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MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University
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MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Dec 16, 2015

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Page 1: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

MET 10 Lecture 7

Air Pressure and WindsChapter 6

Dr. Craig ClementsSan Jose State University

Page 2: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Hydrologic Cycle

Page 3: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Atmospheric PressureAtmospheric Pressure

Air pressure is simply the mass of air above a given level.

As we climb in elevation there are fewer air molecules above us; atmospheric pressure decreases with height.

What causes air pressure to change in the horizontal?

Why does air pressure change at the surface?

Page 4: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

A simplified model

Dots represent air molecules

We assume that:

1. Air molecules are not crowded close to the surface

2. Air density remains constant from surface to top of column.

3. Width of column does not change

4. Air is unable to freely move into or out of the column.

Page 5: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Two air columns, each identical mass, have same surface pressure.

Important concept:

Warm air aloft is normally associated with high atmospheric pressure, and cold air aloft is associated with low pressure.

Page 6: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Becoming more stableHorizontal difference in temperature creates a horizontal difference in pressure. The pressure difference establishes a force (called Pressure Gradient Force) that causes the air to move from higher pressure toward lower pressure.

Page 7: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Air above a region of surface high pressure is more dense than air above a region of surface low pressure (at the same temperature). (The dots in each column represent air molecules.)

Page 8: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

A barometer is an instrument that measures atmospheric pressure.

The mercury barometer.

The height of the mercury column is a measure of atmospheric pressure.

Page 9: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Sea-level pressure vs. station Sea-level pressure vs. station pressurepressureThe barometer reading at a particular location is called station pressure. This is the pressure that has been corrected for temperature, gravity, and instrument error.

Since pressure varies with altitude, the pressure at stations of different altitudes must be corrected in order to compare them. This adjusted pressure is called sea-level pressure.

Page 10: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

The top diagram (a) shows four cities (A, B, C, and D) at varying elevations above sea level, all with different station pressures.

The middle diagram (b) represents sea-level pressures of the four cities plotted on a sea-level chart.

The bottom diagram (c) shows isobars drawn on the chart (dark lines) at intervals of 4 millibars.

Page 11: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Surface and Upper-Air ChartsSurface and Upper-Air Charts

Isobaric maps: maps of constant pressure are constructed to show height variations along a constant pressure surface (isobaric surface).

Lines of constant pressure = isobars

Contour lines– lines that connect points of equal elevation above sea level.

Lines of low height = region of low pressure

Lines of high height = region of high pressure

Lines of constant temperature = isotherms

Page 12: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 13: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 14: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Surface and Upper-Air ChartsSurface and Upper-Air ChartsWhat does upper-air mean?

At what level do we consider upper-level?

Typically, we discuss surface pressures and upper-air. when we refer to upper-air levels we use pressure as our height coordinate.

For example, common levels we use:

850 mb = ~5,000 ft above sea level.700 mb = ~10,000 ft above sea level500 mb = ~16,000 ft above sea level (5000 m)300 mb = ~29,000 ft above sea level (9000 m)

The 300 mb level is the jet stream level.

Page 15: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Areas of low pressure (L) and high pressure (H) are shown.

Arrows indicate wind direction– the direction from which the wind is blowing.

Areas of high pressure are also called anti-cyclones.

Page 16: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

• When the height contours bend strongly to the south, (as in the diagram below), it is called a trough.

• Strong troughs are typically preceded by stormy weather and colder air at the surface.

Trough

• When the height contours bend strongly to the north, this is known as a Ridge.

• Strong ridges are accompanied by warm and dry weather conditions at the surface.

Ridge

Page 17: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Why the wind blowsWhy the wind blowsNewton’s Laws of Motion.

Newton’s first law of motion states that an object at rest will remain at rest and object in motion will remain in in motion as long as no force is exerted on the object.

Newton’s second law of motion states: that the force exerted on an object = its mass times the acceleration produced.

F= ma

To determine which direction the wind will blow we must identify and examine all the forces that affect the horizontal movement of air.

Page 18: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Why the wind blowsWhy the wind blows

To determine which direction the wind will blow we must identify and examine all the forces that affect the horizontal movement of air.

These forces include:

1. Pressure gradient force2. Coriolis force3. Centripetal force4. Friction

Page 19: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 20: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Pressure Gradient ForcePressure Gradient Force

When differences in horizontal air pressure exist there is a net force acting on the air. This force is the Pressure Gradient Force (PGF) and is directed from higher toward lower pressure at right angles to the isobars. The magnitude of the force is directly related to the pressure gradient. Steep pressure gradients correspond to strong forces.

