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Meteo 3: Chapter 8 Stability and Cloud Types Read Chapter 8.

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Presentation on theme: "Meteo 3: Chapter 8 Stability and Cloud Types Read Chapter 8."— Presentation transcript:

1 Meteo 3: Chapter 8 Stability and Cloud Types Read Chapter 8

2 Parcel Theory  Parcel: volume of air assumed to behave separately from the air surrounding it  Environment: everything outside the air parcel

3 Hydrostatic Balance means small vertical motions

4 Hydrostatic Balance can be violated on small space and time scales…requires instability (buoyancy)

5 Role of Stability in Cloud Formation  We already have relationships to determine if net condensation is occurring (e.g. LCL, vapor pressure vs. saturation vapor pressure)  If we can determine how air moves vertically, we can determine whether clouds are likely to form and how deep they might be!

6 Concept of Buoyancy

7 Lifting a Parcel of Air

8 Unstable equilibrium: T parcel > T environment

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10 Stable equilibrium: T parcel < T environment

11 Neutral equilibrium  A parcel is given a push upward and comes to a stop after a short rise (T parcel = T environment ) (T parcel = T environment )  The key to determining stability is comparing a parcel’s temperature to the atmospheric temperature at the altitude of interest

12 Dry Adiabatic Lapse Rate (DALR)

13 More on DALR  An unsaturated sinking air parcel warms at 10°C/km  These temperature changes result from molecules in the parcel doing work for parcel expansion when rising and gaining kinetic energy via compression when sinking  Adiabatic: no exchange of heat energy between a parcel and its surroundings

14 Even more  Environmental lapse rate is what is measured by a weather balloon –Determined locally by height above ground and temperature advection, among other things  On average, is ~6.5°C/km  If temperature decreases with height, lapse rates are positive  If lapse rate is negative (temperature increases with height), an inversion is present

15 Moist Adiabatic Lapse Rate (MALR)

16 Importance of MALR  Since rising, saturated air parcels cool at a slower rate, the parcel has a better chance of staying warmer than its environment longer, thus has a better chance of being positively buoyant  Not constant

17 Conditional Instability

18 Simple Model of Stability  Instability results when an air parcel is warmer than its environment (warm below cool ideal) –Solar heating & low-level warm advection increase instability…sometimes lapse rate near ground is greater than DALR = superadiabatic –Cooling ground increases stability (radiational cooling/evaporational cooling) –Upper-level cooling (warming) increases (decreases) instability  Warm, moist low levels and chilly mid-levels are an ideal setup for an unstable atmosphere (thunderstorms)

19 Warm below, cold above

20 Cloud Classification

21 High Clouds  Composed of ice crystals  Cirrostratus can lead to formation of halo around sun or moon

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24 Middle clouds  If cirrostratus lower and thicken into altostratus, that’s a good sign precipitation may be on the way  Alto-, strato- & cirro- cumulus form from destabilization of cloudy region in a generally stable environment

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28 Low clouds  Stratiform clouds to north of warm front where overrunning is occurring  “Nimbus” means rain

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32 Cumuliform clouds  Form via convection  “Clouds of vertical development”  Can last for minutes-few hours  Cumulonimbus produce thunderstorms, tornadoes, hail  Updrafts range from tens of cm/s (cumulus) to tens of m/s (cumulonimbus)

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39 Wave Clouds  Indicate a stable atmosphere

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41 Smoke as a stability clue

42 Summertime afternoons and wind

43 How does precipitation form?  Liquid water can become supercooled => drops of water exist as liquid with temperatures below 0°C  At temperatures >-40°C, tiny particles are needed to start ice crystal formation (ice nuclei)  Ice, liquid, and vapor coexist in clouds  Equilibrium vapor pressure over ice is less than the equilibrium vapor pressure over water at the same sub-freezing temperature

44 Bergeron Process  Saturation is reached over ice but not over water, thus ice crystals grow at the expense of liquid drops….eventually become large and fall

45 Collision-Coalescence Process  Occurs in “warm” clouds  Falling ice crystals melt into rain  Bigger raindrops fall faster than smaller ones  Larger drops collide with smaller drops  Grow as all or part of smaller drop’s water coalesces with larger drop

46 Virga


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