chapter 18

114
Chapter 18 Moisture, Clouds, and Precipitation

Upload: jmchenry071

Post on 15-Jan-2015

7.018 views

Category:

Business


3 download

DESCRIPTION

 

TRANSCRIPT

Page 1: Chapter 18

Chapter 18

Moisture, Clouds, and Precipitation

Page 2: Chapter 18

Water in the Atmosphere

Water vapor is the source of all condensation and precipitation, which is any form of water that falls from a cloud.

When understanding atmospheric processes, water vapor is the most important gas in the atmosphere.

Atmospheric water vapor varies form 0-4% by volume.

Page 3: Chapter 18

Water’s Changes of State

Its actually is a resident of OhioStupid humor…hehehehehheheehe

Water can exist in all three states of matter at temperatures and pressures that exist on Earth.

Page 4: Chapter 18

Changes of State

Page 5: Chapter 18

The Water Cycle

The water cycle begins with evaporation, then water condenses, precipitation occurs, and finally water either becomes runoff or ground water.

If all the water in the atmosphere were to fall as precipitation it would only be 2mm deep.

Page 6: Chapter 18

Water cycle

Page 7: Chapter 18

Solid to Liquid

The process of changing state requires that energy be transferred in the form of heat.

So what is melting?

Page 8: Chapter 18

“Hidden Heat” When heat is transferred to a glass of ice water,

the temperature of the ice water remains a constant 00C….until all the ice has melted.

If adding heat does not raise the temperature, then where does the heat go?

In this case, the added heat breaks apart the crystal structure of the ice cubes. The bonds between the ice crystals are broken forming liquid water. This is called melting.

Page 9: Chapter 18

Latent Heat

Since the heat did not change the temperature of the ice water, the heat is referred to latent heat.

This energy is measured in joules or calories and is stored in the liquid and is not released until the water returns to the solid state.

Page 10: Chapter 18

Latent and Sensible Heat .5 calories needed to raise 1 gram of ice 1

°C. 80 calories needed to melt 1 gram of ice at

0 °C to water at 0 °C. 1 calorie needed to raise 1 g of water 1 °C. 539 calories needed to evaporate 1 g water

at 100 °C. .5 calories needed to raise 1 g of water

vapor 1 °C.

Page 11: Chapter 18
Page 12: Chapter 18

Question??

How many calories would it take to raise the temperature of 1 gram of ice at –2 °C to 102 °C?

Answer: 721 calories

Page 13: Chapter 18

Importance of Latent Heat

Latent heat is important in the formation of tall cumulus clouds, and is an energy source for thunderstorms, tornadoes, and hurricanes.

Page 14: Chapter 18

Liquid to Gas The process that changes liquid to gas is called

evaporation. The 2258 joules of energy provides enough

motion to allow one gram of water to escape the surface and become a gas.

Example: Stepping from a swimming pool feels cool because the heat from your body causes evaporation to occur. Therefore, evaporation is a cooling process.

Page 15: Chapter 18

Condensation When water changes from a gas to a

liquid condensation occurs. For condensation to occur molecules must release their stored energy or latent heat.

This energy is equal to the amount of energy absorbed during evaporation. How many calories or joules per gram??

Examples include: fog and cloud formation

Page 16: Chapter 18

Solid to Gas Sublimation is the conversion from a solid

to directly to a gas, without passing through the liquid state.

Examples: dry ice or carbon dioxide ice as in fire extinguishers. On occasion crystal-like frost can go through the same process.

Deposition is the reverse process, the conversion of a gas directly to a solid.

Example: When frost forms on cold objects like grass or car windows

Page 17: Chapter 18

Humidity

Humidity is the term that applies to water vapor in the air.

Two important terms include: Relative humidity Dew point

Page 18: Chapter 18

Saturation

As water molecules escape the surface and are added to the air, the pressure in the air increases.

This forces water molecules to return to the liquid state.

Eventually, the number of water molecules returning to the surface will balance the number leaving.

Page 19: Chapter 18

Saturation

At this point the air is said to be saturated.

