meteorology for airborne scientists

Upload: jpeterson1

Post on 30-May-2018

219 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/9/2019 Meteorology for Airborne Scientists

    1/59

    Meteorology for

    Airborne Scien1sts

    Henry Fuelberg

    Department of MeteorologyFlorida State University

  • 8/9/2019 Meteorology for Airborne Scientists

    2/59

    Avia1on Related Parameters

    to Forecast

    Cloud Cover and Fog Precipita1on WindsSurface and Alo

    Temperature

    Humidity

  • 8/9/2019 Meteorology for Airborne Scientists

    3/59

    FirstA Few Basics

    P = RT

  • 8/9/2019 Meteorology for Airborne Scientists

    4/59

    Atmospheric Pressure

    Pressure = Force/Area

    Decreases with al1tude

    Pascal = Newton m2

    millibar (mb) =

    hectoPascal (hPa)

    Mean sea level pressure =

    03.25 mb (or hPa)

  • 8/9/2019 Meteorology for Airborne Scientists

    5/59

    Dry Adiaba1c Process

    st Law dh = cv dT + p d OR dh = cp dT dp Consider an unsaturated parcel, let dq = 0 0 = cp dT dp Parcels s1ll can change temperature due to expansion

    and contrac1on Exampleparcel expands, expends energy, T gets cooler Make subs1tu1ons and solve for dT/dz dT/dz = g/cp = 9.8 oC/km = d (dry adiaba1c lapse rate) d is posi1ve if T decreases with height, nega1ve forinversions Unsat. parcels always follow d Away from clouds and radia1ve processes, parcels

    ~ adiaba1c for several days

  • 8/9/2019 Meteorology for Airborne Scientists

    6/59

    Rising air cools, Subsiding air warms

  • 8/9/2019 Meteorology for Airborne Scientists

    7/59

    Poten1al Temperature ()Have a parcel at T and p

    is temp. parcel would have if taken dry

    adiaba1cally to p = 000 mb

    If p = 000 mb, = T

    = T (000 mb/ p) R/cp R/cp = 0.286

    Parcels conserve during ascent, descent, etc. as

    long as condi1ons are adiaba1cT is not conserved, it changes at d

    Therefore, can serve as a tracer for parcels

  • 8/9/2019 Meteorology for Airborne Scientists

    8/59

    Water Vapor

    Vapor pressure = par1al pressure of vapor (mb) Mixing ra1o = mass vapor/mass dry air (g/kg) Concept of satura1on Dew point temperature = temp to which air must

    be cooled to become saturated (oC)

    Rela1ve humidity = mixing ra1o / sat. mixing ra1o( how chose to sat. is parcel?)

  • 8/9/2019 Meteorology for Airborne Scientists

    9/59

    Saturated Adiaba1c Process

    Parcel is saturated Li parcel, condensa1on occurs, latent heat

    released, dq 0

    dq = cp dT dp Let dq = latent heat release Perform some magic, get a complicated equa1on s d not a constant, depends on how muchvapor is in the air s 6 oC/km

  • 8/9/2019 Meteorology for Airborne Scientists

    10/59

  • 8/9/2019 Meteorology for Airborne Scientists

    11/59

    Radiosondes

  • 8/9/2019 Meteorology for Airborne Scientists

    12/59

  • 8/9/2019 Meteorology for Airborne Scientists

    13/59

    Hydrosta1c Stability

    Displace parcel upward (could go downward)

    Will displacement be

    Suppressed = Stable

    Layered clouds, steady precipita1on

    Enhanced = Unstable

    Towering clouds, showers or Tstorms

    Neither = NeutralParcel moves only to where pushed

  • 8/9/2019 Meteorology for Airborne Scientists

    14/59

  • 8/9/2019 Meteorology for Airborne Scientists

    15/59

    Absolute Instability

    Environ. Lapse Rate greater than Dry Adiaba1c Rate (> 0 deg/km)

  • 8/9/2019 Meteorology for Airborne Scientists

    16/59

    Condi1onal Instability

    Environmental Lapse Rate between the Dry and Wet

    Adiaba1c Rates (between 60 deg/km)

  • 8/9/2019 Meteorology for Airborne Scientists

    17/59

    What Causes Wind to Blow ??