Pressure Gradient is the change of pressure over a given distance:

Pressure Gradient = pressure difference / distance.

Closer the isobars = steeper the gradient = stronger force

Page 21: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

What is the PGF between P1 and P2?

4 mb per 100 km

Page 22: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 23: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 24: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Coriolis ForceCoriolis ForceIs an apparent force that is due to the rotation of the earth.

The Coriolis force causes the wind to deflect to the right of its intended path in the Northern Hemisphere and to the left of its path in the Southern Hemisphere.

The amount of deflection due to the Coriolis force depends upon:

1. The rotation of the earth2. The latitude3. The object’s speed

The Coriolis force acts at right angles to the wind, and only influences wind direction not speed.

Page 25: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.
Page 26: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Except at the equator, a free-moving object heading either east or west (or any other direction) will appear from the earth to deviate from its path as the earth rotates beneath it. The deviation (Coriolis force) is greatest at the poles and decreases to zero at the equator.

The Coriolis force “behaves” as a real force, constantly tending to “pull” the wind.

Page 27: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

When isobars are widely spaced, the flow is weak; when they are narrowly spaced, the flow is stronger. The increase in winds on the chart results in a stronger Coriolis force (CF ), which balances a larger pressure gradient force (PGF ).

Page 28: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Winds around Lows and Highs

Winds and related forces around areas of low and high pressure above the friction level in the Northern Hemisphere. Notice that the pressure gradient force (PGF ) is in red, while the Coriolis force (CF ) is in blue.

Page 29: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Curved Winds around Lows and Highs

A wind blowing at a constant speed, but parallel to curved isobars above the level of surface friction is termed: gradient wind.

A gradient wind blowing around a a low-pressure center is constantly accelerating because it is constantly changing direction. This acceleration is called centripetal acceleration.

Centripetal acceleration is directed at right angles to the wind, inward toward the low center.

The net force acting on the wind must be directed toward the center of the low in order for the air to keep moving in a counterclockwise, circular path.

This inward-directed force is called centripetal force: imbalance between Coriolis and PGF.

Page 30: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Winds around Lows and Highs

centripetal force

centripetal force: inward-directed force caused by an imbalance between the Coriolis force and PGF.

Page 31: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

An upper-level 500-mb map showing wind direction, indicated by lines that parallel the wind.

Page 32: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Winds on a surface weather map do not blow exactly parallel to the isobars; instead they cross the isobars moving higher to lower pressure.

The angle at which the wind crosses the isobars varies, but averages 30°.

The frictional drag of the ground slows the wind down.

Wind speeds increase with height above the ground due to lack of friction.

Surface Winds

Page 33: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

The effect of surface friction is to slow down the wind so that, near the ground, the wind crosses the isobars and blows toward lower pressure.

This phenomenon at the surface produces an outflow of air around a high. Aloft, the winds blow parallel to the lines, usually in a wavy west-to-east pattern.

Force of Surface Friction

Page 34: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Upper-level clouds moving from the southwest indicate isobars and winds aloft.

When extended horizontally, the upper-level chart appears as in (c), where lower pressure is to the northwest and higher pressure is to the southeast.

Estimating Wind Direction and Pressure Aloft by Watching Clouds

Page 35: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Winds in the Southern Hemisphere blow around Highs and Lows opposite in direction than in the Northern Hemisphere.

Page 36: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Winds and Vertical Air Motion

Page 37: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Hydrostatic Balance

Air does not rush off into space because the upward-directed pressure gradient force is nearly always exactly balanced by the downward force of gravity.

When these two forces are in exact balance, the air is said to be in hydrostatic equilibrium or balance.

When air is in hydrostatic balance, there is no net vertical force acting on it– no net vertical acceleration.

Page 38: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

An onshore wind blows from water to land.

An offshore wind blows from land to water.

A prevailing wind is the name given to wind direction most often observed during a given time period at a given location.

Determining WindsWind is characterized by its direction, speed, and gustiness.

Page 39: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

Wind direction can be expressed in degrees about a circle or as compass points.

Page 40: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

These trees standing unprotected from the wind are often sculpted into “flag” trees.

Page 41: MET 10 Lecture 7 Air Pressure and Winds Chapter 6 Dr. Craig Clements San Jose State University.

A wind farm near Tehachapi Pass, California, generates electricity that is sold to Southern California