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Meteorology - Chapter 1:

 Met Theory


Topics:

1. The Atmosphere
2. Clouds
3. Pressure
4. Wind
5. Humidity
6. Temperature
7. Stability
Chapter 1 – 1: The Atmosphere

Atmospheric Composition


   The Earth’s ATMOSPHERE is made up of:

           -78% nitrogen
           -21% oxygen
           -1% rare gases (argon, carbon dioxide,
             water vapour)
Chapter 1 – 1: The Atmosphere

Water Vapour


       Of all of the ingredients that make up the
       atmosphere, the most important
       component for pilots is WATER VAPOUR.

       It is the water vapour that is responsible
       for the formation of clouds, fog, and
       precipitation. In other words, it is the
       water vapour that produces weather.
Chapter 1 – 1: The Atmosphere

Properties of the Atmosphere


       A parcel of atmospheric air processes 3
       properties, namely mobility, capacity for
       expansion, and capacity for compression:

       MOBILITY – like a body of water over a river
       bed, a body of air can move over the Earth’s
       surface.
Chapter 1 – 1: The Atmosphere

Properties of the Atmosphere


       CAPACITY FOR EXPANSION – like a
       balloon, a parcel of air can expand. When
       it does, the parcel of air cools.
Chapter 1 – 1: The Atmosphere

Properties of the Atmosphere


       CAPACITY FOR COMPRESSION – like a
       deflating balloon, a parcel of air can
       compress. When it does, the temperature
       rises.
Chapter 1 – 1: The Atmosphere

Divisions of the Atmosphere

  The layer of atmosphere closest to the Earth is
  called the TROPOSPHERE.

  The Troposphere extends to a height of 28,000 feet
  at the Poles, and 54,000 feet at the Equator.

  In the Troposphere, air pressure, density, and
  temperature all decrease with increasing altitude.
  In other words, with increasing altitude, the air
  becomes lighter, thinner, and colder.

  Because almost all water vapour is found in the
  Troposphere, all active weather occurs in this layer.
Chapter 1 – 1: The Atmosphere

Divisions of the Atmosphere


         Above the Troposphere is a layer called
         the STRATOSPHERE. In the
         Stratosphere, the temperature ceases
         to drop, and remains at -56oC.
Chapter 1 – 1: The Atmosphere

Divisions of the Atmosphere


          The boundary layer separating the
          Troposphere from the Stratosphere is
          called the TROPOPAUSE.
Chapter 1 – 1: The Atmosphere

Divisions of the Atmosphere


 In an earlier chapter on Flight Instruments, we
 talked about “ICAO Standard Atmosphere”. (Recall
 that ICAO stands for “International Civil Aviation
 Organization”).
 This “standard” atmosphere is based on averages
 of atmospheric conditions at 49o of Latitude. By
 definition, ISA (ICAO Standard Atmosphere) is:

         -Pressure = 29.92” Hg (inches of Mercury)
         -Temperature = 15oC at sea level
         -Temperature Decrease (or Lapse Rate) =
           2oC per 1,000 feet above sea level
Chapter 1 – 2: Clouds

High Clouds


        Clouds can be classified according to their
        altitude.

        HIGH clouds have bases starting from
        16,500 feet to 45,000 feet.

        The name of these clouds are prefixed with
        “Cirro”.
Chapter 1 – 2: Clouds

Mid Level Clouds


         MID LEVEL clouds have bases starting
         from 6,500 feet to 23,000 feet.

         The name of mid level clouds are
         prefixed with “Alto”.
Chapter 1 – 2: Clouds

Low Level Clouds


      LOW LEVEL clouds have bases starting at the
      Earth’s surface, or up to 6,500 feet.

      The name of low level clouds have no prefix
      attached to them.
Chapter 1 – 2: Clouds

Cumulus Clouds


       Types of clouds can be further classified
       according to their characteristics.

       Clouds of vertical development (i.e. puffy or
       cotton ball type clouds) are called CUMULUS
       clouds.
Chapter 1 – 2: Clouds

Stratus Clouds


      Clouds that form in horizontal layers or sheet
      are called STRATUS clouds.
Chapter 1 – 2: Clouds

Fractus Clouds


       Clouds that are windblown or broken are
       referred to as FRACTUS clouds.
Chapter 1 – 2: Clouds

Nimbus Clouds


      And finally, clouds from which precipitation
      falls are called NIMBUS clouds.
Chapter 1 – 2: Clouds

Cloud Names


      Now, if we combine any of the above
      classifications of clouds with a cloud’s
      characteristics, we can determine the full
      name of a cloud.

      For example, a high level cloud that is cotton-
      like is called CIRROCUMULUS cloud.

              Cirro = high
              Cumulus = cotton-like
Chapter 1 – 2: Clouds

Cloud Names


     A high level cloud that is made up of sheets
     or layers of clouds is called CIRROSTRATUS
     cloud.

             Cirro = high
             Stratus = horizontal layers
Chapter 1 – 2: Clouds

Cloud Names



     A mid-level cloud that is rounded and puffy is
     called ALTOCUMULUS cloud.

             Alto = middle level
             Cumulus = puffy
Chapter 1 – 2: Clouds

Cloud Names


     A mid-level grey cloud that covers the whole
     sky is called ALTOSTRATUS cloud.

             Alto = middle level
             Stratus = horizontal formation
Chapter 1 – 2: Clouds

Cloud Names



     Low level cloud that resembles a series of
     patches or rounded masses is called
     CUMULUS cloud.

             no prefix = low level
             Cumulus = rounded masses
Chapter 1 – 2: Clouds

Cloud Names


      A uniform layer of low level cloud is called
      STRATUS cloud.

              no prefix = low level
              Stratus = layer cloud
Chapter 1 – 2: Clouds

Cloud Names



      Low level layer cloud that is windbroken is
      called STRATUSFRACTUS cloud.

              Stratus = layer cloud (horizontal
                           formation)

              Fractus = windblown
Chapter 1 – 2: Clouds

Cloud Names



     Heavy masses of vertically developed cloud
     from which precipitation is falling is called
     CUMULONIMBUS cloud.

             Cumulo (from Cumulus) = mass cloud
              (vertical development)

             Nimbus = precipitation
Chapter 1 – 2: Clouds

Cloud Names


    Review your Environment Canada Clouds Poster
    included with your Groundschool kit for further
    cloud names and descriptions.
Chapter 1 – 2: Clouds

Sky Condition


  The SKY CONDITION refers to the amount of sky
  that is covered by cloud, as observed from the
  surface up.

  The sky condition can be any one of the following:

    -SKC = ‘sky clear’ = no cloud
    -FEW = ‘few’ = >0/8 to 2/8 cloud coverage
    -SCT = ‘scattered’ = 3/8 to 4/8 cloud coverage
    -BKN = ‘broken’ = 5/8 to <8/8 cloud coverage
    -OVC = ‘overcast’ = 8/8 cloud coverage
Chapter 1 – 3: Pressure

Atmospheric Pressure


ATMOSPHERIC PRESSURE is the weight of the air
above us.

The greater the amount of air above us, or the
greater the density of the air above us, the greater
the downward pressure the air will apply on us.

Atmospheric pressure changes from location to
location. If there is dense, heavy air over an
area, the pressure will be higher than under an area
of less dense air.
Chapter 1 – 3: Pressure

Atmospheric Pressure


The pressure (whether it be “high” pressure or
“low” pressure) is important to pilots because it:

         -affects our altimeters (as discussed in the
           chapter on Flight Instruments)

         -controls the wind (as we will learn in this
           chapter)
Chapter 1 – 3: Pressure

Mercury Barometer


    For aviation purposes, pressure is measured
    with a Mercury Barometer.

    A simplified Mercury Barometer would be a
    dish filled with liquid mercury and an
    inverted test-tube held in the dish of
    mercury.
Chapter 1 – 3: Pressure

Mercury Barometer


        As the weight of the atmosphere
        increases (i.e. an increase in atmospheric
        pressure), it will push down on the
        surface of the mercury, thereby forcing it
        to rise up in the tube.
Chapter 1 – 3: Pressure

Mercury Barometer


        If we now measure how many inches the
        mercury rises in the tube, (e.g. 29.92
        inches), then we can determine the
        altimeter setting. In this case, we would
        call the altimeter setting 29.92” Hg.
Chapter 1 – 3: Pressure

                      Mercury Barometer


In aviation, we use inches of mercury (”Hg) to express atmospheric
pressure.

Other units used to measure pressure are millibars and kilopascals.
Chapter 1 – 3: Pressure

Isobars

    ISOBARS are lines drawn on a Weather Map
    that join places of equal atmospheric
    pressure.

    Isobars never cross one another, but tend to
    form circular patterns.

    Although we commonly use inches of mercury
    to express pressure in aviation, the Isobars on
    Weather Maps are presented in millibars.
Chapter 1 – 3: Pressure

Low Pressure Area


        If we examine the pattern that the
        Isobars form on this Weather Map, we
        notice that as we move from the center
        of the map to the upper right corner, the
        pressure continually drops.

        We therefore conclude that there is a
        “low” pressure area in the top right
        corner.
Chapter 1 – 3: Pressure

High Pressure Area


        Likewise, if we look at the pattern as we
        move from the center of the map to the
        bottom right corner, we notice that the
        pressure continually rises.