    It is acted on by forcesmostof which we cant see

  • 8/9/2019 Meteorology for Airborne Scientists

    18/59

    Straight IsobarsAbove Surface

    Isobars

  • 8/9/2019 Meteorology for Airborne Scientists

    19/59

    Flow Around Circular Low

    Include Centripetal Accelera1on

  • 8/9/2019 Meteorology for Airborne Scientists

    20/59

    Flow Around Circular High

    Include Centripetal Accelera1on

  • 8/9/2019 Meteorology for Airborne Scientists

    21/59

    Upper Level Charts

    Pressure is Ver1cal Coordinate (Not Z)

  • 8/9/2019 Meteorology for Airborne Scientists

    22/59

    500 mb Chart 8,000 or 5.5 km

    Height Contours Replace Isobars

  • 8/9/2019 Meteorology for Airborne Scientists

    23/59

    Surface MapIsobars = Lines of constant pressure

  • 8/9/2019 Meteorology for Airborne Scientists

    24/59

    Straight IsobarsNear Surface

  • 8/9/2019 Meteorology for Airborne Scientists

    25/59

    Planetary Boundary Layer (PBL) Lowest layer of atmosdirectly influenced by thesurface PBL vs. Free Atmosphere What happens in PBL? Air is heated/cooled from belowradia1on Inversions (stable) at nightsuppress mixing Big lapse rate during dayless stablelots of mixing

    Mechanical Turbulenceroughness (day or night) Thermal Turbulencethermals (day) You can bounce around a lot!!

  • 8/9/2019 Meteorology for Airborne Scientists

    26/59

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

    Theorydirec1on also changes The more mixing the more is constant with height the more mixing ra1o constant with height Height of PBL deep during day, shallow at night Depth determined by

    TemperatureWind SpeedOthers

  • 8/9/2019 Meteorology for Airborne Scientists

    27/59

  • 8/9/2019 Meteorology for Airborne Scientists

    28/59

  • 8/9/2019 Meteorology for Airborne Scientists

    29/59

    Marine Layer

    Strong subsidence due to high pressure

    Warm, dry sinking air

    Cool moist air

    Cold water

    T inversion

  • 8/9/2019 Meteorology for Airborne Scientists

    30/59

    Weaker High Pressure

    Clouds near top of marine layer

  • 8/9/2019 Meteorology for Airborne Scientists

    31/59

    Low pressure allows marine layer to

    deepen as much as 6,000 .

  • 8/9/2019 Meteorology for Airborne Scientists

    32/59

    Smaller Scale Circula1ons

    Are Superimposed onLarger Scale Flow

  • 8/9/2019 Meteorology for Airborne Scientists

    33/59

    Sea/Land Breezes

  • 8/9/2019 Meteorology for Airborne Scientists

    34/59

    Mountain/Valley Breezes

  • 8/9/2019 Meteorology for Airborne Scientists

    35/59

  • 8/9/2019 Meteorology for Airborne Scientists

    36/59

    Clouds

    Most clouds are due to rising air

    All precipita1on is due to rising air

  • 8/9/2019 Meteorology for Airborne Scientists

    37/59

    0 Basic Cloud Types

  • 8/9/2019 Meteorology for Airborne Scientists

    38/59

    FOG

    . Cooling air to satura1on

    2. Increasing Water Vapor

    content to reach satura1on

  • 8/9/2019 Meteorology for Airborne Scientists

    39/59

    Radia1on Fog

  • 8/9/2019 Meteorology for Airborne Scientists

    40/59

  • 8/9/2019 Meteorology for Airborne Scientists

    41/59

    History or Future of Air

    Trajectories

    Backward in 1mewhere did air come from?

