Richard B. Rood (Room 2525, SRB)

Slides:



Advertisements
Similar presentations
The Quasi-Geostrophic Omega Equation (without friction and diabatic terms) We will now develop the Trenberth (1978)* modification to the QG Omega equation.
Advertisements

Class #5: Air pressure and winds Chapter 8 1Class #5 Tuesday, July 13, 2010.
Recitation Geostrophic Balance Thermal Wind Effect of Friction.
SO441 Synoptic Meteorology
Q-G vorticity equation Q-G thermodynamic equation We now have two equations in two unknowns,  and  We will solve these to find an equation for , the.
UPPER AIR DYNAMICS (continued) MSC 243 Lecture #8, 10/22/09.
Leila M. V. Carvalho Dept. Geography, UCSB
General Circulation and Kinetic Energy
Vorticity.
MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 10 Atmospheric Dynamics Dr. Eugene Cordero Ahrens: Chapter 9 W&H:
What Makes the Wind Blow? ATS 351 Lecture 8 October 26, 2009.
AOSS 321, Winter 2009 Earth Systems Dynamics Lecture 12 2/17/2009
General Circulation & Thermal Wind
Things to look for on the weather maps Visible and IR satellite images (& radar too): Look at cloud movements and locations - do they correlate with what.
AOSS 401, Fall 2006 Lecture 8 September 24, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2006 Lecture 19 October 26, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
General Circulation of the Atmosphere Lisa Goddard 19 September 2006.
AOSS 401, Fall 2007 Lecture 24 November 07, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2007 Lecture 27 November 28, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Alternative derivation of Sverdrup Relation Construct vorticity equation from geostrophic balance (1) (2)  Integrating over the whole ocean depth, we.
Structure and dynamical characteristics of mid-latitude fronts.
ADVENTURE IN SYNOPTIC DYNAMICS HISTORY
AOSS 401, Fall 2007 Lecture 25 November 09, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Thickness and Thermal Wind /aos101/wk12.html /aos101/wk12.html.
AOSS 401, Fall 2007 Lecture 15 October 17, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
METR March Review Hydrostatic balance Ideal gas law p = ρ R d T v, ρ = p / R d T v Take layer average virtual temperature, R and g as constants.
AOSS 401, Fall 2006 Lecture 9 September 26, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2007 Lecture 12 October 3, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
ATS/ESS 452: Synoptic Meteorology
AOSS 401, Fall 2007 Lecture 23 November 05, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Synoptic Scale Balance Equations Using scale analysis (to identify the dominant ‘forces at work’) and manipulating the equations of motion we can arrive.
AOSS 401, Fall 2006 Lecture 17 October 22, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2007 Lecture 21 October 31, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2007 Lecture 3 September 10, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
AOSS 401, Fall 2006 Lecture 18 October 24, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
ATS/ESS 452: Synoptic Meteorology Friday 08 January 2016 Review Material Overview of Maps Equations of Motion Advection Continuity.
AOSS 401, Fall 2006 Lecture 16 October 19, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
The vector measure of rotation around a point
Atmospheric Dynamics Suzanne Gray (University of Reading) With thanks to Alan Gadian and Geraint Vaughan. Basic dynamical concepts.
Class #17 Monday, February 16, Class #17: Monday, February 16 Surface pressure and winds Vertical motions Jet streams aloft.
ATS/ESS 452: Synoptic Meteorology Wednesday 09/10/2014 Quiz! (Short?) Weather Discussion Continue Review Material Geostrophic Wind Continuity Vorticity.
Weather Basics Air Pressure and Winds. Air Pressure Air has a mass and exerts a force called atmospheric pressure Air pressure is measured in millibars.
AOSS 401, Fall 2006 Lecture 7 September 21, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
PRESSURE & WIND, GENERAL CIRCULATION, JET STREAMS.
SO254 - Advection.
SO254 – relative and planetary vorticity
Synoptic Scale Balance Equations
Vorticity Vertical component of vorticity: i.e., the rotation about the local vertical There are three types of vorticity used in geophysical fluid dynamics.
Thickness and Thermal Wind
Planetary (Rossby) Waves
Atmospheric Fluid Dynamics
ATS/ESS 452: Synoptic Meteorology
PRESSURE & WIND, GENERAL CIRCULATION, JET STREAMS
Thickness and Thermal Wind
Cause of vertical motions
MADISON’S CURRENT WEATHER
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
EART30351 Lecture 9.
AOSS 401, Fall 2013 Lecture 3 Coriolis Force September 10, 2013
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
Richard B. Rood (Room 2525, SRB)
Air Pressure and Winds Earth Science Ch. 19.
Vorticity Objectives Define Vorticity
Vorticity Objectives Define Vorticity
Vorticity Objectives Define Vorticity
Presentation transcript:

Richard B. Rood (Room 2525, SRB) AOSS 401 Geophysical Fluid Dynamics: Atmospheric Dynamics Prepared: 20131105 Vorticity / Flow Richard B. Rood (Room 2525, SRB) rbrood@umich.edu 734-647-3530 Cell: 301-526-8572

Class News Ctools site (AOSS 401 001 F13) Second Examination on December 10, 2013 Homework Posted on Ctools / Due on Thursday 11/7/13

Weather National Weather Service Weather Underground Model forecasts: Weather Underground NCAR Research Applications Program

Outline Vorticity and Flow

Vorticity Equation Changes in relative vorticity are caused by: DIVERGENCE TILTING SOLENOIDAL or BAROCLINIC Changes in relative vorticity are caused by: Divergence Tilting Gradients in density on a pressure surface Advection

Scale Analysis of the Vorticity Equation Changes in relative vorticity are caused by: Divergence Tilting Gradients in density Advection Which of these are most important for large-scale flows? Back to scale analysis…

Scale factors for “large-scale” mid-latitude

Terms in Vorticity Equation Time rate of change Horizontal advection Divergence Planetary vorticity advection Time rate of change Horizontal advection Vertical advection Divergence Tilting Planetary vorticity advection Solenoidal term

Assume balance among terms of 10-10s-2

Two important definitions barotropic – density depends only on pressure. And by the ideal gas equation, surfaces of constant pressure, are surfaces of constant density, are surfaces of constant temperature. baroclinic – density depends on pressure and temperature.

Barotropic Potential Vorticity We can learn a lot about the atmosphere by considering the barotropic potential vorticity

Barotropic Potential Vorticity Assume constant density Integrate with height, z1  z2 over a layer of depth H.

Remember the Thermal Wind? p is an independent variable, a coordinate. Hence, x and y derivatives are taken with p constant.

Implications of Thermal Wind for a Barotropic Fluid… Barotropic: temperature is constant on a pressure surface This means Geostrophic wind is constant with height in pressure coordinates in a barotropic fluid

Barotropic Potential Vorticity

What happens if the depth (H) is constant? Conservation of potential vorticity becomes conservation of absolute vorticity…

Barotropic Potential Vorticity Potential vorticity is a measure of absolute vorticity relative to the depth of the vortex. What happens if the depth (H) changes?

Relative vorticity with change of depth

The vortex went over the mountain Surface with a hill.

Vorticity and depth There is a relationship between depth and vorticity. As the depth of the vortex changes, the relative vorticity has to change in order to conserve the potential vorticity. We have now linked the rotational and irrotational components of the wind. divergence and curl vorticity and divergence Potential vorticity indicates an interplay between relative and planetary vorticity through conservation of absolute angular momentum.

Let’s explicitly map these ideas to the Earth

Local vertical / planetary vorticity

relative vorticity/planetary vorticity

Compare relative vorticity to planetary vorticity for large-scale and middle latitudes planetary vorticity is usually larger than relative vorticity

Relative and planetary vorticity Planetary vorticity is cyclonic is positive vorticity Planetary vorticity, in middle latitudes, is usually larger than relative vorticity A growing cyclone “adds to” the planetary vorticity. Lows are intense A growing anticyclone “opposes” the planetary vorticity. Highs are less intense

Compare relative vorticity to planetary vorticity and to divergence Flow is rotationally dominated, but divergence is crucial to understanding the flow.

Return to our simple form of potential vorticity From scaled equation, with assumption of constant density.

Fluid of changing depth Stretching and shrinking of a column will change the relative vorticity.

Application to flow on the Earth

What might cause this wave-like flow?

Flow over a mountain Mountain

Use our simple form of potential vorticity From scaled equation, with assumption of constant density and temperature.

Flow over a mountain (long in the north-south) (can’t go around the mountain) west east

Flow over a mountain Depth, H Mountain west east

Flow over a mountain (assume flow is adiabatic) θ + Δθ Depth, H θ Mountain west east

Flow over a mountain (far upstream constant zonal flow) θ + Δθ ζ=0 Depth, H θ Mountain west east

Use the barotropic potential vorticity equation From scaled equation, with assumption of constant density and temperature.

What happens as air gets to mountain? θ + Δθ ζ=0 Depth, H θ Mountain west east

What happens as air gets to mountain? Air is lifted. Lifting higher at ground than upper air. (pressure gradient force spreads it out) θ + Δθ ζ=0 Depth, H θ Mountain west east

What happens as air gets to mountain? Air is lifted. Lifting higher at ground than upper air. (pressure gradient force spreads it out) θ + Δθ ζ=0 Depth, H +ΔH θ Mountain west east

What happens as air gets to mountain? Air is lifted. Lifting higher at ground than upper air. (pressure gradient force spreads it out) θ + Δθ ζ must increase Depth, H +ΔH θ Mountain west east

What does it mean for the relative vorticity to increase?

