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Todays lecture objectives:

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... the fluid is equal in magnitude to the weight of fluid displaced by the object. ... at 'A' will reach its lifting condensation level almost immediately, and beyond ... – PowerPoint PPT presentation

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Title: Todays lecture objectives:


1
ATMS 305 Atmospheric Thermodynamics and Statics
  • Todays lecture objectives
  • The Concept of Static Stability (WH 3.6)
  • Now that we know how to deal with phase changes
    inside the air (Polly) parcel, how does the
    temperature inside the air (Polly) parcel compare
    to the environmental air?

?
2
ATMS 305 The Concept of Static Stability
  • Todays lecture topics
  • The Concept of Static Stability (WH 3.6)
  • What is meant by stability?
  • Unsaturated air
  • Archimedes Principle and buoyancy
  • Saturated air
  • Conditional and convective instability

3
Meteorological Stability
  • The ability of the air to return to its origin
    after displacement

(courtesy F. Remer)
4
Stability
  • Depends on the thermal structure of the atmosphere

(courtesy F. Remer)
5
Stability
  • Can be classified into 3 categories
  • Stable
  • Neutral
  • Unstable

(courtesy F. Remer)
6
Stable
  • Returns to original position after displacement

(courtesy F. Remer)
7
Neutral
  • Remains in new position after being displaced

(courtesy F. Remer)
8
Unstable
  • Moves farther away from its original position

(courtesy F. Remer)
9
Stability
  • How is air displaced?
  • Two methods
  • 1.) Forced Ascent
  • 2.) Auto-Convective Ascent

(courtesy F. Remer)
10
Forced Ascent
  • Some mechanism forces air aloft
  • Usually synoptic scale feature

Cold air
Warm air
Cool Air
(courtesy F. Remer)
11
Forced Ascent
  • Type of clouds
  • Depends on stability

Stable - Stratus Unstable - Cumulus
(courtesy F. Remer)
12
Auto-Convective Ascent
  • Air becomes buoyant by contact with warm ground
  • Usually microscale or mesoscale

Hot
Cool
Cool
(courtesy F. Remer)
13
Auto-Convective Ascent
  • Type of Clouds
  • Cumulus

(courtesy F. Remer)
14
Stability
  • As parcel rises
  • 1.) Parcel Temperature Changes
  • Unsaturated?
  • Dry Adiabatic Lapse Rate

(courtesy F. Remer)
15
Dry Adiabatic Lapse Rate
(courtesy F. Remer)
16
Archimedes Principle
  • The buoyant force exerted by a fluid on an object
    in the fluid is equal in magnitude to the weight
    of fluid displaced by the object.

Archimedes 287 211 BC
(courtesy F. Remer)
17
Archimedes Principle
  • Square bubble in a tank of water

B
B buoyancy force
(courtesy F. Remer)
18
Archimedes Principle
  • Water pressure in tank increases with depth

B
p
z
(courtesy F. Remer)
19
Archimedes Principle
  • Water is in hydrostatic equlibrium

B
(courtesy F. Remer)
20
Archimedes Principle
  • Force on bottom of bubble

Fbottom
(courtesy F. Remer)
21
Archimedes Principle
  • Force on top of bubble

Ftop
Fbottom
(courtesy F. Remer)
22
Archimedes Principle
  • Buoyancy Force

B
Ftop
Fbottom
(courtesy F. Remer)
23
Archimedes Principle
  • Horizontal Pressure Differences Balance

(courtesy F. Remer)
24
Archimedes Principle
  • Pressure Difference Between Top Bottom

ptop
pbottom
(courtesy F. Remer)
25
Archimedes Principle
  • Combine Equations

B
ptop
pbottom
(courtesy F. Remer)
26
Archimedes Principle
Archimedes 287 211 BC
  • Cartoon here??

At the moment of Archimedes famous discovery.
27
Buoyancy
  • Similar to parcel of air in atmosphere
  • At Equilibrium
  • Density of Parcel Same as Density of Environment

(courtesy F. Remer)
28
Buoyancy
  • Density Difference Results in Net Buoyancy Force

B
(courtesy F. Remer)
29
Buoyancy
  • Density Difference Results in Net Buoyancy Force

B
(courtesy F. Remer)
30
Buoyancy
  • Net Buoyancy Force

B
(courtesy F. Remer)
31
ATMS 305 The Concept of Static Stability
  • A parcel of unsaturated air originally located at
    level O
  • Environment A
  • T-storm possible or not?

32
ATMS 305 The Concept of Static Stability
  • A parcel of unsaturated air originally located at
    level O
  • Environment B
  • T-storm possible or not?

33
Stability
  • As parcel rises
  • 1.) Parcel Temperature Changes
  • Saturated?
  • Pseudoadiabatic Lapse Rate

(courtesy F. Remer)
34
Pseudo-Adiabatic Lapse Rate
  • Varies with dws/dT

Big
Small
4oC km-1 lt Gs lt 9.8oC km-1
(courtesy F. Remer)
35
ATMS 305 The Concept of Static Stability
  • If a parcel of air is saturated
  • Static stability
  • Static instability
  • Static neutrality

36
ATMS 305 The Concept of Static Stability
  • Conditional instability
  • Level of free convection
  • Altitude above which the parcel develops a
    positive buoyancy which carries it upward even in
    the absence of further lifting

37
ATMS 305 The Concept of Static Stability
  • Conditional instability
  • If the environmental lapse rate is between the
    dry and saturated adiabatic lapse rates, there is
    the possibility of gravitational instability if
    vertical motions are large enough to lift air
    parcels beyond their level of free convection

38
ATMS 305 The Concept of Static Stability
  • Convective (or potential) instability
  • An air parcel at A will reach its lifting
    condensation level almost immediately, and beyond
    that point it will cool moist adiabatically.
  • An air parcel at B will cool dry adiabatically
    through a deep layer before it reaches its LCL.
  • As the inversion layer is lifted, the top part
    cools much more rapidly than the bottom part and
    the lapse rate quickly becomes destabilized

39
ATMS 305 The Concept of Static Stability
  • Conditional and convective instability
  • Throughout the tropics, the lapse rate is
    conditionally unstable up to 15 km convectively
    unstable up to 6 km
  • Why doesnt deep convection break out everywhere
    in the tropics?

40
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