Geostrophic Adjustment Recall winds adjust to mass for scales larger than L R and mass adjust to wind for scales smaller than L R. In mid-latitude squall.

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Presentation transcript:

Geostrophic Adjustment Recall winds adjust to mass for scales larger than L R and mass adjust to wind for scales smaller than L R. In mid-latitude squall line momentum transport by the rear inflow jet converging with the front updraft inflow produce a mid-level line vortex through momentum transport and the mass field adjusts to the vorticity, ie the pressure lowers along the line vortex. This regionally decreases L R. The melting layer heating function projects on to a small L R because the layer is shallow, further enhancing the line vortex. Hence the squall line grows a quasi-geostrophic component through scale interactions. Eventually the line vortex can ball up creating a circular vortex and a circular convective system of meso-alpha scale proportions.

Dynamic Flywheel The formation of a quasi-geostrophic component to an MCS is significant because : –Quasi-geostrophic flows have long time scales compared to transient gravity wave components, with e-folding times of ½ pendulum day. –The quasi-geostrophic component effectively stores the available energy of the storm’s convective latent heating in its mass balanced circulation. –Essentially, the quasi-geostrophic system works in reverse to what synoptic-small scale flow interaction: The small scale vertical motion, driven by conditionally unstable latent heating, creates a geostrophic flow that would have created the vertical motion had the process run in the forward direction. Hence the tail wags the dog using energy coming from the tail. The mid level line vortex of the middle latitude squall line is such a component that provides a lasting organization of the system. In essence the quasi-geostrophic component of the system, built from cumulus and slant wise processes, stores the energy released in the latent heating into a long time scale balanced quasi-geostrophic circulation.. That is why that circulation can be called a dynamic flywheel.

Tropical Non-Squall Cluster Type 1

Tropical Non-Squall Cluster Type 2

Tropical Non-Squall Cluster Type 3

TCC Organization Long-Lived signature Mean vorticity

Systematic Buildup of the following in a TCC : Vertical Vorticity Horizontal Divergence Vertical Velocity

Density Current MCS Probably most common self-forced MCS Unbalanced organization but density current is slow moving transient Forcing is by lifting air to level of free convection when flow moves over density current. Convection feeds back by building cold pool through evaporation of rain fall. New cumulus tend to form in a line along boundary of density current, forming a linear structure to the deep convection.

Meso- a -Scale Circular Convective Systems Significant projection of heating onto balanced scales above the Rossby radius of deformation. Growth of Vortex from cumulus latent heating –Geostrophic adjustment Deep cumulus heating => Large Rossby Radius => slow and inefficient adjustment Shallow melting zone => more efficient adjustment => rotation => smaller Rossby Radius => more efficient adjustment to deep heating of cumulus updrafts –Mass to wind => line vortex => balls up into circular vortex => shrink rossby radius => efficient geostrophic adjustment to latent heating Role of slantwise convection –Latent heating, ie theta redistribution More efficient than cumulus heating because spread over a larger horizontal scale Driven by melting –Momentum redistribution Form line vortex as with vertical cumulus

Climatology of MCC’s

MCC Evolution

Composite Structure for Pre - MCC Stage

Composite Structure for Mature MCC Stage

Composite Structure for Post MCC Stage

Composite MCC Structure Cotton and Lin

Idealized MCC Structure

Idealized Tropical Cyclone Structure

Tropical Cyclone Extension of the Warm Core middle –level vortex to the surface. Inducement of Ekman pumping Non-linear growth due to increased heating efficiency as vortex strengthens Creation of new instability by increased energy through lowering of pressure Carnot Cycle of heating