What happens in these waves? Loses cyclonic vorticity Same as gains anticyclonic vorticity Gains cyclonic vorticity

Or schematically Rotational Shear Cyclonic Anticyclonic

What happens as air gets to mountain? Air turns cyclonically to increase vorticity. In northern hemisphere turns north. θ + Δθ ζ must increase Depth, H +ΔH θ Mountain west east

In the (east-west, north-south) plane MOUNTAINS Depth, H Depth, H +ΔH n s west east

What happens as air goes over mountain? Air turns anti-cyclonically to decrease vorticity. In northern hemisphere turns south. θ + Δθ ζ must decrease Depth, H -ΔH θ Mountain west east

In the (east-west, north-south) plane MOUNTAINS Depth, H Depth, H +ΔH Depth, H -ΔH n s west east

What happens as air goes down mountain? Air turns cyclonically to increase vorticity. In northern hemisphere turns north. θ + Δθ ζ must increase Depth, H +ΔH θ Mountain west east

In the (east-west, north-south) plane MOUNTAINS Depth, H Depth, H +ΔH Depth, H -ΔH Depth, H +ΔH n Arrives here with northward momentum “Overshoots” Stretching here causes relative vorticity to increase; northward turning s west east

What is happening with planetary vorticity What is happening with planetary vorticity? (In the (east-west, north-south) plane) MOUNTAINS Depth, H Depth, H +ΔH Depth, H -ΔH Depth, H +ΔH n f is greater for deflections to north f is less for deflections to south s west east

What is happening with planetary vorticity What is happening with planetary vorticity? (In the (east-west, north-south) plane) MOUNTAINS Depth, H Depth, H +ΔH Depth, H -ΔH Depth, H +ΔH Has an excess of potential vorticity; relative vorticity must decrease n f = f1 ζ = ζ1 H = H1 f = f2 > f1 ζ = ζ2 = ζ1 H = H2 = H1 s west east

Excursion into the atmosphere

“Colorado Lows”

What happens if wind is from east? θ + Δθ θ Mountain west east

What is happening with planetary vorticity What is happening with planetary vorticity? (In the (east-west, north-south) plane) MOUNTAINS Depth, H Depth, H +ΔH Depth, H -ΔH Depth, H +ΔH n Flow from east: planetary and relative vorticity offset each other; no overshoot or undershoot. s west east

Consider the vertical structure more

Where is this flow more barotropic? 10 m/s 5 m/s 20 m/s 30 m/s B, cooler A, warmer - p, vertical y, north

Idealized vertical cross section

Vorticity on Large Scales Remember, vorticity is caused by Wind shear Rotation in the flow Can we identify these on weather maps? (The following maps come from http://www.aos.wisc.edu/weather/)

300 mb Wind Speed

Where is there positive vorticity?

500 mb Vorticity

Thermal Wind Remember, thermal wind relates Vertical shear of geostrophic wind Horizontal temperature gradients Can we identify these on weather maps?

Where are the strongest ?

850 mb Temperature

Convergence/Divergence Remember, vertical motion on large scales directly related to Convergence/divergence of ageostrophic wind Curvature in the flow Can we identify these on weather maps?

Where are surface lows/highs?

Surface Precipitation

850 mb Temperature

Concepts Vorticity: shear and curvature Why is curvature vorticity (as opposed to shear vorticity) usually associated with developing low pressure systems? Divergence and convergence and location of surface high and low pressure systems Thermal wind—vertical shear of the horizontal wind and horizontal temperature gradients

Concepts Features commonly found together Coincidence? Jet stream Upper level positive vorticity Fronts Midlatitude cyclones (low pressure systems) Coincidence? More on this later…

Mid-latitude cyclones What we know: Low pressure systems Form through spinup of low-level positive vorticity Divergence/convergence is key This is just the beginning… Always closely associated with fronts—why? Sometimes develop rapidly, sometimes not at all—why?

The mid-latitude cyclone

Mid-latitude cyclones: Norwegian Cyclone Model

Fronts and Precipitation Norwegian Cyclone Model CloudSat Radar

Idealized vertical cross section

Cold and warm advection

Lifting and sinking

Increasing the pressure gradient force

Almost Weather

Mid-latitude cyclones: Norwegian Cyclone Model http://www.srh.weather.gov/jetstream/synoptic/cyclone.htm

Weather National Weather Service Weather Underground Model forecasts: Weather Underground NCAR Research Applications Program