    What path did it take?

    Forward in 1mewhere is air going to?What path will it take?

    Kinema1c methodmove parcels using

    threedimensional winds

  • 8/9/2019 Meteorology for Airborne Scientists

    42/59

    WRF Nested Grid 45 km, 5 km, 5 km

  • 8/9/2019 Meteorology for Airborne Scientists

    43/59

    Procedure for Forward Trajectories

    Start with 4D grid of 3D wind componentshope dataevery few hours

    Move parcel one 1me step by these winds

    Now at a new 3D loca1on and a new 1me

    Take winds at new loca1on and 1me and move parcelanother 1me step Repeat the process un1l you reach desired ending 1me Limit is usually 50 days

    Aer that uncertain1es are too great If backward trajectories, process goes in reverse

  • 8/9/2019 Meteorology for Airborne Scientists

    44/59

  • 8/9/2019 Meteorology for Airborne Scientists

    45/59

  • 8/9/2019 Meteorology for Airborne Scientists

    46/59

    Par1cle Dispersion Models

    Establish loca1ons of emissions and rates of emissionRelease par1cles to simulate emission ratePar1cles have specified mass and are released at

    specified rate

    Threedimensional winds move the par1clesCan then watch the transport of the emissions

  • 8/9/2019 Meteorology for Airborne Scientists

    47/59

    Fire loca1ons July 2008

  • 8/9/2019 Meteorology for Airborne Scientists

    48/59

  • 8/9/2019 Meteorology for Airborne Scientists

    49/59

    Sources of Real Time Informa1on

    Surface

    RadiosondesSatellite

    Radar

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

  • 8/9/2019 Meteorology for Airborne Scientists

    50/59

    Surface Plot

  • 8/9/2019 Meteorology for Airborne Scientists

    51/59

  • 8/9/2019 Meteorology for Airborne Scientists

    52/59

    GOESYesterday PM

  • 8/9/2019 Meteorology for Airborne Scientists

    53/59

    Edwards AFB Sounding

  • 8/9/2019 Meteorology for Airborne Scientists

    54/59

  • 8/9/2019 Meteorology for Airborne Scientists

    55/59

    Forecast Products

    All types of input data combined (assimilated) toproduce best 3D ini1al condi1ons for model

    Models iterate forward in 1me

    Various groups run models NWS, USAF, Navy,Europeans, etc.

    Model forecast surface and alo at each itera1on Different models give different solu1ons Meteorologist decides on the most likely forecast

  • 8/9/2019 Meteorology for Airborne Scientists

    56/59

    Your Local NWS Office

    hp://www.srh.noaa.gov

  • 8/9/2019 Meteorology for Airborne Scientists

    57/59

    Other Interes1ng Sites

    Storm Predic1on Center

    hp://www.spc.noaa.gov

    Na1onal Hurricane Center

    hp://www.nhc.noaa.gov

  • 8/9/2019 Meteorology for Airborne Scientists

    58/59

    NWS Forecast for Palmdale

    Friday Night: Clear, with a low around 6.Breezy, with a southwest wind 20 to 25 mph

    decreasing to between 0 and 5 mph. Winds

    could gust as high as 30 mph.

    Saturday: Sunny, with a high near 94.

    Southwest wind around 0 mph.

    Saturday Night: Clear, with a low around 63.

    Southwest wind between 0 and 5 mph, withgusts as high as 25 mph.

    Sunday: Sunny and hot, with a high near 98.

    Sunday Night: Clear, with a low around 63.

    Monday: Sunny, with a high near 95

    Monday Night: Clear, with a low around 60.

    Tuesday: Sunny, with a high near 94.Tuesday Night: Clear, with a low around 59.

    Wednesday: Sunny, with a high near 94.

    Wednesday Night: Clear, with a low around 59.

    Thursday: Sunny, with a high near 94.

  • 8/9/2019 Meteorology for Airborne Scientists

    59/59

    Santa Barbara Channel