The amount of water vapor required for saturation depends upon temperature.

When saturated, warm air contains more water vapor than cool air.

Page 20: Chapter 18

Relative Humidity

Is the ratio of the air’s actual water vapor content compared to the amount of water vapor the air can hold at that temperature and pressure.

Relative humidity indicates how close the air is to saturation.

Page 21: Chapter 18

Relative humidity can change two ways: 1. By adding or removing water vaporExample: evaporation 2. Temperature changes

Once air has become saturated, relative humidity does not change.

Page 22: Chapter 18

Condensation and Cloud Formation

Cooling the air causes condensation, which keeps air at its saturation level for that temperature.

Condensation above the Earth’s surface causes cloud formation.

Water droplets forming clouds are no longer part of the water vapor content of the air.

Page 23: Chapter 18

Lets Summarize

When the water vapor content of the air remains constant, lowering the temperature causes an increase in relative humidity.

And raising the air temperature causes a decrease in relative humidity.

Page 24: Chapter 18

Dew Point

Dew point is the temperature to which a parcel of air would need to be cooled to reach saturation.

During evening hours, an object near the ground often cool below the dew point temperature and becomes coated with water or dew.

Page 25: Chapter 18

Temp. vs. Saturation

For every 100C increase in temperature, the amount of water vapor needed for saturation doubles.

00C saturated air contains about half the water vapor as saturated air at100C.

00C saturated air contains about 1/4th the water vapor as saturated air at 200C.

Page 26: Chapter 18

Generally speaking… higher dew point temperatures indicate moist air, and lower dew point temperatures indicate dry air.

Page 27: Chapter 18

Measuring Humidity

A hygrometer is generally used to measure relative humidity. One type of hygrometer is a psychrometer, which consists of two identical thermometers.

One is dry and is the dry-bulb temperature, the other has a wick and is dipped in water and is called the wet-bulb thermometer.

Page 28: Chapter 18

Reading a Psychrometer

Evaporation of the water causes the wet-bulb temperature to drop.

The amount of cooling that takes place is directly proportional to the dryness of the air.

Page 29: Chapter 18

Reading a Psychrometer

The greater the difference between the wet-bulb and the dry-bulb temperatures indicates a lower relative humidity.

Page 30: Chapter 18

If the air is saturated, than little evaporation occurs, the difference between the two thermometers is slight and the relative humidity is high.

Page 31: Chapter 18

Figuring Relative Humidity

Page 32: Chapter 18

Cloud Formation

Air Compression and Expansion When air is compressed, the motion

of gas molecules increases and the air temperature rises.

As air rises, it expands. As it expands, it cools.

Page 33: Chapter 18

Adiabatic temperature Changes

Temperature changes that happen even though heat isn’t added or subtracted are called adiabatic temperature changes.

These changes result when air is compressed or expands.

Page 34: Chapter 18

Expansion and Cooling

As you gain altitude above the Earth’s surface, the atmospheric pressure decreases due to…..

the fact that there are fewer and fewer gas molecules.

Page 35: Chapter 18

Dry Adiabatic Lapse Rate

This results in air expanding and cooling as it rises.

Unsaturated air-cools at a constant rate of 100C for every 1000 meters of ascent.

Descending air encounters higher pressure; it compresses, and is heated 100C for every 1000 meters it moves downward.

Page 36: Chapter 18

Condensation If a parcel of air rises high enough, it will

eventually cool below its dew point. Here the process of condensation begins. From here on latent heat in the water

vapor will be released. Although the air will continue to cool after

condensation begins, the latent heat works against the adiabatic cooling process and cools slower.

Page 37: Chapter 18

Wet Adiabatic Lapse Rate

This slower rate of cooling caused by the addition of latent heat is called the wet adiabatic rate.

Remember, as condensation occurs, heat is released to the atmosphere.

Page 38: Chapter 18

Adiabatic Lapse Rates

Page 39: Chapter 18

Processes That Lift Air

In general, air resists vertical movement. Air near the surface tends to stay near the surface.

