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Lecture 5 : Wind & effects of friction

Lecture 5 : Wind & effects of friction. The meridional structure of the atmosphere.

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Lecture 5 : Wind & effects of friction

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  1. Lecture 5:Wind & effects of friction

  2. The meridional structure of the atmosphere The atmosphere is warmer in the equatorial belt than over the polar caps. These horizontal temperature gradients induce, by hydrostatic balance, a horizontal pressure gradient force ‘‘P’’ that drive rings of air poleward. Conservation of angular momentum induces the rings to accelerate eastwards until Coriolis forces acting on them, ‘‘C,’’ are sufficient to balance the pressure gradient force ‘‘P,.’

  3. The mean height of the 500 mbar surface in January, 2003 (monthly mean). The contour interval is 6 decameters ≡ 60 m. The surface is 5.88km high in the tropics and 4.98km high over the pole. Latitude circles are marked every 10◦, longitude every 30◦.

  4. Warm columns of air expand, cold columns contract, leading to a tilt of pressure surfaces, a tilt which typically increases with height in the troposphere. In Section 7.3, we will see that the corresponding winds are out of the paper, as marked by in the figure. .

  5. The circulation envisaged by Hadley (1735) comprising one giant meridionalcell stretching from equator to pole. Regions where Hadley hypothesized westerly (W) and easterly (E) winds are marked.

  6. Meridional cross-section of zonal-average zonal wind (ms−1) under annual mean conditions (top), DJF (December, January, February ) (middle) and JJA (June, July, August) (bottom) conditions.

  7. The meridional overturning streamfunctionχ of the atmosphere in annual mean, DJF, and JJA conditions. Units are in 109 kg s−1, or Sverdrups, as discussed in Section 11.5.2. Flow circulates around positive (negative) centers in a clockwise (anticlockwise) sense. Thus in the annual mean, air rises just north of the equator and sinks around ±30◦.

  8. Effects of friction

  9. Geostrophic flow around a high pressure center (left) and a low pressure center (right). Northern hemisphere case, f > 0 .) The effect of Coriolis deflecting flow ‘‘to the right’’ is balanced by the horizontal component of the pressure gradient force, −1/ρ∇p, directed from high to low pressure.

  10. Geostrophic flows u =ug around high and low pressures in N.Hemisphere; here =k. Surface pressure (mbar; top) and winds (bottom) on Nov/21 2011 in NW Pacific.

  11. Balance of forces in flow (a) without and (b) with friction; shown for f > 0.

  12. Surface pressure (mbar; top) and near-surface winds (bottom) on Nov/21 2011 in NW Pacific. East of Taiwan, the p-contours are nearly zonal, so that geostrophic winds are easterly. But the (near-surface) wind vectors are actually from the northeast.

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