        This would indicate that there is a “high”
        pressure area in the bottom right corner.
Chapter 1 – 3: Pressure

High Pressure, Low Pressure


        Likewise, the pattern of Isobars would
        indicate a “high” pressure area in the
        upper left corner, and a “low” pressure
        area in the lower left corner of this
        Weather Map.
Chapter 1 – 3: Pressure

Trough


         A TROUGH is an elongated u-shaped area
         of low pressure.

         A trough is like a “valley” of low pressure.
Chapter 1 – 3: Pressure

Ridge


            A RIDGE is a protruding neck of high
            pressure.

            A ridge is like a “mountain range” of
            high pressure.
Chapter 1 – 3: Pressure

Col


             A COL is a “neutral” area between two
             high pressure areas and two low
             pressure areas.
Chapter 1 – 3: Pressure

Pressure Gradient


          PRESSURE GRADIENT is the rate of
          change of pressure over a given distance.

          The pressure gradient can be a shallow
          gradient (i.e. a small rate of change), or a
          steep gradient (i.e. a large rate of
          change).
Chapter 1 – 3: Pressure

Pressure Gradient


       The pressure gradient (or the nearness of
       the Isobars) is an indication of the
       strength of the wind.

       Where there is a shallow gradient (i.e.
       where the Isobars are far apart), there
       will be light winds.

       Where there is a steep gradient (i.e.
       where the Isobars are close together), the
       wind will be strong.
Chapter 1 – 3: Pressure

Wind


          WIND is simply air trying to move (as it
          wants to) from an area of high pressure
          to an area of lower pressure.

          Just like an inflated balloon, the air
          inside the balloon is under high
          pressure. The air outside the balloon is
          at a much lower pressure. The air wants
          to escape from the balloon. In other
          words, the air wants to move from the
          high pressure area to the low pressure
          area.
Chapter 1 – 3: Pressure

Wind


          So, if we had the above Weather
          Map, the air would want to move
          from the high pressure area to the
          low pressure area. The wind would
          tend to blow from the high to the
          low.

          However, as we are about to see, it
          gets a little more complicated than
          this…
Chapter 1 – 3: Pressure

Wind


      Because the Earth is not stationary, but is
      rotating beneath the atmosphere, the wind
      does not move in a straight line (relative to
      the Earth’s surface) as it attempts to move
      from a high pressure area to a low pressure
      area. It becomes influenced by a force
      called CORIOLIS FORCE.

      In the Northern Hemisphere, Coriolis Force
      causes the air movement to be deflected to
      the right (in relation to the Earth’s
      surface), causing it to flow parallel to the
      Isobars.
Chapter 1 – 3: Pressure

Wind


          If we had a high pressure area on either
          side of a low pressure area, we know
          that the wind would want to blow into
          the low (from high to low).
Chapter 1 – 3: Pressure

Wind


          However, Coriolis Force says that in its
          movement, the wind gets deflected to the
          right.
Chapter 1 – 3: Pressure

Wind


           This pattern shows how the wind
           tends to blow clockwise around a
           HIGH.
Chapter 1 – 3: Pressure

Wind


            It also shows how the wind tends to
            blow counter-clockwise around a
            LOW.
Chapter 1 – 3: Pressure

Wind

      Remember this picture to help you recall
      whether the wind blows clockwise or
      counter-clockwise around a high or low…

      It is a picture of a “high clock over top of a
      low counter”.

               high = clockwise
               low = counter-clockwise

      The wind blows clockwise around a high, and
      counter-clockwise around a low.
Chapter 1 – 3: Pressure

Wind


            Here’s another trick…

            When outdoors, you can always tell
            where the low pressure area is if you
            stand with your back to the wind…
Chapter 1 – 3: Pressure

Wind


        In this position, the low will be to your left.
Chapter 1 – 3: Pressure

Wind

      There is one more element that affects
      the precise direction of the wind.

      In fact, the wind does not blow exactly
      parallel to the Isobars. SURFACE
      FRICTION between the moving air and
      the Earth’s surface tends to slow down
      its motion and retards the effect of the
      Coriolis Force.

      Therefore, the air tends to move across
      the isobars at an angle inward toward a
      low, and outward from a high.
Chapter 1 – 4: Wind

    Wind


As you can imagine, the wind is a very important factor for
pilots. The wind can have a negative or positive effect for us:
 - on takeoff - wind affects takeoff distance
               - wind affects takeoff safety (gusts, crosswind)
 - in cruise - wind affects groundspeed (time, fuel, money)
 - on landing - wind affects landing distance
               - wind affects landing safety (gusts, crosswind)

We will now look at different types of wind…
Chapter 1 – 4: Wind

Sea Breeze


        A SEA BREEZE is a wind that blows from
        the sea (or a large body of water) to the
        land.

        Note: When referring to wind direction, we
        always refer to the direction from which it
        is blowing (e.g. a north wind blows from
        the north).
Chapter 1 – 4: Wind

Sea Breeze

        A Sea Breeze blows during the day.

        The Earth’s surface is a better conductor of
        heat than water. During the day, the sun
        heats the Earth (more-so than the water),
        which in turn heats the air above it. This
        warmed air (over the land) rises.

        Note: Warm air, which is less dense, tends
        to rise. Cool are, which is more dense,
        tends to sink.
Chapter 1 – 4: Wind

Sea Breeze


         This rising air (over the land) creates a
         low pressure area over the land.
         (Because the air is rising, there is less
         downward pressure created by the
         atmosphere, resulting in a lower
         pressure).

         In contrast, the air over the water (sea)
         will be of a higher pressure.
Chapter 1 – 4: Wind

Sea Breeze


        We know that the air tends to move from
        a high pressure area to a low pressure
        area. So, during the day, the wind will
        blow from the sea to the land, creating a
        Sea Breeze.
Chapter 1 – 4: Wind

Land Breeze


          A LAND BREEZE is a wind that blows
          from the land to the sea (or a large body
          of water).
Chapter 1 – 4: Wind

Land Breeze

        A Land Breeze works opposite to a Sea
        Breeze, and blows at night.

        At night, all the sun’s warmth radiates
        from the Earth’s surface into the upper
        atmosphere, and the air over the land
        becomes cool. Water retains heat
        better, so the air over the water remains
        warmer.

        The warmer air over the water will
        rise, creating a low pressure area over the
        water. In contrast, the air over the land will
        be of a higher pressure.
Chapter 1 – 4: Wind

Land Breeze


        With the high pressure over the land at
        night, the wind will blow from the land to
        the sea, creating a Land Breeze.
Chapter 1 – 4: Wind

Mountain Wind

         Wind in the vicinity of mountains can be
         extremely challenging for a pilot. In fact, it
         is recommended that you seek the advise
         (or perhaps even training) of a pilot with
         mountain flying experience before flying
         in the mountains.

         When the wind blows through a mountain
         valley, the valley creates a “funnel
         effect”, whereby the wind velocity
         increases substantially. This strong wind
         can also lead to pronounced turbulence.
         We’ll now look at some specific types of
         mountain winds…
Chapter 1 – 4: Wind

Mountain Wind

       An ANABATIC WIND blows up a mountain
       slope during the day.

       As the sun heats the dark surface of the
       mountain slope, the warmed surface radiates
       its heat to warm the air above it. This warm
       air rises, creating a wind that blows up the
       mountain slope.
Chapter 1 – 4: Wind

Mountain Wind

         A KATABATIC WIND blows down a
         mountain slope.

         If the mountain tops are snow covered,
         the air at the caps will be cooled. This cold
         dense air will sink, causing the wind to
         blow down the slope.

         An Anabatic Wind can turn into a
         Katabatic Wind at night. The removal of
         the sun’s heat causes the mountain slope
         to cool, thereby cooling the air above it.
         Again, this cool dense air will flow down
         the mountain slope.
Chapter 1 – 4: Wind

Mountain Wind

  A MOUNTAIN WAVE forms when the wind blows over
  the top of a mountain peak.
  Just like the airflow over the top of a wing, the wind
  blowing over a mountain top will have:

          -increased speed
          -decreased pressure
          -decreased temperature

  In the chapter on Flight Instruments, we learned how
  this effect can cause the Altimeter to read in error by
  as much as 3,000 feet!
  The decreased temperature can lead to airframe icing
  (ice accumulation on the airplane).
Chapter 1 – 4: Wind

Mountain Wind


         Turbulence associated with a
         mountain wave is most frequent and
         most severe just beneath the wave
         crest at or below mountaintop level.
Chapter 1 – 4: Wind

Mountain Wind


         On the leeward side of the mountain
         there can be strong downdrafts (as
         much as 2000 to 5000 feet per
         minute) and very turbulent eddies.
Chapter 1 – 4: Wind

Wind Gust


         A wind GUST is a rapid change of wind
         speed or direction, that is of brief
         duration (seconds).

         Gusts are usually caused by obstacles
         being in the way of the wind’s path (e.g.
         hangars, buildings, irregular terrain, etc.)
Chapter 1 – 4: Wind

Wind Squall


         A wind SQUALL is a rapid change of
         wind speed or direction, that is of
         prolonged duration.

         A squall is usually caused by the passage
         of a fast moving cold front.
Chapter 1 – 4: Wind

Eddies/Mechanical Turbulence

         EDDIES, also known as MECHANICAL
         TURBULENCE, is disturbed airflow
         (similar to eddies of water in a river
         or stream). They are caused by
         irregular surfaces in the wind’s path
         (like rocks in a shallow river) such as
         hills, buildings, etc.

