A Crash Course in Cyclogenesis

Cyclogenesis is the development and strengthening of surface low pressure areas in the middle latitudes of the globe. These surface low pressure systems are sometimes referred to as cyclones, where a cyclone is defined as a near circular air flow that is in the same direction as the rotating Earth, which is counterclockwise in the northern hemisphere and clockwise in the southern hemisphere. In the northern hemisphere, winds around low pressure centers blow counterclockwise and spiral inward. This inward flow at the surface (convergence) forces rising motion in the vicinity of cyclones. Clouds and precipitation form where air rises. Because cyclones often produce precipitation, they are sometimes just referred to as "storms".

Typical mid-latitude winter weather system. Black lines represent the 500 mb height pattern. The positions of longwave troughs and ridges is shown in red. Green lines denote the position of a surface cyclone or low pressure area.

An air mass is a large area of air (typically thousands of square km) with nearly uniform properties of temperature and humidity. Air masses form when air remains stagnent or sits over a region for a few days or longer. These regions are dominated by persistent high pressure at the surface and light winds. After a few days, the air mass takes on the properties of the underlying surface. Concerning winter weather for the United States, cold air masses often develop over northern Canada or the northern Pacific Ocean, while warm air masses often develop over the Gulf of Mexico or the tropical Pacific Ocean.

Once air masses form, they may be put into motion by the large scale weather pattern. A 500 mb height map is a good way to view the large scale weather pattern. Cold air masses are often pushed southward where the 500 mb winds are from the north, while warm air masses are often pushed northward where the 500 mb winds are from the south. On surface weather maps, a weather front is simply the boundary between two different air masses. Where a cold air mass is invading an area currently covered by a warmer air mass, a cold front is indicated on a surface weather map. Conversely where a warm air mass is invading an area currently covered by a colder air mass, a warm front is indicated on a surface weather map. If neither the cold nor warm air is advancing, the frontal zone is marked by a stationary front. Weather fronts are marked on surface weather maps. Fronts often produce "weather" in the form of clouds and precipitation because air is forced to rise upward along the front. All fronts slope in the vertical so that the warmer (less dense) air mass sits on top of the colder (more dense) air mass. In other words, the warmer air mass is forced to rise over the colder air mass. Thus, the location of weather fronts on surface maps are important to see the boundary between and warm and cold air as well a region where air is forced to rise upward, which is necessary for clouds and precipitation to form.

In general, a rather narrow transition zone develops between two large bodies of air (air masses), which is called the frontal zone. Ideally, the polar frontal zone circles the northern hemisphere, marking a boundary between cold arctic air to the north and warmer subtropical air to the south. The shape of the idealized polar front would basically follow the wavy pattern of the 500 mb troughs and ridges. Cyclogenesis most often occurs along this polar front, especially underneath areas located just downstream of 500 mb troughs because in these areas upper tropospheric divergence is occurring (see polar front, cyclogenesis picture). In the picture, black lines show the 500 mb height pattern, while the green lines indicate the favored position for a strengthening surface low pressure area.

Polar Jet Stream

The polar jet stream a very fast moving current of air located near the top of the troposphere where air pressure is about 250 mb and the altitude is close 10 km. The polar jet stream occurs above the polar front. Energetically, the polar jet stream can be explained by the large pressure gradient (rapid change of the height of the 250 mb pressure surface over a short horizontal distance) that occurs above the polar front (see link provided in the next paragraph). The name jet stream was coined because high-flying military pilots encountered them during World War II. The polar jet stream generally flows from west to east, but follows a wavy path with troughs and ridges, just like the 500 mb flow. Today, commercial jets fly at altitudes near the jet stream. This is why flights from west to east are generally faster than flights from east to west. There is also a subtropical jet stream, which you may have heard mentioned in weather discussions, but we will not be able to cover that in this class.

Please take a look at A pictorial discussion of the polar jet stream. You should be able to explain why the polar jet stream is found above the polar front and why the wind speed above the polar front increases with increasing altitude such that the strongest winds (jet streams) are found near the top of the troposphere. Based on the discussion and figure above, you should be able to understand why a mid-latitude frontal zone produces a vertical wind shear pattern where wind speed increases with increasing altitude. Such a wind shear pattern can aid in the development of severe thunderstorms (assuming conditions are otherwise favorable for the development of thunderstorms).

Map of forecast jet stream level winds from the Weather Channel. On the map, arrows indicate the wind direction and the color shading indicates the wind speed. The actual jet stream typically shows up as a narrow band of strong winds that gets concentrated above the polar front.

The position of the polar front (or warm/cold boundary) is not fixed but moves south and north within the middle latitudes in the winter. We have already seen evidence for this in the 500 mb height patterns. In 500 mb troughs, the polar front moves south as cold air masses plunge southward and in 500 mb ridges, the polar front moves northward as warm air masses push northward.

Due to time constraints we will not cover the remainder of this page this semester. Please feel free to read the remainder of the page if you are interested.

In addition within the 500 mb pattern, rising motion and precipitation is most likely just downwind of 500 mb troughs. In order for everything to work together and be consistent, it should make sense to you that surface low pressure (associated with rising motion) will be found underneath regions just downstream of 500 mb troughs. An idealized picture is shown below.

Typical mid-latitude winter weather system. Green wavy lines represent the 500 mb height pattern. The red circles represent the pattern of sea level isobars around a surface low and high pressure. Notice how the surface circulation brings cold air southward (under the 500 mb trough) and warm air northward under the 500 mb ridge. In this way middle latitude circulations transport energy from the equator toward the poles.

Below is a series of three links to lecture notes that I used in a previous class. It shows an idealized representation of the lifecycle of a middle latitude surface cyclone from birth to death. The last page shows the energetics involved. Weather fronts are sloped in the vertical so that warm air is always lifted above colder air. This should help you to understand the precipitation patterns shown in the links below. Don't be concerned about the occluded front, just realize that it also forces lifing of air.

Finally, we need to put this all together to get a 3-D picture of what occurs during cyclogenesis. As mentioned above, developing surface low pressure areas, which are characterized by surface convergence and rising motion, will tend to form underneath where the upper level wind patterns (500 mb and above) are also favorable for rising motion, i.e., just downstream of upper level troughs where upper level divergence occurs.
Relationship between rising motion, surface convergene, and upper level divergence

You should now realize the following:

• If upper level divergence > surface convergence, surface low strengthens (pressure lowers)
• If upper level divergence = surface convergence, surface low remains steady
• If upper level divergence < surface convergence, surface low weakens (pressure rises)

My best attempt at drawing a 3-D representation of a mid-latitude winter weather pattern is given below.