Meteorology 1

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Meteorology for Airborne Scientists Henry Fuelberg Department of Meteorology Florida State University

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SARP Meteorology

Transcript of Meteorology 1

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Meteorology forAirborne Scientists

Henry FuelbergDepartment of Meteorology

Florida State University

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Atmospheric Structureand Thermodynamics

Some Basics

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Basic Atmospheric Variables

• Pressure (p)• Temperature (T in oC or K)• Density (ρ) ( or specific volume (α = 1/density))

(kg m-3)• Water vapor content• Three dimensional wind

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Atmospheric Pressure Changes with Altitude

Pressure = Force/Area

1 Pascal = 1 Newton m-2

1 millibar (mb) =

1 hectoPascal (hPa)

Mean sea level pressure =

1013.25 mb

Mean sea level density =

1.25 kg m-3

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Thermal Structureof the Atmosphere

Lapse rate = - ∂T/∂z

Troposphere has + lapse

Stratosphere first isothermal, then – lapse

Troposphere has small scale inversions that vary daily

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Height of the TropopauseVaries with Latitude

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ThermodynamicsParcel = imaginary volume of air to study, like a balloon, separate from environmentAtmosphere acts as an ideal gas—a mixtureEquation of state (ideal gas law)

Press = density x gas constant x temp

gas const = weighted by composition and molecular weight

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First Law of Thermodynamics

• dq = cv dT + pdα heat change = internal energy change + work done to expand or contract vol.

• dq = cp dT – α dp heat change = enthalpy change + …….

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Dry Adiabatic Process• Consider an unsaturated parcel• dq = 0• 0 = cp dT – α dp• Parcels still can change temperature due to expansion and

contraction• Example—parcel expands, expends energy, T becomes cooler• Make substitutions and solve for dT/dz• dT/dz = -g/cp = 9.8 oC/km = Γd (dry adiabatic lapse rate)• Unsat. parcels always follow Γd • Away from clouds and radiative processes, parcels ~ adiabatic

for several days

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Rising air cools

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Potential Temperature (θ)Parcel at T and pΘ is temp. parcel would have if taken dry adiabatically to p = 1000 mbIf p = 1000 mb, Θ = TΘ = T (1000 mb/ p) R/cp R/cp = 0.286 Parcels conserve Θ during ascent, descent, etc. as

long as conditions are adiabatic T is not conserved, it changes at ΓdHow does θ vary in previous figure?Therefore, Θ can serve as a tracer for parcels

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Water Vapor

• Vapor pressure = partial pressure of vapor (mb)• Mixing ratio = mass vapor/mass dry air (g/kg)• Concept of saturation• Dew point temperature = temp to which air must

be cooled to become saturated (oC)• Relative humidity = mixing ratio / sat. mixing ratio

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Saturated Adiabatic Process

• Parcel is saturated• Lift parcel, condensation occurs, latent heat

released, dq ≠ 0• dq = cp dT – α dp• Let dq = latent heat release• Perform some magic• Γs = Γd [ ≤ 1]• Therefore……….. Γs ≤ Γd not a constant• Γs ≈ 5-6 oC/km

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Radiosondes

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Hydrostatic StabilityDisplace parcel upward (could go downward)Will displacement be

Suppressed = Stable Layered clouds, steady precipitation Enhanced = Unstable Towering clouds, showers or Tstorms Neither = Neutral Parcel moves only to where pushed

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Absolute StabilityEnvironmental Lapse Rate less than Wet Adiabatic Rate

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Absolute InstabilityEnvironmental Lapse Rate greater than Dry Adiabatic Rate

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Conditional InstabilityEnvironmental Lapse Rate between the Dry and Wet Adiabatic Rates

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What Causes Wind to Blow ??

It is acted on by forces—most of which we can’t see

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Surface Map Isobars = Lines of constant pressure

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Straight Isobars

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Flow Around Circular Low

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Flow Around Circular High

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Upper Level ChartsPressure is Vertical Coordinate

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500 mb Chart

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Planetary Boundary Layer (PBL)• Lowest layer of atmos—directly influenced by the

surface• PBL vs. Free Atmosphere• What happens in PBL?• Air is heated/cooled from below—radiation• Inversions (stable) at night—suppress mixing• Big lapse rate during day—less stable-lots of mixing• Mechanical Turbulence—roughness (day or night)• Thermal Turbulence—thermals (day)• You can bounce around a lot!!

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• Wind Speed goes to zero at surface (no slip)• Speed increases with height according to Ekman

Theory—direction also changes• The more mixing• the more θ is constant with height• the more mixing ratio constant with height• Height of PBL deep during day, shallow at night • Depth determined by– Temperature– Wind Speed– Others

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Transporting Air From Surface to Higher Levels

Winds are stronger thereWind direction often changes with height

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Jet Streams

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Middle Latitude Wave Cyclones

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Major Airstreams in Midlat Cyclone

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Smaller Scale CirculationsAlso Provide Vertical Transport

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Sea/Land Breezes

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Mountain/Valley Breezes

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Santa Ana Winds & Fires

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Wires Fanned by Santa Ana Winds

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Thunderstorms-Major Vertical Transporters

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Lightning Creates NOx

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FOG

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Radiation Fog

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Advection Fog

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Yesterday’s Fog (4:46 PM)

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This morning

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Neat PictureContrails Cover 0.1% of Earth’s Surface

Eastern France

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TrajectoriesBackward in time—where did air come from? What path did it take?Forward in time—where is air going to?

What path will it take?Several possible procedures

Isobaric—air keeps same pressure--move parcel by horizontal winds

Isentropic—air follows θ surface—move air by winds on the θ surface

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• Kinematic method—move parcels by three-dimensional winds—most popular today

Procedure for Forward TrajectoriesStart with 4-D grid of 3-D wind

components—hope data every few hoursMove parcel one time step by these windsNow at a new location and a new time

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• Take winds at new location and time and move parcel another time step

• Repeat the process until you reach theending time that you specify

• Limit is usually 5-10 days• After that uncertainties are too great

• If backward trajectories, process goes in reverse

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Examples from ARCTAS-200810 days back from selected flight legs

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Heading to N CA

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Heading to S CA

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Particle Dispersion Models•Establish locations of emissions and rates of emission•Release particles to simulate emission rate•Particles have specified mass and are released at specified rate•Three-dimensional winds move the particles•Can then watch the transport of the emissions

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WRF Nested Grid 45 km, 15 km, 5 km

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Spring

Summer

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Sources of Real Time Information

Satellite, Radar, Surface Analyses,Upper Air Analyses, Forecasts

http://www.rap.ucar.edu/weather/

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Surface Plot 7 PM

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Edward AFB Radar 8 PM

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Enhanced IR Image 8 PM

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Surface Plot 11 AM

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Visible Images 10 AM

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Edwards AFB Monday 5 AM

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500 mb Analysis 5 AM Monday

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Forecast Products

NOAA National Center for Environmental Prediction

http://www.nco.ncep.noaa.gov

We look at 54 h progs valid11 AM Wednesday

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SFC Forecast

H

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Clouds below 6000 ft

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850 mb Forecast

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700 mb Forecast

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500 mb Forecast500 mb

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Zoom to CA Area

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300 mb Forecast

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Your Local NWS Office

http://www.srh.noaa.gov

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Other Interesting Sites

Storm Prediction Center http://www.spc.noaa.gov

National Hurricane Center http://www.nhc.noaa.gov