 Four mechanisms that can cause air to rise: Orographic lifting Frontal wedging Convergence Localized convective lifting

Page 40: Chapter 18

Orographic lifting

Occurs when terrains, such as mountains, act as barriers to air flow.

As air goes up a mountain slope, adiabatic cooling often generates clouds and precipitation.

Rain falls on the windward side of the mountain.

Page 41: Chapter 18

Leeward Loses Water

By the time air reaches the leeward side of this mountain, much of its moisture has been lost. If the air descends, it warms adiabatically.

This makes condensation and precipitation even less likely.

Page 42: Chapter 18

Rain Shadow

Rain shadow deserts from on leeward sides of mountains….

Example: Great Basin Desert in Southwestern U.S. is separated from the Pacific Ocean by the Sierra Nevada Mountains.

Page 43: Chapter 18
Page 44: Chapter 18
Page 45: Chapter 18

Orographic Lifting

Page 46: Chapter 18

Frontal Wedging

In central North America, masses of warm and cool air collide, producing a front.

Cooler, denser air acts as a barrier over which warmer less dense air rises.

This process is called frontal wedging. Weather producing fronts are associated with storm systems.

Page 47: Chapter 18

Frontal Wedging

Page 48: Chapter 18

Convergence

Occurs when air in the lower atmosphere flows together lifting results.

This is called convergence. When air flows together from more than one direction, it must go somewhere.

As this air rises leading to adiabatic cooling and possibly cloud formation.

Page 49: Chapter 18

Florida Example The Florida peninsula is an example of

where convergence can occur. During the day, ocean air flows inland along both coasts.

This causes a “pile up” of air over the coasts and convergence inland.

This uplift causes intense solar heating inland.

This situation causes a great many mid-afternoon thunderstorms.

Page 50: Chapter 18

Convergence

Page 51: Chapter 18

Localized Convective Uplifting On warm summer days, unequal heating of the

Earth’s surface may cause pockets of air to be warmed more than the surrounding air.

Example: Mall parking lot compared to a grassy field. As a result the air above the warm parking lot rises and is replaced by cooler surrounding air.

The rising warm air is called a thermal. The process that produces rising thermals is

localized convective uplift.

Page 52: Chapter 18

Localized Convective Lifting

Page 53: Chapter 18

Animal Uses…

Birds like hawks, vultures, and eagles use thermals to carry them.  

When warm parcels of air above the condensation level, clouds form.

These clouds may produce mid-afternoon rain showers.

Page 54: Chapter 18

Density Differences

Hot air rises because it is less dense than cold air.

Cold air sinks because it is more dense.

A parcel of air at a given temperature will rise until it reaches a density equilibrium.

Page 55: Chapter 18

Stability

If a volume of air were forced to rise, its temperature would drop because of expansion.

If this volume of air was cooler than the surrounding environment, it would be denser, and if allowed to do so, it would sink to its original position.

Air of this type, called stable air, resists vertical movement.

Page 56: Chapter 18

Balloon Example What causes a hot air balloon to rise?

Warmer air that is less dense than the surrounding air

Ok, now what causes a hot air balloon to stop rising?

The balloon will stop rising when the air inside the balloon equalizes with the air outside the balloon.

The warmer rising air is classified as unstable air.

Page 57: Chapter 18

So……

Stable air tends to remain in its original position, while unstable air tends to rise.

Page 58: Chapter 18

Degrees of Stability

Air is stable when the temperature decreases gradually with increasing altitude.

The most stable conditions happen when the air temperature actually increases with height, called a temperature inversion.

Page 59: Chapter 18

Conditionally Stable

Page 60: Chapter 18

Very Stable Atmosphere

Page 61: Chapter 18

Temperature Inversions

Temperature inversions frequently happen on clear nights as a result of radiation cooling off Earth’s surface.

The inversion is created because the ground and the air above the ground cools faster than the air higher above the ground.

Page 62: Chapter 18

Temperature Inversion

Page 63: Chapter 18

Stability and Daily Weather

When stable air is forced above Earth’s surface, the clouds that form are widespread and have little vertical thickness when compared to their horizontal dimension. Precipitation, if any, is light to moderate.

