Chapter 3 Flashcards

(48 cards)

1
Q

The potential vorticity (PV)

A

the absolute circulation of an air parcel that is enclosed between two isentropic surfaces

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2
Q

…………………………………………. then it is officially called IPV (isentropic potential vorticity).

A

If PV is displayed on a surface of constant potential temperature

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3
Q

PV is simply expressed as

A
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4
Q

Static (hydrostatic) stability refers to

A

the resistive force offered to the motion by the vertical density structure of the atmosphere in the gravitational field, and specifically when the atmosphereis in hydrostatic equilibrium.

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5
Q

Thus, PV in contrast to vorticity on isobaric surfaces, consists of two factors

A

dynamic alelement and a thermodynamical element

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6
Q

Potential Vorticity units:

A
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7
Q

In the middle and upper troposphere, PV is ranging from

A

0.5 to 1.0 PVU

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8
Q

In the middle and upper troposphere, PV is ranging from 0.5 to 1.0 PVU. In the stratosphere

A

PV > 3.0 PVU

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9
Q

In the middle and upper troposphere, PV is ranging from 0.5 to 1.0 PVU. In the stratosphere PV > 3.0 PVU due to

A

the strong increase of the static stability

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10
Q

In terms of the PV concept, the tropopause in mid‐latitudes may be represented by the surface of

A

constant PV = 1.5 PVU, and considered as thedynamical tropopause.

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11
Q

positive PV‐anomaly

A

An abrupt lowering of the dynamical tropopause

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12
Q

A positive PV anomaly is produced by

A

the intrusion of stratospheric air into the
upper troposphere

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13
Q

A positive PV anomaly is produced by the intrusion of stratospheric air into the upper troposphere. An upper level PV anomaly,

A

advected down to middle troposphere is called: tropopause dynamic anomalyor folding of the tropopause

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14
Q

Due to PV conservation, the PV anomaly leads to

A

deformations invertical distribution of potential temperature and vorticity

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15
Q

…………………….. produces a vertical motion

A

In a baroclinic flow increasing with height, the intrusion of PV anomaly in the troposphere

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16
Q

The deformation of the isentropes imposes

A

ascending motion ahead of the anomaly and subsiding motion behind

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17
Q

An idealized cross section of an positive PV anomaly is shown below. The wind speed ……………… 1.5 PVU surface ………………………………….. where ………………. and ……………………..

A

increases with height. 1.5 PVU surface separates the very stable stratosphere, where the isentropes are close to each other, and the much less stable troposphere.

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18
Q

An idealized cross section of an positive PV anomaly is shown below. The wind speed increases with height. 1.5 PVU surface separates the very stable stratosphere, where the isentropes are close to each other, and the much less stable troposphere. Ahead of the PV anomaly there is

A

ascent, behind it descent

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19
Q

In the water vapour image the anomaly appears as

A

a dark, roundish area

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25
F
26
G
27
Analyses of PV appear to have more structure than
height analyses on an isobaric surface.
28
Analyses of PV appear to have more structure than height analyses on an isobaric surface. The reason for this is
a mathematical consequence of the dynamical principles.
29
If the gradient wind formula is examined, one can establish that
the wind is related to the gradient of the geopotential height
30
The horizontal gradient of PV is related to ............................. and show ....................................
second derivatives of the geopotential height, and show a lot more structure than the geopotential height field.
31
The practical consequence is that using PV can identify
e.g. short wave troughs in the geopotential height field more easily.
32
Since fast‐moving troughs can
influence weather dramatically
33
Since fast‐moving troughs can influence weather dramatically, PV is a useful tool to
notify this kind of small‐scale structures.
34
When there is a mismatch between the PV and the imagery it can be an indicative of
a model forecast or analysis error
35
The three types of mismatches between WV imagery and PV fields are:
temporal, location/spatial, and magnitudes/heights
36
To ensure the best comparison between the WV and PV fields make sure to
Compare the NWP analysis with the same time in water vapour imagery. If the times don't match, then an accurate representation of the other components will hinder your ability to accurately adjust the forecast NWP
37
To ensure the best comparison between the WV and PV fields make sure to: 1. Compare the NWP analysis with the same time in water vapour imagery. If the times don't match, then an accurate representation of the other components will hinder your ability to accurately adjust the forecast NWP
2. Compare the locations of synoptic features. Mesoscale or smaller diabatic processes are often not matched well between the NWP and the WV. Only in the largest complexes of diabatic processes comparing those features can be done directly.
38
To ensure the best comparison between the WV and PV fields make sure to: 1. Compare the NWP analysis with the same time in water vapour imagery. If the times don't match, then an accurate representation of the other components will hinder your ability to accurately adjust the forecast NWP 2. Compare the locations of synoptic features. Mesoscale or smaller diabatic processes are often not matched well between the NWP and the WV. Only in the largest complexes of diabatic processes comparing those features can be done directly.
3. Compare the magnitudes/heights of the major synoptic features This can be hard to compare unless the contour interval of the PV surface is high enough to match the gradients of the water vapour imagery.
39
Comparing the water vapour imagery and 1.5PVU surface, will be able to show
the differences well between observations and model
40
Because the 1.5PVU surface and water vapour surface are
so similar in vertical structure and height, we can make a nearly direct comparison
41
Limitations of Comparison
* The images will likely NOT match in areas of diabatic processes or strong frictional forces, and work best in developing systems, not in old systems. * Anticyclonic systems won't match between the WV and 1.5PVU surface as they have an inverse relationship.
42
In the WV image, the areas where the PV field doesn't match because of NWP errors, and not due to
diabatic/frictional processes or anticyclonic flow are identified.
43
In the WV image, the areas where the PV field doesn't match because of NWP errors, and not due to diabatic/frictional processes or anticyclonic flow are identified. Comparison is made to
look for location and magnitude mismatches, as there are no temporal differences.
44
Location a
The dry area east of southern Greenland Mismatch in magnitude (too large in PV, not extended far enough east)
45
location b
The PV anomaly over Denmark • Mismatch in location (too far north compared to dry maximum)
46
location c
The PV anomaly in western Russia • Mismatch in location (too far east in PV) • Mismatch in magnitude (too deep in PV)
47
location D
Location D: The warm dark region over Sweden and Finland • Mismatch in location (not tilting far enough east in PV)
48
Location E
The jetstreak aimed toward the southern UK and Northern France • Mismatch in magnitude (dark area not represented well in PV)