         Mechanical Turbulence only occurs in
         the lower levels of the atmosphere
         (usually below 3,000 feet), and
         depends on the strength of the wind
         being disturbed.
Chapter 1 – 4: Wind

Wind Shear

          A wind SHEAR is a sudden or violent
          change in wind speed or direction.

          Wind shears are most commonly
          associated with thunderstorms.
          They can be extremely dangerous
          because the wind can change much
          faster than an airplane’s ability to
          accelerate or decelerate. They are
          especially dangerous near the
          ground during takeoff and landing.
Chapter 1 – 4: Wind

Jet Stream

         A JET STREAM is a tube-like band of high
         speed wind at high altitudes (20,000 to
         40,000 feet). This band can be from 3,000
         to 7,000 feet thick, with a core wind of
         100 to 150 knots. This wind flows from
         west to east.

         There are two Jet Streams across North
         America: one lies approximately across
         Canada and the other across the USA. The
         Jet Streams migrate south in the summer,
         and move back north in the winter.
Chapter 1 – 4: Wind

Clear Air Turbulence


           CLEAR AIR TURBULENCE (CAT) is a
           very turbulent condition that occurs
           in a cloudless sky, usually associated
           with a Jet Stream or Mountain Wave.
           Because it occurs in a clear sky, CAT is
           almost impossible to forecast.
Chapter 1 – 4: Wind

Wind Speed and Direction


            In aviation, wind speed is
            expressed in knots (nautical miles
            per hour).

            Wind direction is the direction
            from which it is blowing. Using the
            compass rose to express precise
            direction, a wind blowing from the
            south would be a wind of 180o.
Chapter 1 – 4: Wind

Wind Speed and Direction


           A wind of 040o would be blowing from
           the north-east (NE).
Chapter 1 – 4: Wind

Wind Speed and Direction


         A VEER is a clockwise change in wind
         direction.

         For example, if the wind changed from
         270o to 300o, we would say that the
         wind veered.
Chapter 1 – 4: Wind

Wind Speed and Direction


            A BACK is a counter-clockwise
            change in wind direction.

            For example, if the wind changed
            from 270o to 240o, we would say
            that the wind backed.
Chapter 1 – 4: Wind

Diurnal (Daily) Wind Variations


          We all know that the wind tends to
          increase during a hot afternoon, and
          then calms at night. This is due to
          Diurnal Variation…
Chapter 1 – 4: Wind

Diurnal (Daily) Wind Variations


           During the hot afternoon, the sun
           heats the Earth’s surface. The Earth
           then heats the air above it by
           radiation. This warming air rises. As it
           rises, it expands, cools, and begins to
           fall again.

           As it falls, it transfers the higher level
           wind (from about 3,000 feet) to the
           surface. The higher level wind in
           unaffected by surface friction and is
           therefore stronger, and flows more
           parallel to the Isobars.
Chapter 1 – 4: Wind

Diurnal (Daily) Wind Variations


          As a result, during the daytime, the
          wind veers and increases in strength.

          At night, the wind resumes its normal
          direction and speed: it backs and
          decreases.
Chapter 1 – 5: Humidity

Humidity


            HUMIDITY is the amount of moisture in
            the air.

            This moisture can be one of 2 forms:

               - invisible form (which is water
                       vapour)

               - visible form (which is water
                       droplets or ice crystals,
                       making up clouds or fog)
Chapter 1 – 5: Humidity

Condensation


            CONDENSATION is when water
            vapour changes into water droplets. In
            other words, the moisture changes
            from a gas to a liquid, or from its
            invisible form to its visible form.

            Condensation can be seen as moisture
            on the inside of a window on a cold
            winter day.
Chapter 1 – 5: Humidity

Sublimation


           SUBLIMATION is when water vapour
           changes into ice crystals. In other
           words, the moisture changes from a
           gas to a solid. Again, it changes from
           its invisible form to its visible form,
           but in this case, the liquid stage is
           bypassed.

           Sublimation can be seen as frost on a
           car window on a cold winter morning.
Chapter 1 – 5: Humidity

Sublimation


      Here is an important point to remember
      about humidity:

                Warm air can hold more moisture
                than cold air

      A parcel of warm air has the ability to hold
      more water molecules than a similar parcel of
      cold air.
Chapter 1 – 5: Humidity

Saturated Air


      SATURATED AIR is when a parcel of air
      contains the maximum amount of water
      vapour that it can hold at a given
      temperature.
Chapter 1 – 5: Humidity

Saturated Air

    If the air is saturated (i.e. it contains all the
    moisture it can hold), and then the temperature
    drops, that parcel of air will have more moisture
    than it can hold. (Remember: warm air can hold
    more moisture than cold air).

    This excess moisture (or vapour) will be forced into
    condensation or sublimation. The excess moisture
    will change from its invisible form to its visible
    form, creating either cloud, fog, dew, or frost.

    You’ve noticed that fog, dew and frost tend to
    form at night, when the temperature drops. Clouds
    form in the higher altitudes. Remember… the
    temperature decreases with increasing altitude.
Chapter 1 – 5: Humidity

Saturated Air

       So, saturated air can be forced into
       condensation or sublimation be decreasing
       the temperature.

       Another way for this to happen is to increase
       the moisture content of the air. If the air is
       already saturated, then adding more
       moisture will also force the excess vapour
       into condensation or sublimation.

       An example of this is when you see your
       breath on a cold day (since the air you
       breathe out has a lot of moisture in it from
       your lings)
Chapter 1 – 5: Humidity

Super-Cooled Water Droplets

         SUPER-COOLED WATER DROPLETS are
         liquid water droplets that exist in the
         liquid form at temperatures well below
         0oC. This is a condition that does not
         normally happen, and requires specific
         atmospheric conditions to exist. They are
         sometimes associated with thunderstorms
         cells. They can exist at temperatures as
         low as -40oC.
         Super-cooled water droplets are a hazard
         because, when they are disturbed (e.g. by
         a wing), they turn into ice instantaneously.
         They create a rapid accumulation of
         airframe icing.
Chapter 1 – 5: Humidity

Dewpoint

         The DEWPOINT is the temperature to
         which unsaturated air must be cooled to
         become saturated.

         The dewpoint is the temperature at
         which invisible moisture changes into
         visible moisture. It is the temperature at
         which fog, dew, frost, or clouds form.
Chapter 1 – 5: Humidity

Relative Humidity

         RELATIVE HUMIDITY is the ratio of the
         amount of water vapour present in the
         air to the amount it would hold if it
         were saturated (at the same pressure
         and temperature).

         For example, if the air is holding 80% of
         the moisture that it can hold, then we
         say that the Relative Humidity is 80%.

         Saturated air has a Relative Humidity of
         100%.
Chapter 1 – 5: Humidity

Relative Humidity


          If a parcel of air is heated, then its Relative
          Humidity decreases. (Remember: warm air
          can hold more moisture than cold air).

          If a parcel of air is cooled, then its Relative
          Humidity increases.
Chapter 1 – 5: Humidity

Relative Humidity


       The smaller the spread between the
       temperature and the dewpoint, the higher
       the Relative Humidity.
Chapter 1 – 6: Temperature

Temperature


         As we’ve already stated, the sun heats
         the Earth, and the Earth heats the
         atmosphere above it by radiation.

         This is an important point to remember.
         The atmosphere is heated from
         below, not from above.
Chapter 1 – 6: Temperature

Seasonal Variation

      So, why is the atmosphere’s temperature
      different at different places?

      One reason is due to SEASONAL VARIATION.
      The Earth’s axis of rotation is not
      perpendicular to the Earth’s path of
      travel, but is at a “tilt”. Hence, during North
      America’s summer months, the sun’s rays are
      more perpendicular to the continent’s
      surface (shine from overhead).
      But in the winter, the sun is lower on the
      horizon, so the sun’s rays are at more of an
      angle to the continent’s surface.
Chapter 1 – 6: Temperature

Seasonal Variation

        Like a beam of light shining directly onto
        a surface, the light’s rays are
        concentrated in a small area. But if we
        shine the light at an angle to the surface,
        then that same beam covers a larger
        surface area.

        If both beams are producing the same
        amount of energy (heat), then the beam
        of light shining from directly above will
        concentrate its heat over a smaller are.
        Therefore, this surface will be warmer.
        The sun has the same effect on the
        Earth’s surface in summer vs. winter.
Chapter 1 – 6: Temperature

Latitudinal Variation


     This same principle explains LATITUDINAL
     VARIATION of the Earth’s temperature.

     Locations near the Equator have the sun
     more directly overhead than locations
     further north or south of the Equator. Hence,
     near the Equator the temperatures are
     warmer.
Chapter 1 – 6: Temperature

Topography

       TOPOGRAPHY (the makeup of the Earth’s
       surface) also has an effect on temperature.
       Since dark colours absorb more light than
       light colours do (this is Physics!), dark colours
       get warmer when the sun shines on them.

       The same holds true for the Earth’s surface.
       Dark coloured terrain (dark soil, asphalt, etc.)
       gets hotter than does light coloured terrain
       (water, snow, etc.).

       Therefore, the atmosphere above a dark
       surface will be warmer.
Chapter 1 – 6: Temperature

Cloud Cover

      CLOUD COVER can have an effect on
      temperature. During the day, the absence of
      cloud cover allows for maximum heat from
      the sun to heat the Earth’s surface, creating
      warmer air (by radiation).

