How to Calculate the Geostrophic Wind Using ‘Real’ Data

Slides:



Advertisements
Similar presentations
Air Motions Geology 390 WSUV Dr. Robert M MacKay.
Advertisements

Air Pressure, Forces, and Motion Meteorology 101 Dr. Robert M MacKay.
Chapter 4. Atmospheric Pressure and Wind
Pressure Gradient Force How does the air move as a result of the pressure gradient force? 996hPa 998hPa 1000hPa 1002hPa LOW PRESSURE HIGH PRESSURE (1)
Recitation Geostrophic Balance Thermal Wind Effect of Friction.
Air Pressure and Wind Pressure: the amount of force exerted per unit of surface area Pressure can be increased in 2 ways 1.By increasing density or decreasing.
Fig. 1. NCEP/NCAR Composite analysis 24 hours prior to event onset (T-24) for a) 250-hPa vector wind, b) 500-hPa geopotential height, c) 850-hPa temperature,
Atmospheric Motion ENVI 1400: Lecture 3.
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:
Steady State General Ocean Circulation “steady state” means: constant in time, no accelerations or Sum of all forces = 0 Outline:1. Ekman dynamics (Coriolis~Friction)
1. The horizontal equations of motion: smaller-scale motion 2. The vertical equation of motion 3. The thermal wind ATOC 4720 class34.
Geostrophic and thermal wind. Reminder Geostrophic wind in pressure coordinates In the free atmosphere, wind is usually close to geostrophic. The departure.
AOSS 321, Winter 2009 Earth System Dynamics Lecture 4 1/20/2009 Christiane Jablonowski Eric Hetland
Chapter 1. Introduction 1.1 Atmospheric Continuum –Continuous fluid medium –“mass point” = air parcel (or air particle) –Field variables: p, , T and their.
Lab 3 Estimating the Geostrophic Wind.  (or “Now I’ve seen it all”!)  Last week, we learned that we could estimate a derivative quantity using finite.
EOSC 112: THE FLUID EARTH CORIOLIS EFFECT AND GEOSTROPHY Atm3 Read: Kump et al. Chap.4, p Why do weather / climate vary around the globe? Why is.
AOSS 321, Winter 2009 Earth System Dynamics Lecture 9 2/5/2009 Christiane Jablonowski Eric Hetland
AOSS 321, Winter 2009 Earth Systems Dynamics Lecture 12 2/17/2009
Chapter 6: Air Pressure and Winds Atmospheric pressure Atmospheric pressure Measuring air pressure Measuring air pressure Surface and upper-air charts.
Warning! In this unit, we switch from thinking in 1-D to 3-D on a rotating sphere Intuition from daily life doesn’t work nearly as well for this material!
Atmospheric Force Balances
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.
What Causes the Wind? Newton’s Second Law F = ma.
Basic dynamics  The equations of motion and continuity Scaling Hydrostatic relation Boussinesq approximation  Geostrophic balance in ocean’s interior.
Atmospheric Motions & Climate
What set the atmosphere in motion?. Review of last lecture Thickness of the atmosphere: less than 2% of Earth’s thickness Thickness of the atmosphere:
Atmospheric Forces Nick Bassill April 8 th Why Are Forces Important? When we speak of “forces,” we’re really describing why the air in the atmosphere.
Chapter 7 cover. Figure 7.1 Figure 7.2 Figure mb/km 115G150 knots.
StationTempSLP trend CCWind dir Dew point Precip A Low, steady FallingCirrostratusE to SEModerateNo B Low, steady FallingOvercast, (nb)stratus E to SEModerateChance.
Navigation: A Closer Look. Recap: A coordinate system is used to locate your position on earth. The science of locating ones position is called navigation.
EVAT 554 OCEAN-ATMOSPHERE DYNAMICS FILTERING OF EQUATIONS FOR ATMOSPHERE (CONT) LECTURE 6 (Reference: Peixoto & Oort, Chapter 3)
