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NATS 101 Lecture 11 Air Pressure. http://en.wikipedia.org/wiki/Atmospheric_pressure. Plastic bottle sealed at 14,000’; crushed at 1,000’. What is Air Pressure?. Pressure = Force/Area What is a Force? It’s like a push/shove
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NATS 101Lecture 11Air Pressure http://en.wikipedia.org/wiki/Atmospheric_pressure Plastic bottle sealed at 14,000’; crushed at 1,000’.
What is Air Pressure? Pressure = Force/Area What is a Force? It’s like a push/shove In an air filled container, pressure is due to molecules pushing the sides outward by recoiling off them Recoil Force
Recoil Force Air Pressure Concept applies to an “air parcel” surrounded by more air parcels, but molecules create pressure through rebounding off air molecules in other neighboring parcels
Recoil Force Air Pressure At any point, pressure is the same in all directions But pressure can vary from one point to another point
Higher density at the same temperature creates higher pressure by more collisions among molecules of average same speed Higher temperatures at the same density creates higher pressure by collisions between faster moving molecules
Ideal Gas Law • Relation between pressure, temperature and density is quantified by the Ideal Gas Law P(mb)=Const(mb m3/kg/K) d(kg/m3) T(K) • Where P is pressure in millibars (mb) • Where d is density in kilograms/meter3 (kg/m3) • Where T is temperature in Kelvin (K) • Where Const=2.87 is a constant (mb m3/kg/K)(Parenthetical expressions are units)
Ideal Gas Law • Ideal Gas Law is complex P(mb) = Const d(kg/m3) T(K) P(mb) = 2.87 mb m3/kg/K d(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 d T (constant) With T constant, Ideal Gas Law reduces to P varies with d Boyle's Law Denser air has a higher pressure than less dense air at the same temperature Why? You give the physical reason at home.
Ideal Gas Law P = constant d (constant) T With d constant, Ideal Gas Law reduces to P varies with T Guy Lussac’s Law 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 d T With P constant, Ideal Gas Law reduces to T varies with 1/d Charles Law Colder air is more dense (d big, 1/d small) than warmer air at the same pressure Why? Again, you reason the mechanism.
Summary • Ideal Gas Law Relates Temperature-Density-Pressure Fundamental Relationship that governs the state of air in our atmosphere
Pressure-Temperature-Density Pressure Decreases with height at same rate in air of same temperature Constant Pressure (Isobaric) Surfaces Slopes are horizontal 300 mb 400 mb 500 mb 9.0 km 9.0 km 600 mb 700 mb 800 mb 900 mb 1000 mb Minneapolis Houston
Pressure-Temperature-Density WARM 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 300 mb COLD 400 mb 500 mb 9.5 km 600 mb 8.5 km 700 mb 800 mb 900 mb 1000 mb Minneapolis Houston
Pressure-Temperature-Density WARM Pressure Higher along horizontal red line in warm air than in cold air Pressure difference is a non-zero force Pressure Gradient Force or PGF (red arrow) Air will accelerate from column 2 towards 1 Pressure falls at bottom of column 2, rises at 1 Animation 300 mb COLD 400 mb 500 mb H L PGF 9.5 km 600 mb 8.5 km 700 mb 800 mb 900 mb 1000 mb H L PGF Minneapolis Houston SFC pressure rises SFC pressure falls
Summary • Ideal Gas Law Implies Pressure decreases more rapidly with height in cold air than in warm air. • Consequently….. Horizontal temperature differences lead to horizontal pressure differences! And horizontal pressure differences lead to air motion…or the wind!
N. Pacific Pressure Analysis (isobars every 4 mb) 2000 km Pressure varies by 1 mb per 100 km horizontally or 0.0001 mb per 10 m
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 Consequently……….Vertical pressure changes from differences in station elevation dominate horizontal changes
Station Pressure Ahrens, Fig. 6.7 Pressure is recorded at stations with different altitudes Station pressure differences mostly reflect height differences Wind is forced by horizontal pressure differences Since true horizontal pressure changes are 1 mb per 100 km We adjust station pressures to one standard horizontal level: Mean Sea Level
Reduction to Sea-Level-Pressure Ahrens, Fig. 6.7 Station pressures are adjusted toSea Level PressureMake altitude correction of 1 mb per 10 m elevation
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
Local Example to Try at Home The station pressure at PHX is ~977 mb. The station pressure at TUS is ~932 mb. Which station has the higher SLP?
Sea Level Pressure Values 882 mb (26.04 in.) Wilma (October, 2005) Ahrens, Fig. 6.3
Summary • Because horizontal pressure differences are the force that drives the wind Station pressures are adjusted to one standard level…Mean Sea Level…to remove the dominating impact of different elevations on pressure change
PGF Ahrens, Fig. 6.7
Key Points • 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 Mean-Sea-Level to Mitigate the Dominate Impact of Altitude on Pressure Change
Surface Maps • Pressure reduced to Mean Sea Level is plotted and analyzed for surface maps. Estimated from station pressures • Actual surface observations for other weather elements (e.g. temperatures, dew points, winds, etc.) are plotted on surface maps. • NCEP/HPC Daily Weather Map
Next Lecture AssignmentNewton’s Laws, Upper-Air Maps • Reading -Ahrens 3rd: 146-155 4th: 148-157 5th: 148-156 • Problems -D2L (Due Wednesday Mar 3) 3rd-Pg 162: 6.09, 10, 12, 13, 17, 19, 22 4th-Pg 164: 6.09, 10, 12, 13, 17, 19, 22 5th-Pg 165: 6.10, 11, 13, 14, 18, 20, 23