      However, at night, a clear sky allows all the
      Earth’s heat (gained during the daytime) to
      radiate into the upper atmosphere, creating
      cool temperatures at the surface.

      A cloudy night produces a sort of blanket,
      keeping the heat near the surface, creating a
      warmer night.
Chapter 1 – 6: Temperature

How the Atmosphere is Heated


       The atmosphere can be heated by any one
       of 4 methods:

               -Convection
               -Advection
               -Turbulence
               -Compression

       We will look at each of these…
Chapter 1 – 6: Temperature

How the Atmosphere is
Heated/Convection

   CONVECTION works much like bubbles that form
   in a pot of boiling water.
   The air nearest the Earth’s surface is warmed.
   Because warm air is less dense than cold air, it
   begins to rise. As it rises, it cools, by expansion.
   (Remember… at higher altitudes the pressure
   decreases, allowing the air to expand. When it
   expands, it cools).
   As the air cools, it becomes more dense
   (heavier), and begins to fall again, replacing the
   rising warm air below.

   It is the rising air that warms the air aloft.
Chapter 1 – 6: Temperature

How the Atmosphere is
Heated/Advection



          ADVECTION refers to the horizontal
          movement of air from one place to
          another. Advection heating occurs when
          cool air moves over a warm surface.

          The warm surface warms the air above
          it.
Chapter 1 – 6: Temperature

How the Atmosphere is
Heated/Turbulence



         When an obstruction in the path of
         the air’s movement (such as a hill or
         irregular terrain) disturbs
         it, TURBULENCE is created.

         This turbulence can push the warm
         air aloft.
Chapter 1 – 6: Temperature

How the Atmosphere is
Heated/Compression


        When a parcel of air is COMPRESSED, it
        warms.

        This can occur on the leeward side of a
        mountain range. As the air flows down
        the mountain, it is compressed at the
        mountain’s base. The compressed air
        becomes warmer.
Chapter 1 – 6: Temperature

How the Atmosphere is Cooled


      The atmosphere can be cooled by any one
      of 3 methods:

              -Radiation
              -Advection
              -Expansion

      We will look at each of these…
Chapter 1 – 6: Temperature

How the Atmosphere is
Cooled/Radiation


       At night, solar RADIATION ceases. All the
       heat absorbed by the Earth’s surface from
       the previous day radiates, or
       transfers, into the upper atmosphere. As
       a result, the lower levels of the
       atmosphere cool.
Chapter 1 – 6: Temperature

How the Atmosphere is
Cooled/Advection



      Remember, ADVECTION refers to the
      horizontal movement of air from one place
      to another. Advection cooling occurs when
      warm air moves over a cool surface.

      The cool surface cools the air above it.
Chapter 1 – 6: Temperature

How the Atmosphere is
Cooled/Expansion


          When a parcel of air EXPANDS, it cools.
          (This is the opposite of compression).

          If you’ve ever used a can of spray paint,
          then you’ve experienced this. The paint
          inside the can is under compression. As it
          comes out of the nozzle, it expands, and
          cools. You may have noticed that the tip of
          your finger on the nozzle gets cold!
Chapter 1 – 6: Temperature

How the Atmosphere is
Cooled/Expansion


         The same thing happens when air is
         forced to rise… the pressure
         decreases, so the air expands. When it
         expands, the temperature decreases.
Chapter 1 – 6: Temperature

Isotherms


           ISOTHERMS are lines drawn on a
           Weather Map that join places of equal
           temperature.
Chapter 1 – 6: Temperature

Temperature Scales

  The international aeronautical unit used to express
  temperature is Degrees Celsius.

  In Degrees Celsius:
            - the freezing point of water = 0oC
            - the boiling point of water = 100oC

  However, you may come across some airplane
  manuals (especially for airplanes built in the USA) that
  express temperature in Degrees Fahrenheit.

  In Degrees Fahrenheit:
            - the freezing point of water = 32oF
            - the boiling point of water = 212oF
Chapter 1 – 6: Temperature

Temperature Scales


          To convert from oC to oF:

                  oF = 9/5 oC + 32
                  oC = 5/9 (oF – 32)



          Or, simply use your E6B Flight Computer!
Chapter 1 – 6: Temperature

Density vs. Temperature


         Cold air is more dense than warm air.
         Therefore, it is heavier and tends to
         sink.

         Warm air is less dense, or lighter, and
         tends to rise.
Chapter 1 – 6: Temperature

Lapse Rate

          LAPSE RATE is the rate of decrease in
          temperature with height.

          There are 3 different Lapse Rates:

            - ICAO Standard Lapse Rate
            - Dry Adiabatic Lapse Rate
            - Saturated Adiabatic Lapse Rate

          We will look at each of these…
Chapter 1 – 6: Temperature

ICAO Standard Lapse Rate

        The ICAO STANDARD LAPSE RATE is an
        average lapse rate, as derived by ICAO.
        (Remember, ICAO = International Civil
        Aviation Organization).

        This standard lapse rate is 1.98oC/1000
        feet

        For simplicity, we commonly say that it
        is 2oC/1000 feet.

        This ICAO Standard Lapse Rate is an
        assumption used for the calibration of
        aircraft Altimeters.
Chapter 1 – 6: Temperature

Dry Adiabatic Lapse Rate


            The DRY ADIABATIC LAPSE RATE is
            the actual lapse rate in air that is
            not saturated. This is the lapse rate
            when the temperature is greater
            that the dewpoint.

            By definition, this lapse rate is
            3oC/1000 feet.
Chapter 1 – 6: Temperature

Standard Adiabatic Lapse Rate

  The SATURATED ADIABATIC LAPSE RATE (or
  sometimes called the WET ADIABATIC LAPSE RATE) is
  the lapse rate in air that is saturated. This is the lapse
  rate when the temperature meets the dewpoint.

  (Remember that at the dewpoint, moisture changes
  into its visible form. Clouds form at the dewpoint. The
  base of clouds, then, represents the altitude at which
  the temperature meets the dewpoint).

  By definition, the Saturated Adiabatic Lapse Rate is
  1.5oC/1000 feet.

  So, at or above the base of clouds, the lapse rate
  becomes 1.5oC/1000 feet.
Chapter 1 – 6: Temperature

Standard Adiabatic Lapse Rate

 Here is a sample problem:

 Question: If the surface temperature is 10oC and the
 dewpoint is 1oC, what is the altitude of the base of the
 clouds?

 Solution: We know that below the cloud base, the air is
 unsaturated, so the lapse rate is 3oC/1000 feet (we use the
 Dry Adiabatic Lapse Rate below the cloud base).

 So, at: -1000 feet above ground, the temperature = 7oC
         -2000 feet above ground, the temperature = 4oC
         -3000 feet above ground, the temperature = 1oC
 Therefore, at 3000 feet we’ve reached the dewpoint of
 1oC, and cloud will begin to form.
Chapter 1 – 6: Temperature

Inversion


       An INVERSION is when the temperature
       increases with height.

       Inversions are not the norm. They are
       usually associated with a frontal surface.
       (We will talk more about fronts soon).
Chapter 1 – 6: Temperature

Isothermal Layer


          An ISOTHERMAL LAYER is when the
          temperature remains constant (neither
          decreases nor increases) throughout a
          layer for some depth.
Chapter 1 – 7: Stability

Stability


                STABLE air is air that resists upward
                of downward displacement.

                UNSTABLE air is air that tends to
                move further away when displaced.
Chapter 1 – 7: Stability

Unstable Air


             If a parcel of air is warmer than the
             surrounding air, it will tend to rise.

             (Remember: warm air is less
             dense, or lighter, then cool air)

             This parcel of air is therefore
             unstable.
Chapter 1 – 7: Stability

Stable Air


                Air that is cooler than the
                surrounding air will resist upward
                motion.

                (Remember: cool air is more
                dense and therefore will not want
                to rise)

                This parcel of air is therefore
                stable.
Chapter 1 – 7: Stability

Lapse Rate vs. Stability


                The steeper the lapse rate, the
                more unstable the air.
Chapter 1 – 7: Stability

Flight Characteristics in Stable Air


   Flight through STABLE air will provide the following
   flight characteristics:
   - poor low level visibility (because stable air tends
              not to rise, so the pollutants get trapped
              near the surface)
   - stratus type cloud (layer cloud)
   - steady precipitation (e.g. that “all day” type of
              rain, which is characteristic of stratus type
              cloud)
   - steady (constant) winds
   - smooth flying conditions
Chapter 1 – 7: Stability

Flight Characteristics in Unstable Air


Flight through UNSTABLE air will provide the following
flight characteristics:

     - good visibility (except in precipitation)
     - cumulus type cloud (heap type cloud of vertical
           development, built from unstable, rising air)
     - showery precipitation (e.g. “bursts” of rain,
           which are characteristic of cumulus type
           cloud)
     - gusty winds
     - turbulent flying conditions (produced by rising
           columns of unstable air)
     - smooth flying conditions
Chapter 1 – 7: Stability

Lifting Agents


    LIFTING AGENTS are the forces or conditions
    that provide the lift to initiate rising currents of
    air.

    If a lifting agent provides a force onto a parcel
    of unstable air, then this air will experience
    significant lift. Stable air will have substantially
    less lift.

