tropical convection: a product of convergence. but what drives convergence? one theory: cisk ...
TRANSCRIPT
But What Drives Convergence?
But What Drives Convergence?
ONE THEORY: CISK Conditional Instability of the Second
Kind A Positive Feedback Mechanism . . .
ONE THEORY: CISK Conditional Instability of the Second
Kind A Positive Feedback Mechanism . . .
CISK
Increased Evaporation
Increased Winds
Surface Low:Low Level CONV
Cum. Towers:Upper Level DIV
LHR
Evaporation
CISK
Increased Evaporation
Increased Winds
Surface Low:Low Level CONV
Cum. Towers:Upper Level DIV
LHR
Evaporation
CISK: Convergence Driven by LH Release Aloft
CISK: Convergence Driven by LH Release Aloft
Is this the Whole Story?
Other Process….Other Process….
Barotropic Instability Sea Surface Temperature
Gradients (Lindzen and Nigam)
*All processes play a role to some extent*
Barotropic Instability Sea Surface Temperature
Gradients (Lindzen and Nigam)
*All processes play a role to some extent*
But how do they compare? But how do they compare?
General Circulation:Conv driven by upper-level
Div
Local Circulation:Conv driven by SST
gradient
General Circulation:Conv driven by upper-level
Div
Local Circulation:Conv driven by SST
gradient
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Basic Hypothesis: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 TropicsSmall Changes Large Influence
-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 TropicsSmall Changes Large Influence
Basic Approach/Methodology
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
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
Model DevelopmentModel DevelopmentVertical Temp structure of BL linear function of SST:
Flow in Boundary Layer Incompressible:
Given Temp & Density Pressure via Hydrostatic Eq
Vertical Temp structure of BL linear function of SST:
Flow in Boundary Layer Incompressible:
Given Temp & Density Pressure via Hydrostatic Eq
Momentum Equations: Balance of PGF, Coriolis,
Friction
Momentum Equations: Balance of PGF, Coriolis,
FrictionZonal Component:
Coriolis PGF Turbulent
Stress (friction)
Meridional Component
Zonal Component:
Coriolis PGF Turbulent
Stress (friction)
Meridional Component
Major Approximation/Error:
Major Approximation/Error:
-Lindzen & Nigam assume top of Boundary Layer (taken to be 700mb or 3km) is flat and does not
varyin time
-Convection occurs instantaneously
-These simplifications are later revised in order to Get realistic flow pattern in the model (back-pressure effect)
-Lindzen & Nigam assume top of Boundary Layer (taken to be 700mb or 3km) is flat and does not
varyin time
-Convection occurs instantaneously
-These simplifications are later revised in order to Get realistic flow pattern in the model (back-pressure effect)
Back-Pressure adjustmentBack-Pressure adjustment
-In original model, BL (700mb sfc) is a rigid sfc that can’t 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)
-In original model, BL (700mb sfc) is a rigid sfc that can’t 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)
2 Major New Variables Introduced: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
= 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
Revised Equations in ModelRevised Equations in Model
- Allows for modulation of 700mb sfc with upward vertical motion
variation in top of BL
- Allows for modulation of 700mb sfc with upward vertical motion
variation in top of BL
Note new variables directly proportional to each other:
Note new variables directly proportional to each other:
time scale conv/div time scale conv/div
New SolutionsNew Solutions
If tau=30s looks like old model (excessive convergence)
If tau=3hrs Weak to no convergence (Big back-pressure)
If tau=30mins resembles flow from real data
If tau=30s looks like old model (excessive convergence)
If tau=3hrs Weak to no convergence (Big back-pressure)
If tau=30mins resembles flow from real data
Both Gradients ImportantBoth Gradients Important
Forcing from Meridional -Represents ITCZ better
Forcing from Zonal -Represents SPCZ better
Forcing from Meridional -Represents ITCZ better
Forcing from Zonal -Represents SPCZ better
Criticisms/NotesCriticisms/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*
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*
Inherent Ambiguity: What drives what?
Low level vs. Upper Level
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
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