Class number 2 /27  Jan 24,  2011 More on thermodynamics

Sil's notes from this class

Loose ends from last class:

Weather briefing/ phenomenon show at start of class - rotating assignment

Today's material:

* Maybe a few more points in interactive skew-T mastery from COMET.

Recasting the 3 variables needed for moist air thermodynamics (at equilibrium).

    Which 3 are the best for conceptual and/or calculation purposes?
  1. pressure -- altitude for all practical purposes
  2. total water mixing ratio q -- conserved, linearly mixing (Dewpoint is monotonic, but not linear)
  3. Conserved heat or entropy type variable... (handout)

Relevant journal literature: (somewhat random selection)

Defining the variables

Comparison of theta-e and moist static energy (Betts 1974)
Relating Static Energy to Potential Temperature: A Caution (DeCaria 2004)
Moist entropy: a full blown equation with ice effects (Zeng et al. 2005) Or see Emanuel book.
Cloud model based on simpler "frozen moist static energy" (Khairoutdinov and Randall 2003) 

Budgets of entropy in convecting atmopsheres

Dry entropy and its budget in a moist convecting atmosphere (Romps 2008)
Moist entropy budget of a convecting atmosphere (Pauluis and Held 2002 Part I)
Entropy budget of the water substance (Pauluis and Held 2002 Part II)


From thermo to vertical momentum dynamics: book stuff

How to invert (entropy, qv, p) to get density (for buoyancy): HOMEWORK

Wyoming soundings site - skewT or text files

Open questions, assignments, and loose ends for next class:

Mazatlan q, PW example skewt

Testable questions about today's material:

* How many variables are needed to specify the state of moist air (assuming thermo. equilibrium)?
* Do these 3 variables suffice?
* What is the difference between reversible and pseudoadiabatic ascent? A microphysical difference.