    When air is lifted to a higher altitude, it expands
    and cools. If it expands and cools
    sufficiently, then cloud formation occurs, and
    hence weather is produced.
Chapter 1 – 7: Stability

Lifting Agents


      There are 5 different Lifting Agents:

               -Convection
               -Orographic Lift
               -Frontal Lift
               -Mechanical Lift
               -Convergence

      We will look at each of these…
Chapter 1 – 7: Stability

Lifting Agents/Convection


             CONVECTION works much like the
             bubbles that form in a pot of boiling
             water. (We talked about this earlier
             when we looked at how the
             atmosphere is heated).

             The warm surface heats the air above
             it. This warm, less dense air rises,
             expands, cools, and falls again,
             replacing the rising warm air below.
Chapter 1 – 7: Stability

Lifting Agents/Orographic Lift



             OROGRAPHIC LIFT occurs when air
             that is moving horizontally meets
             uneven terrain. It gets disturbed and
             is pushed upward.
Chapter 1 – 7: Stability

Lifting Agents/Frontal Lift


             FRONTAL LIFT occurs when a wedge
             of cold dense air moves horizontally
             and pushes under a mass of warm air
             (much like a snow plow). The warm
             air will be forced aloft.

             This is an example of a “Cold Front”
             (hence the term “Frontal Lift”).
Chapter 1 – 7: Stability

Lifting Agents/Mechanical Turbulence



             MECHANICAL TURBULENCE occurs
             when air that is moving horizontally
             meets an obstruction (e.g. a building
             or hangar). It is disturbed and
             becomes turbulent. This turbulence
             can cause the air to be pushed
             upward.
Chapter 1 – 7: Stability

Lifting Agents/Convergence



                When two horizontally opposing air
                masses meet, they will be forced to
                rise by CONVERGENCE.