Physical Oceanography SACS/AAPT Spring Meeting March 29, 2003 Coastal Carolina University.
Ekman Flow September 27, 2006.
Basic dynamics ●The equations of motion and continuity Scaling
Chapter 6: Air Pressure and Winds Atmospheric pressure Atmospheric pressure Measuring air pressure Measuring air pressure Surface and upper-air charts.
NATS 101 Section 13: Lecture 15 Why does the wind blow? Part I.
Atmospheric Motion SOEE1400: Lecture 7. Plan of lecture 1.Forces on the air 2.Pressure gradient force 3.Coriolis force 4.Geostrophic wind 5.Effects of.
GEU 0047: Meteorology Lecture 8 Air Pressure and Winds.
OCN 5401 Chapter 5 Equations of Motion Instructor: Dr. George A. Maul / X 7453.
Wind Wind is the general horizontal motion of air from one location to another based on differences in air pressure Wind is the general horizontal motion.
Synoptic Scale Balance Equations Using scale analysis (to identify the dominant ‘forces at work’) and manipulating the equations of motion we can arrive.
--- Introduction to Geophysical Fluid Dynamics Ch. 6 Fundamentals of Atmospheric/Ocean Modeling.
AOSS 401, Fall 2007 Lecture 11 October 1, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Lecture 7 Forces (gravity, pressure gradient force)
Basic dynamics ●The equations of motion and continuity Scaling Hydrostatic relation Boussinesq approximation ●Geostrophic balance in ocean’s interior.
You are here! But how do I know where here is? Longitude and Latitude.
Isobars and wind barbs sea level pressure. factors affecting wind wind is the result of horizontal differences in pressure air flows from higher to lower.
1. The geostrophic wind: scale analysis 2. Effects of friction 3. The gradient wind ATOC 4720 class33.
I. Air Pressure 19.1 Understanding Air Pressure  A)  A) The pressure exerted by the weight of air.  B)  B) Air pressure is exerted in all directions.
SO254 – Forces and the equation of motion
Synoptic Scale Balance Equations
Dynamics I: Basic forces
Winds and Forces Atmospheric Sciences 101.
2-2 Acceleration At the start of a race what happens?
Dynamical Balance in the Earth’s Atmosphere
ATOC 4720 class31 1. Coordinate systems 2. Forces.
ATOC 4720 class32 1. Forces 2. The horizontal equation of motion.
Hydrostatics Dp Dz Air Parcel g.
Latitude and Longitude
--- Introduction to Geophysical Fluid Dynamics
Chapter 2 – Mapping Our World
Geostrophic and thermal wind
Fundamental Force Balances
Circulation in the atmosphere
AOSS 401, Fall 2013 Lecture 3 Coriolis Force September 10, 2013
Latitude and Longitude
Richard B. Rood (Room 2525, SRB)
Isobars and wind barbs sea level pressure.
LATITUDES AND LONGITUDES
Pressure Pressure Gradient Force Coriolis Force
Presentation transcript:

How to Calculate the Geostrophic Wind Using ‘Real’ Data Geostrophic Wind Eqns. As you know from class, geostrophy represents an exact balance between the pressure gradient force (PGF) and the Coriolis force (f; units of 1/s). In equations (1), the PGF is represented by the horizontal partial derivative of the geopotential. (1) In practice, the horizontal partial derivates in (1) can be represented by the change in height (z) over the horizontal distance (latitude for y; longitude for x) on a constant pressure map. (2) Coriolis Force (f) ϕ = latitude and Ω is the angular velocity of the Earth’s rotation Useful #’s: 0.5 m/s = 1 knot; 1 degree of latitude = 111 km; g = gravity = 9.8 m/s2

Fig. 1: 500 hPa Heights, Wind Vectors (knots) B C

Fig. 2 700 hPa Heights 250hPa Heights X X X X