Page 64: Chapter 18

Storm Clouds

Clouds associated with the lifting of unstable air are towering and often generate thunderstorms and occasionally tornadoes. Called Cumulonimbus Clouds

Page 65: Chapter 18

Cumulonimbus Cloud

Page 66: Chapter 18

Review Condensation

The forms of condensation include dew, fog, or clouds.

For condensation to occur, the air must be saturated.

Saturation most often occurs when air is cooled to its dew point.

Page 67: Chapter 18

Types of Surfaces

Generally, there must be a surface for or water vapor to condense on.

Dew forms on surfaces near the ground. Clouds form on tiny bits of particulate

matter called condensation nuclei. This material includes dust, smoke, and

salt particles.

Page 68: Chapter 18

CCN (Cloud Condensation Nuclei)

If condensation nuclei were not present in the atmosphere the relative humidity would need to exceed 100% to form clouds.

Since they are present, the relative humidity rarely exceeds 100%.

Page 69: Chapter 18

CCN

Salt particles are excellent condensation nuclei since they absorb water.

Clouds then are formed from millions of tiny bits of water droplets that are so tiny, they stay suspended in the air.

Page 70: Chapter 18

Cloud Types and Precipitation

Clouds are classified on the basis of their form and height.

Page 71: Chapter 18

Types of Clouds

There are three basic cloud forms:1. cirrus – high, white, thin clouds. Described as

wispy or feathery in appearance.2. cumulus – cauliflower in appearance. These

clouds can have a lot of vertical height and are generally flat on the bottom.

3. stratus – described as sheets or layers that blanket the sky. They do not appear to have individual cloud units.

Page 72: Chapter 18

Altitude Heights

There are three levels of cloud heights:

High (cirro) – cloud base is above 6000 meters

Middle (alto) – cloud occupy heights between 2000 & 6000 meters.

Low – form below 2000 meters

Page 73: Chapter 18
Page 74: Chapter 18

High clouds

Three types1 – cirrus2 – cirrostratus3 – cirrocumulus High clouds are made of ice crystals. These

clouds generally do not produce precipitation.

However, if they follow each other increasing in coverage they may warn of approaching stormy weather.

Page 75: Chapter 18
Page 76: Chapter 18
Page 77: Chapter 18

Middle clouds

These clouds have the prefix “alto” as part of their name.

Altocumulus or altostratus They may produce infrequent light

drizzle or snow

Page 78: Chapter 18
Page 79: Chapter 18

Low clouds

Three types1- stratus2 – stratocumulus, appear as long

parallel rows that blanket the sky3 – nimbostratus, are rain clouds.

These clouds make precipitation and are formed from stable air.

Page 80: Chapter 18
Page 81: Chapter 18

Clouds of Vertical Development

These clouds form from unstable air. Cumulus clouds are often associated with good weather, but when vertical development begins it accelerates and generally ends in a cumulonimbus or thunderstorm cloud.

Page 82: Chapter 18
Page 83: Chapter 18
Page 84: Chapter 18

Fog

Physically fog and clouds are the same. Fogs result from radiation cooling or the

movement of air over a cool surface. Fogs can also form when enough water

vapor is added to the air to bring about saturation.

Fog is defined as a cloud with its base at or very near the ground.

Page 85: Chapter 18

Fogs Caused by Cooling

A blanket of fog is produced in some West Coast locations when warm, moist air from the Pacific Ocean moves over the cold California Current and then is carried on shore.

Page 86: Chapter 18

Fogs can also form on calm, clear, cool nights when Earth’s surface cools rapidly by radiation.

As the night progresses, a thin layer of air in contact with the ground cools below dew point.

As the air cools, it becomes denser and drains into low areas such as river valleys.

Page 87: Chapter 18
Page 88: Chapter 18

Fogs Caused by Evaporation When cool air moves over warm water,

enough moisture may evaporate from the water surface to produce saturation.

As the rising water vapor meets the cold air it immediately condenses and rises with the air.

