Cyclogenesis is the development or strengthening ofcyclonic circulation in the atmosphere (alow-pressure area).[1] Cyclogenesis is anumbrella term for at least three different processes, all of which result in the development of some sort ofcyclone, and at any size from themicroscale to thesynoptic scale.
The process in which an extratropical cyclone undergoes a rapid drop in atmospheric pressure (24 millibars or more) in a 24-hour period is referred to asexplosive cyclogenesis, and is usually present during the formation of anor'easter.[2] Similarly, a tropical cyclone can undergorapid intensification.
The anticyclonic equivalent, the process of formation ofhigh-pressure areas, isanticyclogenesis.[3] The opposite of cyclogenesis iscyclolysis.
There are four main scales, or sizes of systems, dealt with in meteorology: the macroscale, the synoptic scale, themesoscale, and the microscale.[4] The macroscale deals with systems with global size, such as theMadden–Julian oscillation. Synoptic scale systems cover a portion of a continent, such asextratropical cyclones, with dimensions of 1,000–2,500 km (620–1,550 mi) across.[5] The mesoscale is the next smaller scale, and often is divided into two ranges: meso-alpha phenomena range from 200–2,000 km (120–1,240 mi) across (the realm of thetropical cyclone), while meso-beta phenomena range from 20–200 km (12–124 mi) across (the scale of themesocyclone). The microscale is the smallest of the meteorological scales, with a size under two kilometers (1.2 miles) (the scale oftornadoes andwaterspouts).[6] These horizontal dimensions are not rigid divisions but instead reflect typical sizes of phenomena having certain dynamic characteristics. For example, a system does not necessarily transition from meso-alpha to synoptic scale when its horizontal extent grows from 2,000 to 2,001 km (1,242.7 to 1,243.4 mi).
TheNorwegian cyclone model is an idealized formation model ofcold-core cyclonic storms developed by Norwegian meteorologists during theFirst World War.[7] The main concept behind this model, relating to cyclogenesis, is that cyclones progress through a predictable evolution as they move up a frontal boundary, with the most mature cyclone near the northeast end of the front and the least mature near the tail end of the front.[8]
A preexisting frontal boundary, as defined insurface weather analysis, is required for the development of a mid-latitude cyclone. The cyclonic flow begins around a disturbed section of the stationary front due to an upper level disturbance, such as ashort wave or an upper-level trough,[9][10] near a favorable quadrant of the upper-level jet.[11] However, enhanced along-frontal stretching rates in the lower troposphere can suppress the growth of extratropical cyclones.[12][13]
Cyclogenesis can only occur when temperature decreases polewards (to the north, in the northern hemisphere), and pressure perturbation lines tilt westward with height. Cyclogenesis is most likely to occur in regions of cyclonic vorticityadvection, downstream of a strong westerly jet.[14] The combination of vorticity advection and thermal advection created by the temperature gradient and a low pressure center cause upward motion around the low.[a]If the temperature gradient is strong enough, temperature advection will increase, driving more vertical motion. This increases the overall strength of the system. Shearwise updrafts[b] are the most important factor in determining cyclonic growth and strength.[16]
A surface low can have a variety of causes for forming. Topography can force a surface low to form when an existingbaroclinic wave moves over a mountain barrier; this is known as "lee cyclogenesis" since the low forms on theleeward side of the mountains.[17][18]Mesoscale convective systems can spawn surface lows which are initially warm core.[19] The disturbance can grow into a wave-like formation along thefront and the low will be positioned at the crest. Around the low, flow will become cyclonic, by definition. This rotational flow will push polar air equator-ward west of the low via its trailing cold front, and warmer air will push poleward low via the warm front. Usually the cold front will move at a quicker pace than the warm front and "catch up" with it due to the slow erosion of higher density airmass located out ahead of the cyclone and the higher density airmass sweeping in behind the cyclone, usually resulting in a narrowing warm sector.[20] At this point anoccluded front forms where the warm air mass is pushed upwards into a trough of warm air aloft, which is also known as atrowal (atrough ofwarm airaloft).[21] All developing low-pressure areas share one important aspect, that of upward vertical motion within the troposphere. Such upward motions decrease the mass of local atmospheric columns of air, which lower surface pressure.[22]
Maturity is after the time of occlusion when the storm has completed strengthening and the cyclonic flow is at its most intense.[23] Thereafter, the strength of the storm diminishes as the cyclone couples with the upper-level trough or upper-level low, becoming increasingly cold core. The spin-down of cyclones, also known as cyclolysis, can be understood from an energetics perspective. As occlusion occurs and the warm air mass is pushed upwards over a cold air airmass, the atmosphere becomes increasingly stable and the centre of gravity of the system lowers.[24] As the occlusion process extends further down the warm front and away from the central low, more and more of the available potential energy of the system is exhausted. This potential energy sink creates a kinetic energy source which injects a final burst of energy into the storm's motions. After this process occurs, the growth period of the cyclone, or cyclogenesis, ends, and the low begins to spin down (fill) as more air is converging into the bottom of the cyclone than is being removed out the top since upper-level divergence has decreased.
