atmospheric dynamics

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Atmospheric Dynamics The atmosphere is a fluid What are the properties of fluids? 1. Flow under the influence of forces Important forces for the atmosphere (and ocean): Gravity Friction Pressure gradient The so-called “fictitious forces”: Coriolis, Centrifugal 2. Generally considered continuous, although they are in fact composed of discrete atoms/molecules 3. Come in two general forms: Liquids Gases

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Atmospheric Dynamics. Flow under the influence of forces Important forces for the atmosphere (and ocean): Gravity Friction Pressure gradient The so-called “ fictitious forces ” : Coriolis, Centrifugal - PowerPoint PPT Presentation

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Page 1: Atmospheric Dynamics

Atmospheric DynamicsThe atmosphere is a fluid

What are the properties of fluids? 1. Flow under the influence of forces

Important forces for the atmosphere (and ocean):• Gravity• Friction• Pressure gradient• The so-called “fictitious forces”: Coriolis, Centrifugal

2. Generally considered continuous, although they are in fact composed of discrete atoms/molecules

3. Come in two general forms:• Liquids• Gases

Page 2: Atmospheric Dynamics

Forces and Motions

Gravity – “heavy” fluid sinks / “light” fluid risesExample: buoyancy, like in a lava lamp – “BLOOP… BLOOP…”

Friction – drag force acting on the fluid on account of its coming in contact with a rigid surface

Example: excess drag on one side of a spinning baseball causes a net force (in this case, on the ball) in that direction – “STRIKE ONE!”

Pressure Gradient – motion ensues from high-pressure to low-pressure under this force

Example: fill your hose, set it on the ground, step on one end: what happens? Under your foot is high pressure, at the open end the pressure is low – “SQUIRT!”

Page 3: Atmospheric Dynamics

Forces and Motions

FICTICIOUS FORCES

Centrifugal Force – if you wish to move in a circle, you must overcome your inertia, i.e. your tendency to move in straight lines unless you are acted on by a force

Example: sharp left turn in your car – “WHOA!”

Coriolis Force – motion relative to a rotating surface is apparently affected by this force

Example: rather like playing catch on a merry-go-round – “SMACK!”

Page 5: Atmospheric Dynamics

Forces and MotionsNewton’s Second Law:

In words, a net force acting on an object causes it to accelerate by an amount proportional to the sum of forces and inversely proportional to its mass. If the net force acting on an object is zero, the object will move in a straight line at constant speed (Newton’s First Law).

Page 6: Atmospheric Dynamics

Density, Pressure and Temperature

Density

Mass per unit volume

mks units: kg m-3 – “kilograms per cubic meter”cgs units: g cm-3 – “grams per cubic centimeter”

Page 7: Atmospheric Dynamics

Density, Pressure and Temperature

Pressure

Force per unit area

mks units: kg s-2 m-1 – Pa “Pascals”other units: bar, mb, atm, hPa

Page 8: Atmospheric Dynamics

Density, Pressure and Temperature

Temperature (and the Ideal Gas Law)

Temperature: Average kinetic energy of moleculesunits: Kelvins (K), degrees Celcius (oC)

: pressure exerted by vapor: volume occupied by vapor

: mass of vapor: specific gas constant of substance

: temperature of vapor (must be in K)

Page 9: Atmospheric Dynamics

Density, Pressure and TemperatureUse definition of density to formulate yet another version of the

Ideal Gas Law

: pressure exerted by the vapor: density of the vapor

: specific gas constant of the substance: temperature of the vapor

Page 10: Atmospheric Dynamics

BuoyancyArchimedes' principle

Vitruvius (De architectura IX.9–12) recounts the famous story of Archimedes making this discovery while in the bath. He was given the task of finding out if a goldsmith, who worked for the king, was carefully replacing the king's gold with silver. While doing this Archimedes decided he should take a break so went to take a bath. While entering the bath he noticed that when he placed his legs in, water spilled over the edge. Struck by a moment of realisation, he shouted "Eureka!" He informed the king that there was a way to positively tell if the smith was cheating him. Knowing that gold has a higher density than silver, he placed the king's crown and a gold crown of equal weight into a pool. Since the king's crown caused more water to overflow, it was, therefore, less dense, Archimedes concluded that it contained silver, causing the smith to be executed. The actual record of Archimedes' discoveries appears in his two-volume work, On Floating Bodies.

source: http://en.wikipedia.org/wiki/Buoyancy

Page 11: Atmospheric Dynamics

BuoyancyArchimedes' principle

Buoyancy Force = weight of the displaced fluid

Weight: force of gravity

Example Problem:The volume of a lake freighter hull is V = 300 m X 30 m X 20 m = 1.8 x 105 m3. If the density of lake water is 1000 kg m-3, what is the buoyancy force acting on the ship if it is nearly submerged (i.e. the water line is at the deck)? What is the cargo capacity, assuming the mass of the ship is negligible compared to the mass of the cargo it is carrying (this is probably a fairly bad assumption)?

