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Classification of the directions of ageostrophic winds It is useful to sort out which direction does the force take, or does the ageostrophic wind
take. Because, the force will change the wind (movement).
I want to divide the directions of force foura quadrants.
So, Fig7.5 show us that if an air parcel has an ageostrophic wind on the left side of actual wind, the force will accelerate the speed.
And, Fig7.6 show us that if an air parcel has an ageostrophic wind on the right side of actual wind, the force will decelerate the speed. Let us see the example. Fig7.7 shows the distributions of the actual winds( Black arrows) and the ageostrophic winds(red arrows) around Asia at 12Z on June 9th in 2011.
We can see the accelerating area around Japan sea. Acceleraing area tend to be divergent area, and divergent area tend to cloud area. Meanwhile, we can see the decelerating area around Yellow Sea. Decelerating area tend to be
convergent area, and tend to be fine weather area. We can see black area on the water vapor
Fig7.8 shows the distribution of divergence on the water vapor image.cloud images.
These divergent distributions have been gotten from the real(analyzed) wind, not from divergent wind(from velocity potential). I think that the ageostrophic wind is very useful to explane these meteorological phenomena. I think it is no need to use divergent wind, nor velocity potential. If you want to think the Meteorology as a science which includes dynamics, you should not use the divergent wind driven from the velocity potential. Because, the divergent wind leaves from an air parcel(mass), force and acceleration. Dynamics is a science which deals in masses, forces and accelerations etc.. |
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7. On the forces acting on the air parcel in the actual ageostrophic motionWe have been thinking an air parcel on many kinds of hypothetical condition. I wanted you to know what the theoretical ageostrophic motion is. Fig.7.1 shows a sample of ageostrophic wind in the real world.
We can see the ageostrophic wind which can’t be denied. Especially, near the boundary of
the westerlies zone and the tropical zone. The air parcels which have gone up from the lower layer are thrown out into the upper layer. They have been mingled with the air on the way of
middle layer, and have gotten a little similar velocity of upper layer air which has been
took a balance of geostrophic wind. But they have not gotten perfect geostrophic balance, and are beginning to act as ageostrophic(non-geostrophic) wind in the westerlies zone.
Fig.7.1 shows that the actual ageostrophic component is not as large as the theoretical
ageostrophic wind, but smaller than it.
Fig 7.2 shows the real wind model.
A black arrow shows an actual wind. An actual wind can be decomposed into a geostrophic
wind component and an ageostrophic(non-geostrophic) wind component. A blue arrow shows
a geostrophic wind component, and a red arrow shows an ageostrophic wind component.
The force acting on the real air parcel
Fig 7.3 shows the velocities of an real air parcel, and forces acting to it.
The upper side of this illustration shows north. So, contours are stretched east to west.
The thinner arrows show velocity vectors, and bolder arrows show force vectors.
If the wind have a balance of force, the pressure gradient force is equal to the Coriolis
force of the wind, but they are oppositely-oriented. The balanced wind is the geostrophic wind.
The Coriolis force is proportional to the speed at which the air is moving, and deflected
to the right. So, we can indicate how to calculate the Coriolis forces by drawing right
triangles which has velocity vectors and force vectors. These triangles are similar to each
others.
Fig7.4 shows the actual wind and its component, and acting forces. From this illustration,
we can understand that the actual force working the air is the Coriolis force obtained with
an ageostrophic wind component as the followings.
Coriolis forceAD with actual wind velocity. So, the total force is given a composition of AG
The solid thin blue arrowAB shows the geostrophic wind component, and the thinner black
arrowAE shows actual wind.
The real forces which act to this air parcel are the pressure gradient forceAG and the
and AD. If you draw a parallelogramADHG, it is given as a diagonalAH.
Then, ∠BAE=∠CAD
Coriolis force for the geostrophic wind is given as a broken blue arrowAC, From geostrophic
theorem, AG =AC.
Here, △ADE∽ △ACB、∠DAE=∠CAB=right angle.
Here, we pay attention to △ACD. The ratio of the segmentAC to the segmentAB is the same as
the ratio of the segmentAD to the segmentAE.
So, △ACD∽ △ABE
continueHere, I want to call △ABE a velocity triangle, and want to call △ACD a force triangle. If you turn this force triangle counterclockwise, it get the place △AC’D’. Then, this segmentC’D’ is parallel to segment BE. So, we can confirm that the real force that is acting on an air moving as an ageostrophic wind motion is given in the same way as Coriolis force, but with an ageostrophic component instead analyzed wind |
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