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Chapter 1 met theory

  • 1. Meteorology - Chapter 1: Met Theory Topics: 1. The Atmosphere 2. Clouds 3. Pressure 4. Wind 5. Humidity 6. Temperature 7. Stability
  • 2. Chapter 1 – 1: The Atmosphere Atmospheric Composition The Earth’s ATMOSPHERE is made up of: -78% nitrogen -21% oxygen -1% rare gases (argon, carbon dioxide, water vapour)
  • 3. Chapter 1 – 1: The Atmosphere Water Vapour Of all of the ingredients that make up the atmosphere, the most important component for pilots is WATER VAPOUR. It is the water vapour that is responsible for the formation of clouds, fog, and precipitation. In other words, it is the water vapour that produces weather.
  • 4. Chapter 1 – 1: The Atmosphere Properties of the Atmosphere A parcel of atmospheric air processes 3 properties, namely mobility, capacity for expansion, and capacity for compression: MOBILITY – like a body of water over a river bed, a body of air can move over the Earth’s surface.
  • 5. Chapter 1 – 1: The Atmosphere Properties of the Atmosphere CAPACITY FOR EXPANSION – like a balloon, a parcel of air can expand. When it does, the parcel of air cools.
  • 6. Chapter 1 – 1: The Atmosphere Properties of the Atmosphere CAPACITY FOR COMPRESSION – like a deflating balloon, a parcel of air can compress. When it does, the temperature rises.
  • 7. Chapter 1 – 1: The Atmosphere Divisions of the Atmosphere The layer of atmosphere closest to the Earth is called the TROPOSPHERE. The Troposphere extends to a height of 28,000 feet at the Poles, and 54,000 feet at the Equator. In the Troposphere, air pressure, density, and temperature all decrease with increasing altitude. In other words, with increasing altitude, the air becomes lighter, thinner, and colder. Because almost all water vapour is found in the Troposphere, all active weather occurs in this layer.
  • 8. Chapter 1 – 1: The Atmosphere Divisions of the Atmosphere Above the Troposphere is a layer called the STRATOSPHERE. In the Stratosphere, the temperature ceases to drop, and remains at -56oC.
  • 9. Chapter 1 – 1: The Atmosphere Divisions of the Atmosphere The boundary layer separating the Troposphere from the Stratosphere is called the TROPOPAUSE.
  • 10. Chapter 1 – 1: The Atmosphere Divisions of the Atmosphere In an earlier chapter on Flight Instruments, we talked about “ICAO Standard Atmosphere”. (Recall that ICAO stands for “International Civil Aviation Organization”). This “standard” atmosphere is based on averages of atmospheric conditions at 49o of Latitude. By definition, ISA (ICAO Standard Atmosphere) is: -Pressure = 29.92” Hg (inches of Mercury) -Temperature = 15oC at sea level -Temperature Decrease (or Lapse Rate) = 2oC per 1,000 feet above sea level
  • 11. Chapter 1 – 2: Clouds High Clouds Clouds can be classified according to their altitude. HIGH clouds have bases starting from 16,500 feet to 45,000 feet. The name of these clouds are prefixed with “Cirro”.
  • 12. Chapter 1 – 2: Clouds Mid Level Clouds MID LEVEL clouds have bases starting from 6,500 feet to 23,000 feet. The name of mid level clouds are prefixed with “Alto”.
  • 13. Chapter 1 – 2: Clouds Low Level Clouds LOW LEVEL clouds have bases starting at the Earth’s surface, or up to 6,500 feet. The name of low level clouds have no prefix attached to them.
  • 14. Chapter 1 – 2: Clouds Cumulus Clouds Types of clouds can be further classified according to their characteristics. Clouds of vertical development (i.e. puffy or cotton ball type clouds) are called CUMULUS clouds.
  • 15. Chapter 1 – 2: Clouds Stratus Clouds Clouds that form in horizontal layers or sheet are called STRATUS clouds.
  • 16. Chapter 1 – 2: Clouds Fractus Clouds Clouds that are windblown or broken are referred to as FRACTUS clouds.
  • 17. Chapter 1 – 2: Clouds Nimbus Clouds And finally, clouds from which precipitation falls are called NIMBUS clouds.
  • 18. Chapter 1 – 2: Clouds Cloud Names Now, if we combine any of the above classifications of clouds with a cloud’s characteristics, we can determine the full name of a cloud. For example, a high level cloud that is cotton- like is called CIRROCUMULUS cloud. Cirro = high Cumulus = cotton-like
  • 19. Chapter 1 – 2: Clouds Cloud Names A high level cloud that is made up of sheets or layers of clouds is called CIRROSTRATUS cloud. Cirro = high Stratus = horizontal layers
  • 20. Chapter 1 – 2: Clouds Cloud Names A mid-level cloud that is rounded and puffy is called ALTOCUMULUS cloud. Alto = middle level Cumulus = puffy
  • 21. Chapter 1 – 2: Clouds Cloud Names A mid-level grey cloud that covers the whole sky is called ALTOSTRATUS cloud. Alto = middle level Stratus = horizontal formation
  • 22. Chapter 1 – 2: Clouds Cloud Names Low level cloud that resembles a series of patches or rounded masses is called CUMULUS cloud. no prefix = low level Cumulus = rounded masses
  • 23. Chapter 1 – 2: Clouds Cloud Names A uniform layer of low level cloud is called STRATUS cloud. no prefix = low level Stratus = layer cloud
  • 24. Chapter 1 – 2: Clouds Cloud Names Low level layer cloud that is windbroken is called STRATUSFRACTUS cloud. Stratus = layer cloud (horizontal formation) Fractus = windblown
  • 25. Chapter 1 – 2: Clouds Cloud Names Heavy masses of vertically developed cloud from which precipitation is falling is called CUMULONIMBUS cloud. Cumulo (from Cumulus) = mass cloud (vertical development) Nimbus = precipitation
  • 26. Chapter 1 – 2: Clouds Cloud Names Review your Environment Canada Clouds Poster included with your Groundschool kit for further cloud names and descriptions.
  • 27. Chapter 1 – 2: Clouds Sky Condition The SKY CONDITION refers to the amount of sky that is covered by cloud, as observed from the surface up. The sky condition can be any one of the following: -SKC = ‘sky clear’ = no cloud -FEW = ‘few’ = >0/8 to 2/8 cloud coverage -SCT = ‘scattered’ = 3/8 to 4/8 cloud coverage -BKN = ‘broken’ = 5/8 to <8/8 cloud coverage -OVC = ‘overcast’ = 8/8 cloud coverage
  • 28. Chapter 1 – 3: Pressure Atmospheric Pressure ATMOSPHERIC PRESSURE is the weight of the air above us. The greater the amount of air above us, or the greater the density of the air above us, the greater the downward pressure the air will apply on us. Atmospheric pressure changes from location to location. If there is dense, heavy air over an area, the pressure will be higher than under an area of less dense air.
  • 29. Chapter 1 – 3: Pressure Atmospheric Pressure The pressure (whether it be “high” pressure or “low” pressure) is important to pilots because it: -affects our altimeters (as discussed in the chapter on Flight Instruments) -controls the wind (as we will learn in this chapter)
  • 30. Chapter 1 – 3: Pressure Mercury Barometer For aviation purposes, pressure is measured with a Mercury Barometer. A simplified Mercury Barometer would be a dish filled with liquid mercury and an inverted test-tube held in the dish of mercury.
  • 31. Chapter 1 – 3: Pressure Mercury Barometer As the weight of the atmosphere increases (i.e. an increase in atmospheric pressure), it will push down on the surface of the mercury, thereby forcing it to rise up in the tube.
  • 32. Chapter 1 – 3: Pressure Mercury Barometer If we now measure how many inches the mercury rises in the tube, (e.g. 29.92 inches), then we can determine the altimeter setting. In this case, we would call the altimeter setting 29.92” Hg.
  • 33. Chapter 1 – 3: Pressure Mercury Barometer In aviation, we use inches of mercury (”Hg) to express atmospheric pressure. Other units used to measure pressure are millibars and kilopascals.
  • 34. Chapter 1 – 3: Pressure Isobars ISOBARS are lines drawn on a Weather Map that join places of equal atmospheric pressure. Isobars never cross one another, but tend to form circular patterns. Although we commonly use inches of mercury to express pressure in aviation, the Isobars on Weather Maps are presented in millibars.
  • 35. Chapter 1 – 3: Pressure Low Pressure Area If we examine the pattern that the Isobars form on this Weather Map, we notice that as we move from the center of the map to the upper right corner, the pressure continually drops. We therefore conclude that there is a “low” pressure area in the top right corner.
  • 36. Chapter 1 – 3: Pressure High Pressure Area Likewise, if we look at the pattern as we move from the center of the map to the bottom right corner, we notice that the pressure continually rises. This would indicate that there is a “high” pressure area in the bottom right corner.
  • 37. Chapter 1 – 3: Pressure High Pressure, Low Pressure Likewise, the pattern of Isobars would indicate a “high” pressure area in the upper left corner, and a “low” pressure area in the lower left corner of this Weather Map.
  • 38. Chapter 1 – 3: Pressure Trough A TROUGH is an elongated u-shaped area of low pressure. A trough is like a “valley” of low pressure.
  • 39. Chapter 1 – 3: Pressure Ridge A RIDGE is a protruding neck of high pressure. A ridge is like a “mountain range” of high pressure.
  • 40. Chapter 1 – 3: Pressure Col A COL is a “neutral” area between two high pressure areas and two low pressure areas.
  • 41. Chapter 1 – 3: Pressure Pressure Gradient PRESSURE GRADIENT is the rate of change of pressure over a given distance. The pressure gradient can be a shallow gradient (i.e. a small rate of change), or a steep gradient (i.e. a large rate of change).
  • 42. Chapter 1 – 3: Pressure Pressure Gradient The pressure gradient (or the nearness of the Isobars) is an indication of the strength of the wind. Where there is a shallow gradient (i.e. where the Isobars are far apart), there will be light winds. Where there is a steep gradient (i.e. where the Isobars are close together), the wind will be strong.
  • 43. Chapter 1 – 3: Pressure Wind WIND is simply air trying to move (as it wants to) from an area of high pressure to an area of lower pressure. Just like an inflated balloon, the air inside the balloon is under high pressure. The air outside the balloon is at a much lower pressure. The air wants to escape from the balloon. In other words, the air wants to move from the high pressure area to the low pressure area.
  • 44. Chapter 1 – 3: Pressure Wind So, if we had the above Weather Map, the air would want to move from the high pressure area to the low pressure area. The wind would tend to blow from the high to the low. However, as we are about to see, it gets a little more complicated than this…
  • 45. Chapter 1 – 3: Pressure Wind Because the Earth is not stationary, but is rotating beneath the atmosphere, the wind does not move in a straight line (relative to the Earth’s surface) as it attempts to move from a high pressure area to a low pressure area. It becomes influenced by a force called CORIOLIS FORCE. In the Northern Hemisphere, Coriolis Force causes the air movement to be deflected to the right (in relation to the Earth’s surface), causing it to flow parallel to the Isobars.
  • 46. Chapter 1 – 3: Pressure Wind If we had a high pressure area on either side of a low pressure area, we know that the wind would want to blow into the low (from high to low).
  • 47. Chapter 1 – 3: Pressure Wind However, Coriolis Force says that in its movement, the wind gets deflected to the right.
  • 48. Chapter 1 – 3: Pressure Wind This pattern shows how the wind tends to blow clockwise around a HIGH.
  • 49. Chapter 1 – 3: Pressure Wind It also shows how the wind tends to blow counter-clockwise around a LOW.
  • 50. Chapter 1 – 3: Pressure Wind Remember this picture to help you recall whether the wind blows clockwise or counter-clockwise around a high or low… It is a picture of a “high clock over top of a low counter”. high = clockwise low = counter-clockwise The wind blows clockwise around a high, and counter-clockwise around a low.
  • 51. Chapter 1 – 3: Pressure Wind Here’s another trick… When outdoors, you can always tell where the low pressure area is if you stand with your back to the wind…
  • 52. Chapter 1 – 3: Pressure Wind In this position, the low will be to your left.
  • 53. Chapter 1 – 3: Pressure Wind There is one more element that affects the precise direction of the wind. In fact, the wind does not blow exactly parallel to the Isobars. SURFACE FRICTION between the moving air and the Earth’s surface tends to slow down its motion and retards the effect of the Coriolis Force. Therefore, the air tends to move across the isobars at an angle inward toward a low, and outward from a high.