Solution: The mass of displaced water is 1.8 x 108 kg and the weight of this water is then about 1.8 x 109 N. Thus, the buoyancy force acting on the ship will be about 2 billion Newtons. The cargo capacity would be somewhat less than 1.8 x 108 kg, depending on exactly how massive the empty ship itself is.

Page 12: Atmospheric Dynamics

How does buoyancy affect motion in fluids?

ambient fluidparcel

Will the parcel rise, fall or remain still?

Page 13: Atmospheric Dynamics

How does buoyancy affect motion in fluids?

Forces acting on the parcel:1. Gravity2. Buoyancy

Apply Newton’s Second Law:

Page 14: Atmospheric Dynamics

So, if the parcel is more dense than the ambient fluid ( ), it will sink. Examples: ocean convection/deep water formation

However, if the parcel is less dense than the environment ( ), it will rise.

Examples: hot air balloons, dirigibles, moist air in atmospheric convection

Page 15: Atmospheric Dynamics

How is buoyancy generated in the atmosphere?

There are two main ways that buoyancy (and therefore motion) is generated in the atmosphere:

1. Add/Subtract moisture, since H2O has a lower molecular weight than dry air composed of N2, O2 and Ar

2. Increase/Decrease temperature

(or a combination of the two, of course)

Page 16: Atmospheric Dynamics

Global Energy Budget (revisited)

Page 18: Atmospheric Dynamics

Atmospheric MotionThe Tropics: The Hadley Circulation

Page 19: Atmospheric Dynamics

Atmospheric MotionThe Tropics: Precipitation Patterns

Page 20: Atmospheric Dynamics

Atmospheric Motion

The Tropics: Precipitation Patterns(Seasonal Cycle in Soil Moisture)

http://geography.uoregon.edu/envchange/clim_animations/gifs/prate_web.gif

Page 21: Atmospheric Dynamics

Why do we have jet streams?Angular Momentum Conservation

angular momentum per unit mass

distance to rotation axis

east-west wind speed

Page 22: Atmospheric Dynamics

Figure Skater

Page 23: Atmospheric Dynamics

Atmosphere

Page 24: Atmospheric Dynamics

Atmospheric MotionThe Extra-tropics: The Jet Streams

Page 25: Atmospheric Dynamics

Atmospheric MotionThe Hadley Cell and Angular Momentum

Page 26: Atmospheric Dynamics

What is weather?

Midlatitude weather systems are instabilities of the zonal jet. A perfectly symmetric jet is unstable and begins to “meander”, producing mobile high and low pressure systems.

Weather is the response of the fluid atmosphere to a local imbalance in the energy budget.

Page 27: Atmospheric Dynamics

The meandering jet stream

Page 28: Atmospheric Dynamics

Jet Stream and Weather Systems

Page 29: Atmospheric Dynamics

What is weather?

Midlatitude weather systems are instabilities of the zonal jet. A perfectly symmetric jet is unstable and begins to “meander”, producing mobile high and low pressure systems.

Weather is the response of the fluid atmosphere to a local imbalance in the energy budget.

Page 30: Atmospheric Dynamics

The function of large-scale atmospheric motions, including

“weather” phenomena, is to transport thermal energy from

the equator to the poles, thereby balancing the GLOBAL

ENERGY BUDGET.

Page 31: Atmospheric Dynamics

Global Energy Budget (revisited)

Page 32: Atmospheric Dynamics

Global Energy Budget

Balanced global energy budget comprises radiative energy input and output as well as

1.Sensible heat transport (temperature)2.Latent heat transport (water vapor)

We just spent some time on the sensible heat budget; let’s look at water vapor transport…

Page 33: Atmospheric Dynamics

Moving warm air to the poles and cold air to the tropics…

Page 34: Atmospheric Dynamics

The Hydrological Cycle

Page 35: Atmospheric Dynamics

The Hydrological Cycle

Page 36: Atmospheric Dynamics

The Hydrological Cycle

Page 37: Atmospheric Dynamics

The Hydrological CycleHow in the world does evaporation and precipitation

constitute heat transport in the atmosphere?!?

1. dump some radiative energy into tropical ocean surface and evaporate water – the energy is not used to heat the ocean but to evaporate the water

2. move the newly evaporated water vapor toward the poles in atmospheric circulations

3. condense the water vapor in extra-tropical clouds/rain – energy released by condensation warms extra-tropical air

Net Result: Radiative energy deposited in the tropics has been used to warm extra-tropical air!

Page 38: Atmospheric Dynamics

Schematic of the General Circulation

Page 39: Atmospheric Dynamics

The General Circulationof the Atmosphere

Page 40: Atmospheric Dynamics

The General Circulationof the Atmosphere

Page 41: Atmospheric Dynamics

Some other climate animations…

http://geography.uoregon.edu/envchange/clim_animations/