />

<strong>the</strong> temper<strong>at</strong>ure difference th<strong>at</strong> existed vertically<br />

<strong>in</strong> <strong>the</strong> firn <strong>at</strong> <strong>the</strong> time of bubble trapp<strong>in</strong>g<br />

<strong>and</strong> to determ<strong>in</strong>e <strong>the</strong> thickness of firn <strong>in</strong> which<br />

w<strong>in</strong>d was not mix<strong>in</strong>g <strong>the</strong> gas (Sever<strong>in</strong>ghaus et<br />

al., 1998). If <strong>the</strong> surface temper<strong>at</strong>ure changed<br />

very quickly, <strong>the</strong> magnitude of <strong>the</strong> temper<strong>at</strong>ure<br />

difference across <strong>the</strong> firn will peak <strong>at</strong> <strong>the</strong><br />

magnitude of <strong>the</strong> surface-temper<strong>at</strong>ure change;<br />

for a slower change, <strong>the</strong> temper<strong>at</strong>ure difference<br />

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