Tropical Convection: A Product of Convergence - PowerPoint PPT Presentation

1 / 24
About This Presentation
Title:

Tropical Convection: A Product of Convergence

Description:

Conditional Instability of the Second Kind. A Positive Feedback ... Time Adjustment of 30 mins chosen b/c it looks the nicest' (No theoretical Justification) ... – PowerPoint PPT presentation

Number of Views:62
Avg rating:3.0/5.0
Slides: 25
Provided by: patric225
Category:

less

Transcript and Presenter's Notes

Title: Tropical Convection: A Product of Convergence


1
Tropical Convection A Product of Convergence
2
But What Drives Convergence?
  • ONE THEORY CISK
  • Conditional Instability of the Second Kind
  • A Positive Feedback Mechanism . . .

3
(No Transcript)
4
CISK Convergence Driven by LH Release Aloft
Is this the Whole Story?
5
Other Process.
  • Barotropic Instability
  • Sea Surface Temperature Gradients
  • (Lindzen and Nigam)
  • All processes play a role to some extent

6
But how do they compare?
  • General Circulation
  • Conv driven by upper-level Div
  • Local Circulation
  • Conv driven by SST gradient

7
Basic Hypothesis
  • -Momentum Balance of Hadley circulation aloft
    does not account for total low-level moisture
    Convergence
  • -SST directly influence Convection apart from
    thermodynamic properties
  • -Variation or Gradient in SST pattern important
    for Convection
  • In Tropics
  • Small Changes Large Influence

8
Environment of Tropical Ocean
9
Basic Approach/Methodology
  • ATS capped at 700mb (height of inversion)
  • Inversion decouples upper ATS from below
  • No influence from LHR in cumulus towers (CISK)
  • Convergence in lower layer driven by SST Gradient
  • Pressure Gradient
  • Well Mixed BL SST and gradients
    correlated in vertical
  • Model Eddy (anomalous) surface flow
  • Zonally averaged flow well represented by Hadley
    Circulation
  • Compare model with observational data (FGGE) in
    order to determine relative importance of
    low-level forcing in eddy convergence

10
Model Development
  • Vertical Temp structure of BL linear function of
    SST
  • Flow in Boundary Layer Incompressible
  • Given Temp Density Pressure via
    Hydrostatic Eq

11
Momentum Equations Balance of PGF, Coriolis,
Friction
  • Zonal Component
  • Coriolis PGF Turbulent
    Stress (friction)
  • Meridional Component


12
  • Compute Eddy SLP from Observed temperature using

13
Initial Results

14
Major Approximation/Error
  • -Lindzen Nigam assume top of Boundary Layer
  • (taken to be 700mb or 3km) is flat and does not
    vary
  • in time
  • -Convection occurs instantaneously
  • -These simplifications are later revised in order
    to
  • Get realistic flow pattern in the model
  • (back-pressure effect)

15
Back-Pressure adjustment
  • -In original model, BL (700mb sfc) is a rigid sfc
    that cant be modified
  • -In reality, vertical motion above SFC LOW raises
    the top of the BL (700mb sfc) and this adiabatic
    expansion acts to cool the lower tropopause
    raises pressure Negative
    feedback
  • -This cooling is eventually dampened by ample LHR
  • But it takes time for convective clouds to
    develop (30mins)

16
2 Major New Variables Introduced
  • Deviation of 700mb layer from flat 3km sfc
  • Proportional to uptake of mass via
    convergence
  • Proportional to cooling of tropopause
  • If large cooling offsets warm SST
    Convergence suppressed
  • Time Scale Cloud development time
  • Represents adjustment time of ATS to reach
    steady state
  • If small, LHR quickly compensates cooling from
    h
  • Convergence excessive

17
Revised Equations in Model
  • Allows for modulation of 700mb sfc with upward
    vertical motion
  • variation in top of BL

18
Note new variables directly proportional to each
other
  • time scale
    conv/div

19
New Solutions
  • If tau30s looks like old model
    (excessive convergence)
  • If tau3hrs Weak to no convergence (Big
    back-pressure)
  • If tau30mins resembles flow from real
    data

20
Solution with tau30mins
21
Both Gradients Important
  • Forcing from Meridional
  • -Represents ITCZ better
  • Forcing from Zonal
  • -Represents SPCZ better

22
(No Transcript)
23
Criticisms/Notes
  • Questionable parameterizations
  • -3km can be considered too high for mean
    Boundary Layer
  • -Time Adjustment of 30 mins chosen b/c it looks
    the nicest
  • (No theoretical Justification)
  • Poor Results for NH Winter
  • -Boundary Layer is shallower
  • -Greater influence from motions aloft
  • Are Results repeatable
  • -How does model compare against other reanalysis
  • and data sets (future work)
  • Conceptual Problem

24
Inherent Ambiguity What drives what?Low level
vs. Upper Level
  • SST gradient Pressure gradient
    Low-level flow
  • (Lindzen Nigam)
  • Deep Convection/LHR Pressure gradient
    Low-level flow
  • (Gill others)
  • Different Forcing can yield similar results
  • Each Mechanism only valid given assumptions made
Write a Comment
User Comments (0)
About PowerShow.com