Occasionally, cyclogenesis will re-occur with occluded cyclones. When this happens a new low center will form on the triple-point (the point where the cold front, warm front, and occluded front meet). During triple-point cyclogenesis, the occluded parent low will fill as the secondary low deepens into the main weathermaker.
Tropical cyclones exist within a mesoscale alpha domain. As opposed to mid-latitude cyclogenesis, tropical cyclogenesis is driven by strong convection organised into a central core with nobaroclinic zones, or fronts, extending through their center. Although the formation oftropical cyclones is the topic of extensive ongoing research and is still not fully understood, there are six main requirements for tropical cyclogenesis:sea surface temperatures that are warm enough, atmospheric instability, highhumidity in lower to middle levels of thetroposphere, enoughCoriolis force to develop a low pressure center, a pre-existing low level focus or disturbance, and low verticalwind shear. These warm core cyclones tend to form over the oceans between 10 and 30 degrees of the equator.[25][26]
Mesocyclones range in size from mesoscale beta to microscale. The term mesocyclone is usually reserved for mid-level rotations within severe thunderstorms,[27] and are warm core cyclones driven by latent heat of its associated thunderstorm activity.
Tornadoes form in the warm sector ofextratropical cyclones where a strong upper-level jet stream exists.[28] Mesocyclones are believed to form when strong changes of wind speed and/or direction with height ("wind shear") sets parts of the lower part of the atmosphere spinning in invisible tube-like rolls. The convective updraft of a thunderstorm is then thought to draw up this spinning air, tilting the rolls' orientation upward (from parallel to the ground to perpendicular) and causing the entire updraft to rotate as a vertical column.
As the updraft rotates, it may form what is known as a wall cloud. The wall cloud is a spinning layer of clouds descending from the mesocyclone. The wall cloud tends to form closer to the center of the mesocyclone. The wall clouds do not necessarily need a mesocyclone to form and do not always rotate. As the wall cloud descends, a funnel-shaped cloud may form at its center. This is the first stage of tornado formation.[29] The presence of a mesocyclone is believed to be a key factor in the formation of the strong tornadoes associated with severe thunderstorms.
Tornadoes exist on the microscale or low end of the mesoscale gamma domain. The cycle begins when a strong thunderstorm develops a rotating mesocyclone a few miles up in the atmosphere, becoming a supercell. As rainfall in the storm increases, it drags with it an area of quickly descending air known as therear flank downdraft (RFD). This downdraft accelerates as it approaches the ground, and drags the rotating mesocyclone towards the ground with it.[30]
As the mesocyclone approaches the ground, a visible condensation funnel appears to descend from the base of the storm, often from a rotating wall cloud. As the funnel descends, the RFD also reaches the ground, creating a gust front that can cause damage a good distance from the tornado. Usually, the funnel cloud begins causing damage on the ground (becoming a tornado) within minutes of the RFD reaching the ground.[31]
Waterspouts exist on the microscale. While some waterspouts are strong (tornadic) like their land-based counterparts, most are much weaker and caused by different atmospheric dynamics. They normally develop in moisture-laden environments with little verticalwind shear along lines of convergence, such asland breezes, lines of frictional convergence from nearby landmasses, or surface troughs.[32] Their parent cloud can be as innocuous as a moderate cumulus, or as significant as athunderstorm. Waterspouts normally develop as their parent clouds are in the process of development, and it is theorized that they spin up as they move up the surface boundary from the horizontalwind shear near the surface, and then stretch upwards to the cloud once the low level shear vortex aligns with a developing cumulus or thunderstorm. Weak tornadoes, known as landspouts, across eastern Colorado have been witnessed to develop in a similar manner.[33] An outbreak occurred in theGreat Lakes in late September and early October 2003 along a lake effect band. September is the peak month of landspout and waterspout occurrence aroundFlorida and for waterspout occurrence around theGreat Lakes.[33][34]
Cyclogenesis is the opposite of cyclolysis, which concerns the weakening of surface cyclones. The term has an anticyclonic (high-pressure system) equivalent—Anticyclogenesis, which deals with the formation of surface high-pressure systems.[3]
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