NATS 101

Lecture 14
Air Pressure

What is Air Pressure?
Pressure = Force/Area
What is a Force?          ItŐs like a push/shove
In an air filled container, pressure is due to molecules pushing the sides outward by recoiling off them

Air Pressure
Concept applies to       an Ňair parcelÓ surrounded by     more air parcels,    but molecules create pressure through rebounding off air molecules in other neighboring parcels

Air Pressure
At any point, pressure  is the same in all directions
But pressure can vary from one point to another point

"Higher density"
Higher density                        at the same temperature creates higher pressure by more collisions among molecules of average same speed

Ideal Gas Law
Relation between pressure, temperature and density is quantified by the Ideal Gas Law
P(mb) = constant « r(kg/m3) « T(K)
Where P is pressure in millibars
Where r is density in kilograms/(meter)3
Where T is temperature in Kelvin

Ideal Gas Law
Ideal Gas Law is complex
P(mb) = constant « r(kg/m3) « T(K)
P(mb) = 2.87 « r(kg/m3) « T(K)
If you change one variable, the other two will change. It is easiest to understand the concept if one variable is held constant while varying the other two

Ideal Gas Law
P = constant « r « T (constant)
With T constant, Ideal Gas Law reduces to
F P varies with r E
Denser air has a higher pressure than less dense air at the same temperature
Why? You give the physical reason!

Ideal Gas Law
P = constant « r (constant) « T
With r constant, Ideal Gas Law reduces to
F P varies with T E
Warmer air has a higher pressure than colder air at the same density
Why? You answer the underlying physics!

Ideal Gas Law
P (constant) = constant « r « T
With P constant, Ideal Gas Law reduces to
F T varies with 1/r E
Colder air is more dense (r big, 1/r small) than warmer air at the same pressure
Why? Again, you reason the mechanism!

Summary
Ideal Gas Law Relates
Temperature-Density-Pressure

Pressure-Temperature-Density
Pressure
Decreases with height at same rate in air of same temperature
Isobaric Surfaces
Slopes are horizontal

Pressure-Temperature-Density
Pressure (vertical scale highly distorted)
Decreases more rapidly with height in cold air than in warm air
Isobaric surfaces will slope downward toward cold air
Slope increases with height to tropopause, near 300 mb in winter

Pressure-Temperature-Density
Summary
Ideal Gas Law Implies
Pressure decreases more rapidly with height in cold air than in warm air.
ConsequentlyÉ..
Horizontal temperature differences lead to horizontal pressure differences!
And horizontal pressure differences lead       to air motionÉor the wind!

Review: Pressure-Height
Remember
Pressure falls very rapidly with height near sea-level
3,000 m 701 mb
2,500 m 747 mb
2,000 m 795 mb
1,500 m 846 mb
1,000 m 899 mb
500 m 955 mb
0 m 1013 mb
    1 mb per 10 m height

Station Pressure
Reduction to Sea-Level-Pressure
Correction for Tucson
Elevation of Tucson AZ is ~800 m
Station pressure at Tucson runs ~930 mb
So SLP for Tucson would be
SLP = 930 mb + (1 mb / 10 m) « 800 m
SLP = 930 mb + 80 mb = 1010 mb

Correction for Denver
Elevation of Denver CO is ~1600 m
Station pressure at Denver runs ~850 mb
So SLP for Denver would be
SLP = 850 mb + (1 mb / 10 m) « 1600 m
SLP = 850 mb + 160 mb = 1010 mb
Actual pressure corrections take into account temperature and pressure-height variations, but 1 mb / 10 m is a good approximation

You Try at Home for Phoenix
Elevation of Phoenix AZ is ~340 m
Assume the station pressure at Phoenix was ~977 mb at 3pm yesterday
So SLP for Phoenix would be?

Sea Level Pressure Values
Summary
Because horizontal pressure differences are the force that drives the wind
Station pressures are adjusted to one standard levelÉMean Sea LevelÉto remove the dominating impact of different elevations on pressure change

Slide 24
Key Points for Today
Air Pressure
Force / Area (Recorded with Barometer)
Ideal Gas Law
Relates Temperature, Density and Pressure
Pressure Changes with Height
Decreases more rapidly in cold air than warm
Station Pressure
Reduced to Sea Level Pressure

Assignment
Reading - Ahrens pg 148-149
include Focus on Special Topic: Isobaric Maps
Problems - 6.9, 6.10