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Fig. 7-15, p.182 Single cell model: simple but not good enough, e.g., our surface winds do not flow N-S. We really do need to include Earth’s rotation.

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Presentation on theme: "Fig. 7-15, p.182 Single cell model: simple but not good enough, e.g., our surface winds do not flow N-S. We really do need to include Earth’s rotation."— Presentation transcript:

1 Fig. 7-15, p.182 Single cell model: simple but not good enough, e.g., our surface winds do not flow N-S. We really do need to include Earth’s rotation and land masses in a more complex model sun Unequal heating of surface by the Sun (the beginning of ALL weather). Uneven energy input is redistributed by atmosphere and oceans convective cell

2 Fig. 7-16, p.183 Three cell model: much better, but not perfect. Here we “allow” rotation, but still have ocean-covered planet. Land masses obscure this predicted three-cell pattern. Must be an odd number of cells: what goes up at beginning of first cell must be “balanced” by what comes down at end of last cell. Could be 1, 3, 5, etc. Three on Earth dictated by rotation speed. On Venus, where rotation is very slow, only one cell develops. Predicted surface winds after PGF and CF included

3 Fig. 7-15b, p.182 Minot, N. Dakota (48 N) Tucson, Arizona (32 N) easterlies westerlies

4 Fig. 7-17a, p.184 Subtropical high Subpolar low (shows up as a trough, as predicted) Subpolar low Equatorial low

5 Fig. 7-17b, p.185 Pacific H has moved N. and W. allowing sinking, warming air to subside along Pacific coast Bermuda H. has moved S. and W. driving air to thermal low over AZ and setting up conditions for monsoons For more about the monsoon see http://www.wrh.noaa.gov/twc/monsoon/monsoon.php

6 Fig. 7-18, p.186

7 Fig. 7-19, p.187 Elevated inversion due to sinking air from Ferrel cell, which warms as it compresses on the way down to the surface (see Fig. 12.12).

8 Fig. 7-20, p.187 During summer, the eastern edge of the Pacific High is well situated to force sinking warming air down over Los Angeles causing a strong elevated inversion that prevents convection and clouds/rain (see Fig. 7.17b).

9 Fig. 7-21, p.187 Polar low

10 Fig. 7-22, p.188

11 Fig. 7-23, p.189

12 Fig. 7-24, p.190 For us, the following are the most important ocean currents: 1) Gulf Stream 2) North Atlantic Drift 3) Newfoundland Current 9) South Equatorial Current 16) California Current 17) Peru (Humbolt) Current

13 Table 7-2, p.190

14 Fig. 7-25, p.191 If the CA current brings cold water down from Alaska then why is the coldest water halfway down the coast and not further north? Answer – upwelling. Cold CA current

15 Fig. 7-26, p.191 Upwelling of very cold water from the bottom of the Pacific is evident off San Francisco Coriolis “force” causes ocean current to deflect to the right, i.e., offshore

16 Fig. 7-27, p.193 ENSO = El Nino/Southern Oscillation (in atmospheric pressure and wind direction)

17 Fig. 7-28, p.194 Current sea surface temperature animation: http://www.cpc.ncep.noaa.gov/products/analysis_monitoring/enso_update/sstanim.html 97/98 El Nino animation: http://www.cdc.noaa.gov/map/clim/sst_olr/old_sst/sst_9798_anim.shtml “Temperature anomaly” scale

18 Fig. 7-29, p.195 Very weak ENSO this winter: warmer/wetter conditions to SE AZ

19 Table 7-1, p.168


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