Study Guide (lecture # 12)
Book pages: 120-121, 128-134, skim: 116-119, 122-127
Review:
(lecture # 11)
- potential energy considerations:
- introduction to APE
- conceptual models of APE
- Hadley cell as a Carnot cycle
Today's topics:
- "Global" definitions of APE
- limited area APE -- Interpretation of:
- efficiency factor
- diabatic processes
Jargon:
efficiency factor, Leibnitz's rule
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"Global" APE:
(Section 4.3; continued)
How is APE defined mathematically? (“global” definition now,
limited area next) (Chap. 4.3)
- the reference state -- measures the minimum PE
- APE proportional to departures from the mean:
P on theta surfaces; theta on P surfaces, or T on P surfaces
- APE is created by heating the air that is already hot and/or
cooling the cold air
<< Note: interpretation of the 4 formulae is important, NOT the
derivation. >>
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Limited-volume APE derivation:
(Section 4.4)
- why formulate limited area equations?
- reference pressure
- << Note: interpretation of the formulae: 4.30, 4.31, 4.34 is important,
NOT the derivation >>
- efficiency factor
- weighting based on deviation from reference state
Interpretation of limited domain APE and KE:
(Section 4.5.1)
- five groups of terms change APEj : only first 3 listed are
important to discuss
- diabatic processes (includes 5 sources/sinks)
- 2nd term: similar term found in the KEj
and APEj equations
- divergence of heat flux -- conversion between APE forms:
internal to the domain and external.
- divergence of mass in domain (sort of)
- changes in composition that alter the reference pressure in
the domain
- distribution of the efficiency factor —
- tropical max; high latitude minimums,
- largest magnitudes mainly in middle troposphere
diabatic processes: the epislon*q integrand in (4.30)
Solar Radiation:
q>0. So:
- generates APE in winter since tropical q >> polar q.
- albedo causes weak generation in summer too
Terrestrial Radiation: q<0. (slightly greater in
tropics, so:
- might expect this to destroy APE, but
- generates APE because emission in high latitudes is from
cloud tops where epsilon<0. (subtropial latitudes have emission
where epsilon is much smaller)
NOTE: [epsilon] is nearly zero in midlatitudes, so
the sign of epsilon probably varies as follows:
- epsilon >0 for relatively warm areas (e.g. oceans in winter,
or warm sector of a frontal cyclone)
- epsilon <0 for relatively cold areas (e.g. continents in
winter or cold air sector (behind a cold front). )
Sensible Heat Surface Flux: (SHF)
- SHF is largest near WBC's
- ambiguous as to APE tendency since:
- heating input where air is hot thus reducing T departure,
- But, heating reduces atmospheric static stability, which
encourages cyclogenesis
Latent Heat Surface Flux: (LHF)
- while most evaporation is near WBCs, the heat is released
elsewhere
- when the latent heating increases warm front precipitation
(which it often does) eddy APE is generated
Friction:
- only important for KE
- always destroys KE