  • 54. Chapter 1 – 4: Wind Wind As you can imagine, the wind is a very important factor for pilots. The wind can have a negative or positive effect for us: - on takeoff - wind affects takeoff distance - wind affects takeoff safety (gusts, crosswind) - in cruise - wind affects groundspeed (time, fuel, money) - on landing - wind affects landing distance - wind affects landing safety (gusts, crosswind) We will now look at different types of wind…
  • 55. Chapter 1 – 4: Wind Sea Breeze A SEA BREEZE is a wind that blows from the sea (or a large body of water) to the land. Note: When referring to wind direction, we always refer to the direction from which it is blowing (e.g. a north wind blows from the north).
  • 56. Chapter 1 – 4: Wind Sea Breeze A Sea Breeze blows during the day. The Earth’s surface is a better conductor of heat than water. During the day, the sun heats the Earth (more-so than the water), which in turn heats the air above it. This warmed air (over the land) rises. Note: Warm air, which is less dense, tends to rise. Cool are, which is more dense, tends to sink.
  • 57. Chapter 1 – 4: Wind Sea Breeze This rising air (over the land) creates a low pressure area over the land. (Because the air is rising, there is less downward pressure created by the atmosphere, resulting in a lower pressure). In contrast, the air over the water (sea) will be of a higher pressure.
  • 58. Chapter 1 – 4: Wind Sea Breeze We know that the air tends to move from a high pressure area to a low pressure area. So, during the day, the wind will blow from the sea to the land, creating a Sea Breeze.
  • 59. Chapter 1 – 4: Wind Land Breeze A LAND BREEZE is a wind that blows from the land to the sea (or a large body of water).
  • 60. Chapter 1 – 4: Wind Land Breeze A Land Breeze works opposite to a Sea Breeze, and blows at night. At night, all the sun’s warmth radiates from the Earth’s surface into the upper atmosphere, and the air over the land becomes cool. Water retains heat better, so the air over the water remains warmer. The warmer air over the water will rise, creating a low pressure area over the water. In contrast, the air over the land will be of a higher pressure.
  • 61. Chapter 1 – 4: Wind Land Breeze With the high pressure over the land at night, the wind will blow from the land to the sea, creating a Land Breeze.
  • 62. Chapter 1 – 4: Wind Mountain Wind Wind in the vicinity of mountains can be extremely challenging for a pilot. In fact, it is recommended that you seek the advise (or perhaps even training) of a pilot with mountain flying experience before flying in the mountains. When the wind blows through a mountain valley, the valley creates a “funnel effect”, whereby the wind velocity increases substantially. This strong wind can also lead to pronounced turbulence. We’ll now look at some specific types of mountain winds…
  • 63. Chapter 1 – 4: Wind Mountain Wind An ANABATIC WIND blows up a mountain slope during the day. As the sun heats the dark surface of the mountain slope, the warmed surface radiates its heat to warm the air above it. This warm air rises, creating a wind that blows up the mountain slope.
  • 64. Chapter 1 – 4: Wind Mountain Wind A KATABATIC WIND blows down a mountain slope. If the mountain tops are snow covered, the air at the caps will be cooled. This cold dense air will sink, causing the wind to blow down the slope. An Anabatic Wind can turn into a Katabatic Wind at night. The removal of the sun’s heat causes the mountain slope to cool, thereby cooling the air above it. Again, this cool dense air will flow down the mountain slope.
  • 65. Chapter 1 – 4: Wind Mountain Wind A MOUNTAIN WAVE forms when the wind blows over the top of a mountain peak. Just like the airflow over the top of a wing, the wind blowing over a mountain top will have: -increased speed -decreased pressure -decreased temperature In the chapter on Flight Instruments, we learned how this effect can cause the Altimeter to read in error by as much as 3,000 feet! The decreased temperature can lead to airframe icing (ice accumulation on the airplane).
  • 66. Chapter 1 – 4: Wind Mountain Wind Turbulence associated with a mountain wave is most frequent and most severe just beneath the wave crest at or below mountaintop level.
  • 67. Chapter 1 – 4: Wind Mountain Wind On the leeward side of the mountain there can be strong downdrafts (as much as 2000 to 5000 feet per minute) and very turbulent eddies.
  • 68. Chapter 1 – 4: Wind Wind Gust A wind GUST is a rapid change of wind speed or direction, that is of brief duration (seconds). Gusts are usually caused by obstacles being in the way of the wind’s path (e.g. hangars, buildings, irregular terrain, etc.)
  • 69. Chapter 1 – 4: Wind Wind Squall A wind SQUALL is a rapid change of wind speed or direction, that is of prolonged duration. A squall is usually caused by the passage of a fast moving cold front.
  • 70. Chapter 1 – 4: Wind Eddies/Mechanical Turbulence EDDIES, also known as MECHANICAL TURBULENCE, is disturbed airflow (similar to eddies of water in a river or stream). They are caused by irregular surfaces in the wind’s path (like rocks in a shallow river) such as hills, buildings, etc. Mechanical Turbulence only occurs in the lower levels of the atmosphere (usually below 3,000 feet), and depends on the strength of the wind being disturbed.
  • 71. Chapter 1 – 4: Wind Wind Shear A wind SHEAR is a sudden or violent change in wind speed or direction. Wind shears are most commonly associated with thunderstorms. They can be extremely dangerous because the wind can change much faster than an airplane’s ability to accelerate or decelerate. They are especially dangerous near the ground during takeoff and landing.
  • 72. Chapter 1 – 4: Wind Jet Stream A JET STREAM is a tube-like band of high speed wind at high altitudes (20,000 to 40,000 feet). This band can be from 3,000 to 7,000 feet thick, with a core wind of 100 to 150 knots. This wind flows from west to east. There are two Jet Streams across North America: one lies approximately across Canada and the other across the USA. The Jet Streams migrate south in the summer, and move back north in the winter.
  • 73. Chapter 1 – 4: Wind Clear Air Turbulence CLEAR AIR TURBULENCE (CAT) is a very turbulent condition that occurs in a cloudless sky, usually associated with a Jet Stream or Mountain Wave. Because it occurs in a clear sky, CAT is almost impossible to forecast.
  • 74. Chapter 1 – 4: Wind Wind Speed and Direction In aviation, wind speed is expressed in knots (nautical miles per hour). Wind direction is the direction from which it is blowing. Using the compass rose to express precise direction, a wind blowing from the south would be a wind of 180o.
  • 75. Chapter 1 – 4: Wind Wind Speed and Direction A wind of 040o would be blowing from the north-east (NE).
  • 76. Chapter 1 – 4: Wind Wind Speed and Direction A VEER is a clockwise change in wind direction. For example, if the wind changed from 270o to 300o, we would say that the wind veered.
  • 77. Chapter 1 – 4: Wind Wind Speed and Direction A BACK is a counter-clockwise change in wind direction. For example, if the wind changed from 270o to 240o, we would say that the wind backed.
  • 78. Chapter 1 – 4: Wind Diurnal (Daily) Wind Variations We all know that the wind tends to increase during a hot afternoon, and then calms at night. This is due to Diurnal Variation…
  • 79. Chapter 1 – 4: Wind Diurnal (Daily) Wind Variations During the hot afternoon, the sun heats the Earth’s surface. The Earth then heats the air above it by radiation. This warming air rises. As it rises, it expands, cools, and begins to fall again. As it falls, it transfers the higher level wind (from about 3,000 feet) to the surface. The higher level wind in unaffected by surface friction and is therefore stronger, and flows more parallel to the Isobars.
  • 80. Chapter 1 – 4: Wind Diurnal (Daily) Wind Variations As a result, during the daytime, the wind veers and increases in strength. At night, the wind resumes its normal direction and speed: it backs and decreases.
  • 81. Chapter 1 – 5: Humidity Humidity HUMIDITY is the amount of moisture in the air. This moisture can be one of 2 forms: - invisible form (which is water vapour) - visible form (which is water droplets or ice crystals, making up clouds or fog)
  • 82. Chapter 1 – 5: Humidity Condensation CONDENSATION is when water vapour changes into water droplets. In other words, the moisture changes from a gas to a liquid, or from its invisible form to its visible form. Condensation can be seen as moisture on the inside of a window on a cold winter day.
  • 83. Chapter 1 – 5: Humidity Sublimation SUBLIMATION is when water vapour changes into ice crystals. In other words, the moisture changes from a gas to a solid. Again, it changes from its invisible form to its visible form, but in this case, the liquid stage is bypassed. Sublimation can be seen as frost on a car window on a cold winter morning.
  • 84. Chapter 1 – 5: Humidity Sublimation Here is an important point to remember about humidity: Warm air can hold more moisture than cold air A parcel of warm air has the ability to hold more water molecules than a similar parcel of cold air.
  • 85. Chapter 1 – 5: Humidity Saturated Air SATURATED AIR is when a parcel of air contains the maximum amount of water vapour that it can hold at a given temperature.
  • 86. Chapter 1 – 5: Humidity Saturated Air If the air is saturated (i.e. it contains all the moisture it can hold), and then the temperature drops, that parcel of air will have more moisture than it can hold. (Remember: warm air can hold more moisture than cold air). This excess moisture (or vapour) will be forced into condensation or sublimation. The excess moisture will change from its invisible form to its visible form, creating either cloud, fog, dew, or frost. You’ve noticed that fog, dew and frost tend to form at night, when the temperature drops. Clouds form in the higher altitudes. Remember… the temperature decreases with increasing altitude.
  • 87. Chapter 1 – 5: Humidity Saturated Air So, saturated air can be forced into condensation or sublimation be decreasing the temperature. Another way for this to happen is to increase the moisture content of the air. If the air is already saturated, then adding more moisture will also force the excess vapour into condensation or sublimation. An example of this is when you see your breath on a cold day (since the air you breathe out has a lot of moisture in it from your lings)
  • 88. Chapter 1 – 5: Humidity Super-Cooled Water Droplets SUPER-COOLED WATER DROPLETS are liquid water droplets that exist in the liquid form at temperatures well below 0oC. This is a condition that does not normally happen, and requires specific atmospheric conditions to exist. They are sometimes associated with thunderstorms cells. They can exist at temperatures as low as -40oC. Super-cooled water droplets are a hazard because, when they are disturbed (e.g. by a wing), they turn into ice instantaneously. They create a rapid accumulation of airframe icing.
  • 89. Chapter 1 – 5: Humidity Dewpoint The DEWPOINT is the temperature to which unsaturated air must be cooled to become saturated. The dewpoint is the temperature at which invisible moisture changes into visible moisture. It is the temperature at which fog, dew, frost, or clouds form.
  • 90. Chapter 1 – 5: Humidity Relative Humidity RELATIVE HUMIDITY is the ratio of the amount of water vapour present in the air to the amount it would hold if it were saturated (at the same pressure and temperature). For example, if the air is holding 80% of the moisture that it can hold, then we say that the Relative Humidity is 80%. Saturated air has a Relative Humidity of 100%.
  • 91. Chapter 1 – 5: Humidity Relative Humidity If a parcel of air is heated, then its Relative Humidity decreases. (Remember: warm air can hold more moisture than cold air). If a parcel of air is cooled, then its Relative Humidity increases.
  • 92. Chapter 1 – 5: Humidity Relative Humidity The smaller the spread between the temperature and the dewpoint, the higher the Relative Humidity.
  • 93. Chapter 1 – 6: Temperature Temperature As we’ve already stated, the sun heats the Earth, and the Earth heats the atmosphere above it by radiation. This is an important point to remember. The atmosphere is heated from below, not from above.