This type of fog has a steamy appearance.

It is fairly common over lakes and rivers in the fall and spring.

Page 89: Chapter 18
Page 90: Chapter 18

How Precipitation Forms

Clouds are made of tiny water droplets perhaps 20 micrometers in diameter.

These tiny droplets drop very slowly. Most of the droplets would evaporate after falling only a few meters.

Precipitation forms when cloud droplets grow in volume at least one million times.

Page 91: Chapter 18
Page 92: Chapter 18

Cold Cloud Precipitation

The Bergeron Process relies on two physical processes, supercooling and saturation.

Cloud droplets do not freeze at 00C as one would expect.

Pure water suspended in air doesn’t freeze until it reaches a temperature of nearly -400C.

Page 93: Chapter 18

Bergeron Process

Page 94: Chapter 18

Super-cooled water

Water in the liquid state below 00C is called supercooled water.

Supercooled water will freeze when it contacts a solid object.

Page 95: Chapter 18

Freezing Nuclei

Freezing nuclei are materials that have crystal form.

Freezing nuclei can cause supercooled water to freeze.

Page 96: Chapter 18

Saturation Differences

When air is saturated (100% relative humidity) with respect to water, it is supersaturated with respect to ice (greater than 100% humidity).

Ice crystals cannot exist with water droplets in the air because the air is supersaturated.

Excess water vapor becomes ice, which lowers relative humidity.

Page 97: Chapter 18

Bergeron Process

Water droplets then evaporate to provide a continual source of water vapor for the growth of ice crystals.

Because the level of supersaturation with respect to ice can be quite high, the growth of ice crystals is rapid enough to produce crystals that are large enough to fall.

Page 98: Chapter 18

As they fall ice crystals contact cloud droplets causing them to freeze.

A chain reaction can occur and large crystals, called snowflakes form.

Page 99: Chapter 18
Page 100: Chapter 18
Page 101: Chapter 18

Snow

Each snow flake is different because of all the possible ways water molecules can freeze.

They are usually 6 sided.

It takes approx. 10 - 12 inches of snow to equal 1 inch of water.

Page 102: Chapter 18
Page 103: Chapter 18

Warm Cloud Precipitation

The mechanism that forms raindrops is the collision-coalescence process.

Some water-absorbing particles, such as salt, can remove water vapor from the air at relative humilities less than 100%, forming droplets that are quite large.

As these large droplets move through the cloud, they collide and coalesce (join) with smaller, slower droplets.

Page 104: Chapter 18

Forms of Precipitation

The type of precipitation that reaches the Earth’s surface depends on the temperature profile in the lowest few kilometers of the atmosphere.

Even on a hot summer day a large down pour may have started as snowstorm high the the clouds.

Page 105: Chapter 18

Rain and Snow

Rain – means drops of water that falls from a cloud and have a diameter of at least .5mm.

When the surface temperature is above 40C, snowflakes usually melt and continue to descend as rain.

Page 106: Chapter 18

Let it Snow

Snow – at very low temperatures (when the moisture content of the air is small) light, fluffy snow made up of individual six sided ice crystals forms.

Page 107: Chapter 18
Page 108: Chapter 18

Sleet, Glaze, and Hail

Sleet – is the fall of small particles of clear – to – translucent ice.

Sleet forms when a layer of above freezing air overlies a subfreezing layer near the ground.

Page 109: Chapter 18
Page 110: Chapter 18

Freezing Rain

Glaze – or freezing rain, results when raindrops become supercooled as they fall through subfreezing air near the ground and turns to ice when they impact objects.

Page 111: Chapter 18

Hail

Hail – is produced in cumulonimbus clouds. Hailstones begin as small ice pellets that grow by collecting supercooled water droplets as they fall through a cloud.

If the pellets encounter a strong updraft, they may be carried upward and begin to fall downward again.

Each trip upward causes more accumulation on the ice pellet much like the layers of an onion.

Page 112: Chapter 18

Hail

Page 113: Chapter 18
Page 114: Chapter 18