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Erdfernerkundung - Numerische Physik: Modellierung

Erdfernerkundung - Numerische Physik: Modellierung

Erdfernerkundung - Numerische Physik: Modellierung

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5.5. CAWSES 275<br />

variation expected from the solar-cycle variation of the UV radiation.<br />

Vanishing Geomagnetic Field<br />

Abbildung 5.42:<br />

Variation in total<br />

ozone during the solar<br />

cycle without geomagnetic<br />

field (courtesy M.<br />

Sinnhuber, U Bremen)<br />

§ 911 A worst case estimate for the ozone balance during a magnetic field reversal is obtained<br />

in case of a vanishing geomagnetic field. Then particles precipitate into the atmosphere at all<br />

latitudes and not only at high latitudes. Figure 5.42 shows model calculations or this case.<br />

The results are quite similar to the ones obtained for the present day geomagnetic field in<br />

Fig. 5.41:<br />

• total ozone depletion is higher during solar maximum than during solar minimum,<br />

• the effects of individual events are visible,<br />

• ozone depletion in individual events shows a hemispheric asymmetry,<br />

• the spatial pattern of ozone depletion varies with the solar cycle.<br />

Despite all these similarities (in fact, there is one similarity too much) there is also a fundamental<br />

and surprising difference between the two figures: ozone depletion in high latitudes<br />

is much more pronounced in case of a vanishing geomagnetic field although the number of<br />

particles precipitating at high latitudes does not change! The difference in particle precipitation<br />

between the present-day field and the vanishing field, on the other hand, occurs at<br />

low- and mid-latitudes: here the difference in ozone depletion between the two runs is less<br />

pronounced than at polar latitudes where no difference would be expected. This again reflects<br />

the complex relation between photochemical processes and atmospheric circulation.<br />

§ 912 A closer inspection of Fig. 5.42 suggests ozone depletion by 10–20% at high latitudes<br />

lasting for a few month. Ozone has radiative properties, in particular, it absorbs UV<br />

radiation and is also a greenhouse gas, that is, it affects the terrestrial long-wave emission.<br />

In consequence, a local change in ozone concentration can cause a local change in temperature.<br />

Since pressure gradients resulting from temperature gradients are the driving forces for<br />

atmospheric motion, a change in ozone concentration might cause a change in atmospheric<br />

velocity fields and thus modify climate.<br />

Consequences for Climate?<br />

§ 913 A first indication for such a process is given in Fig. 5.43: in the top panel ozone<br />

depletion at 75N is shown for a large solar energetic particle event at the time of polarity<br />

reversal, that is for a vanishing geomagnetic field. Ozone depletion can amount to more than<br />

50% in the stratosphere and stay at such high levels for almost a year. The lower panel in<br />

Fig. 5.43 shows the resulting changes in temperature (sorry for the color-coding). Although<br />

temperature changes are rather small (rarely larger than 5 K), temperature gradients can<br />

become quite large. In consequence, wind fields change. And once the wind fields are modified,<br />

the entire temperature distribution in the atmosphere is modified, which certainly will affect<br />

climate.<br />

c○ M.-B. Kallenrode 2. Juli 2008

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