  • 94. Chapter 1 – 6: Temperature Seasonal Variation So, why is the atmosphere’s temperature different at different places? One reason is due to SEASONAL VARIATION. The Earth’s axis of rotation is not perpendicular to the Earth’s path of travel, but is at a “tilt”. Hence, during North America’s summer months, the sun’s rays are more perpendicular to the continent’s surface (shine from overhead). But in the winter, the sun is lower on the horizon, so the sun’s rays are at more of an angle to the continent’s surface.
  • 95. Chapter 1 – 6: Temperature Seasonal Variation Like a beam of light shining directly onto a surface, the light’s rays are concentrated in a small area. But if we shine the light at an angle to the surface, then that same beam covers a larger surface area. If both beams are producing the same amount of energy (heat), then the beam of light shining from directly above will concentrate its heat over a smaller are. Therefore, this surface will be warmer. The sun has the same effect on the Earth’s surface in summer vs. winter.
  • 96. Chapter 1 – 6: Temperature Latitudinal Variation This same principle explains LATITUDINAL VARIATION of the Earth’s temperature. Locations near the Equator have the sun more directly overhead than locations further north or south of the Equator. Hence, near the Equator the temperatures are warmer.
  • 97. Chapter 1 – 6: Temperature Topography TOPOGRAPHY (the makeup of the Earth’s surface) also has an effect on temperature. Since dark colours absorb more light than light colours do (this is Physics!), dark colours get warmer when the sun shines on them. The same holds true for the Earth’s surface. Dark coloured terrain (dark soil, asphalt, etc.) gets hotter than does light coloured terrain (water, snow, etc.). Therefore, the atmosphere above a dark surface will be warmer.
  • 98. Chapter 1 – 6: Temperature Cloud Cover CLOUD COVER can have an effect on temperature. During the day, the absence of cloud cover allows for maximum heat from the sun to heat the Earth’s surface, creating warmer air (by radiation). However, at night, a clear sky allows all the Earth’s heat (gained during the daytime) to radiate into the upper atmosphere, creating cool temperatures at the surface. A cloudy night produces a sort of blanket, keeping the heat near the surface, creating a warmer night.
  • 99. Chapter 1 – 6: Temperature How the Atmosphere is Heated The atmosphere can be heated by any one of 4 methods: -Convection -Advection -Turbulence -Compression We will look at each of these…
  • 100. Chapter 1 – 6: Temperature How the Atmosphere is Heated/Convection CONVECTION works much like bubbles that form in a pot of boiling water. The air nearest the Earth’s surface is warmed. Because warm air is less dense than cold air, it begins to rise. As it rises, it cools, by expansion. (Remember… at higher altitudes the pressure decreases, allowing the air to expand. When it expands, it cools). As the air cools, it becomes more dense (heavier), and begins to fall again, replacing the rising warm air below. It is the rising air that warms the air aloft.
  • 101. Chapter 1 – 6: Temperature How the Atmosphere is Heated/Advection ADVECTION refers to the horizontal movement of air from one place to another. Advection heating occurs when cool air moves over a warm surface. The warm surface warms the air above it.
  • 102. Chapter 1 – 6: Temperature How the Atmosphere is Heated/Turbulence When an obstruction in the path of the air’s movement (such as a hill or irregular terrain) disturbs it, TURBULENCE is created. This turbulence can push the warm air aloft.
  • 103. Chapter 1 – 6: Temperature How the Atmosphere is Heated/Compression When a parcel of air is COMPRESSED, it warms. This can occur on the leeward side of a mountain range. As the air flows down the mountain, it is compressed at the mountain’s base. The compressed air becomes warmer.
  • 104. Chapter 1 – 6: Temperature How the Atmosphere is Cooled The atmosphere can be cooled by any one of 3 methods: -Radiation -Advection -Expansion We will look at each of these…
  • 105. Chapter 1 – 6: Temperature How the Atmosphere is Cooled/Radiation At night, solar RADIATION ceases. All the heat absorbed by the Earth’s surface from the previous day radiates, or transfers, into the upper atmosphere. As a result, the lower levels of the atmosphere cool.
  • 106. Chapter 1 – 6: Temperature How the Atmosphere is Cooled/Advection Remember, ADVECTION refers to the horizontal movement of air from one place to another. Advection cooling occurs when warm air moves over a cool surface. The cool surface cools the air above it.
  • 107. Chapter 1 – 6: Temperature How the Atmosphere is Cooled/Expansion When a parcel of air EXPANDS, it cools. (This is the opposite of compression). If you’ve ever used a can of spray paint, then you’ve experienced this. The paint inside the can is under compression. As it comes out of the nozzle, it expands, and cools. You may have noticed that the tip of your finger on the nozzle gets cold!
  • 108. Chapter 1 – 6: Temperature How the Atmosphere is Cooled/Expansion The same thing happens when air is forced to rise… the pressure decreases, so the air expands. When it expands, the temperature decreases.
  • 109. Chapter 1 – 6: Temperature Isotherms ISOTHERMS are lines drawn on a Weather Map that join places of equal temperature.
  • 110. Chapter 1 – 6: Temperature Temperature Scales The international aeronautical unit used to express temperature is Degrees Celsius. In Degrees Celsius: - the freezing point of water = 0oC - the boiling point of water = 100oC However, you may come across some airplane manuals (especially for airplanes built in the USA) that express temperature in Degrees Fahrenheit. In Degrees Fahrenheit: - the freezing point of water = 32oF - the boiling point of water = 212oF
  • 111. Chapter 1 – 6: Temperature Temperature Scales To convert from oC to oF: oF = 9/5 oC + 32 oC = 5/9 (oF – 32) Or, simply use your E6B Flight Computer!
  • 112. Chapter 1 – 6: Temperature Density vs. Temperature Cold air is more dense than warm air. Therefore, it is heavier and tends to sink. Warm air is less dense, or lighter, and tends to rise.
  • 113. Chapter 1 – 6: Temperature Lapse Rate LAPSE RATE is the rate of decrease in temperature with height. There are 3 different Lapse Rates: - ICAO Standard Lapse Rate - Dry Adiabatic Lapse Rate - Saturated Adiabatic Lapse Rate We will look at each of these…
  • 114. Chapter 1 – 6: Temperature ICAO Standard Lapse Rate The ICAO STANDARD LAPSE RATE is an average lapse rate, as derived by ICAO. (Remember, ICAO = International Civil Aviation Organization). This standard lapse rate is 1.98oC/1000 feet For simplicity, we commonly say that it is 2oC/1000 feet. This ICAO Standard Lapse Rate is an assumption used for the calibration of aircraft Altimeters.
  • 115. Chapter 1 – 6: Temperature Dry Adiabatic Lapse Rate The DRY ADIABATIC LAPSE RATE is the actual lapse rate in air that is not saturated. This is the lapse rate when the temperature is greater that the dewpoint. By definition, this lapse rate is 3oC/1000 feet.
  • 116. Chapter 1 – 6: Temperature Standard Adiabatic Lapse Rate The SATURATED ADIABATIC LAPSE RATE (or sometimes called the WET ADIABATIC LAPSE RATE) is the lapse rate in air that is saturated. This is the lapse rate when the temperature meets the dewpoint. (Remember that at the dewpoint, moisture changes into its visible form. Clouds form at the dewpoint. The base of clouds, then, represents the altitude at which the temperature meets the dewpoint). By definition, the Saturated Adiabatic Lapse Rate is 1.5oC/1000 feet. So, at or above the base of clouds, the lapse rate becomes 1.5oC/1000 feet.
  • 117. Chapter 1 – 6: Temperature Standard Adiabatic Lapse Rate Here is a sample problem: Question: If the surface temperature is 10oC and the dewpoint is 1oC, what is the altitude of the base of the clouds? Solution: We know that below the cloud base, the air is unsaturated, so the lapse rate is 3oC/1000 feet (we use the Dry Adiabatic Lapse Rate below the cloud base). So, at: -1000 feet above ground, the temperature = 7oC -2000 feet above ground, the temperature = 4oC -3000 feet above ground, the temperature = 1oC Therefore, at 3000 feet we’ve reached the dewpoint of 1oC, and cloud will begin to form.
  • 118. Chapter 1 – 6: Temperature Inversion An INVERSION is when the temperature increases with height. Inversions are not the norm. They are usually associated with a frontal surface. (We will talk more about fronts soon).
  • 119. Chapter 1 – 6: Temperature Isothermal Layer An ISOTHERMAL LAYER is when the temperature remains constant (neither decreases nor increases) throughout a layer for some depth.
  • 120. Chapter 1 – 7: Stability Stability STABLE air is air that resists upward of downward displacement. UNSTABLE air is air that tends to move further away when displaced.
  • 121. Chapter 1 – 7: Stability Unstable Air If a parcel of air is warmer than the surrounding air, it will tend to rise. (Remember: warm air is less dense, or lighter, then cool air) This parcel of air is therefore unstable.
  • 122. Chapter 1 – 7: Stability Stable Air Air that is cooler than the surrounding air will resist upward motion. (Remember: cool air is more dense and therefore will not want to rise) This parcel of air is therefore stable.
  • 123. Chapter 1 – 7: Stability Lapse Rate vs. Stability The steeper the lapse rate, the more unstable the air.
  • 124. Chapter 1 – 7: Stability Flight Characteristics in Stable Air Flight through STABLE air will provide the following flight characteristics: - poor low level visibility (because stable air tends not to rise, so the pollutants get trapped near the surface) - stratus type cloud (layer cloud) - steady precipitation (e.g. that “all day” type of rain, which is characteristic of stratus type cloud) - steady (constant) winds - smooth flying conditions
  • 125. Chapter 1 – 7: Stability Flight Characteristics in Unstable Air Flight through UNSTABLE air will provide the following flight characteristics: - good visibility (except in precipitation) - cumulus type cloud (heap type cloud of vertical development, built from unstable, rising air) - showery precipitation (e.g. “bursts” of rain, which are characteristic of cumulus type cloud) - gusty winds - turbulent flying conditions (produced by rising columns of unstable air) - smooth flying conditions
  • 126. Chapter 1 – 7: Stability Lifting Agents LIFTING AGENTS are the forces or conditions that provide the lift to initiate rising currents of air. If a lifting agent provides a force onto a parcel of unstable air, then this air will experience significant lift. Stable air will have substantially less lift. When air is lifted to a higher altitude, it expands and cools. If it expands and cools sufficiently, then cloud formation occurs, and hence weather is produced.
  • 127. Chapter 1 – 7: Stability Lifting Agents There are 5 different Lifting Agents: -Convection -Orographic Lift -Frontal Lift -Mechanical Lift -Convergence We will look at each of these…
  • 128. Chapter 1 – 7: Stability Lifting Agents/Convection CONVECTION works much like the bubbles that form in a pot of boiling water. (We talked about this earlier when we looked at how the atmosphere is heated). The warm surface heats the air above it. This warm, less dense air rises, expands, cools, and falls again, replacing the rising warm air below.
  • 129. Chapter 1 – 7: Stability Lifting Agents/Orographic Lift OROGRAPHIC LIFT occurs when air that is moving horizontally meets uneven terrain. It gets disturbed and is pushed upward.
  • 130. Chapter 1 – 7: Stability Lifting Agents/Frontal Lift FRONTAL LIFT occurs when a wedge of cold dense air moves horizontally and pushes under a mass of warm air (much like a snow plow). The warm air will be forced aloft. This is an example of a “Cold Front” (hence the term “Frontal Lift”).
  • 131. Chapter 1 – 7: Stability Lifting Agents/Mechanical Turbulence MECHANICAL TURBULENCE occurs when air that is moving horizontally meets an obstruction (e.g. a building or hangar). It is disturbed and becomes turbulent. This turbulence can cause the air to be pushed upward.
  • 132. Chapter 1 – 7: Stability Lifting Agents/Convergence When two horizontally opposing air masses meet, they will be forced to rise by CONVERGENCE.