Difference between revisions of "Coastal meteorology"

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Coastal mountains form a barrier to the wind field that may affect both the downstream and upstream evolution of the flow. The problem is characterized by two free parameters, the Froude number Fr, defined by U/(Nhm) and the Rossby number Ro, defined by U/(flm), where U is the speed of the air stream, hm is the height of the barrier, f is the Coriolis parameter, lm is the half width of the barrier, N is the Brunt-Vaisala frequency and is equal to (g/q0 dq/dz)0.5, g is gravity, and q0 is the mean potential temperature (the temperature of a parcel of air moved dry adiabatically to a pressure of 1000 mb). Generally blocking of the air flow occurs when Fr is < 1, which for a typical value of N of 10-1 s-1 can occur with elevations as low as 100 m. The influence of the earth's rotation on the deceleration of the upstream flow is considered through Ro. Deceleration is insignificant when Ro < 1. In steep topography it has been shown that the deceleration zone will grow upstream to a width defined by the Rossby radius of deformation lr, which is equal to Nhm/f. Steep topography is defined by the non-dimensional slope (hm/lm)(N/f), being greater than 1. This may also be written as Ro/Fr. In the coastal region the mountains often represent a wall such that lr is typically greater than lm, where Ro > 1, and the flow is not expected to be geostrophic (i.e., the flow will not remain perpendicular to the pressure gradient). The offshore influence of mountain coasts is given by the Rossby radius of deformation, which typically varies from 10 to 100 km.
 
Coastal mountains form a barrier to the wind field that may affect both the downstream and upstream evolution of the flow. The problem is characterized by two free parameters, the Froude number Fr, defined by U/(Nhm) and the Rossby number Ro, defined by U/(flm), where U is the speed of the air stream, hm is the height of the barrier, f is the Coriolis parameter, lm is the half width of the barrier, N is the Brunt-Vaisala frequency and is equal to (g/q0 dq/dz)0.5, g is gravity, and q0 is the mean potential temperature (the temperature of a parcel of air moved dry adiabatically to a pressure of 1000 mb). Generally blocking of the air flow occurs when Fr is < 1, which for a typical value of N of 10-1 s-1 can occur with elevations as low as 100 m. The influence of the earth's rotation on the deceleration of the upstream flow is considered through Ro. Deceleration is insignificant when Ro < 1. In steep topography it has been shown that the deceleration zone will grow upstream to a width defined by the Rossby radius of deformation lr, which is equal to Nhm/f. Steep topography is defined by the non-dimensional slope (hm/lm)(N/f), being greater than 1. This may also be written as Ro/Fr. In the coastal region the mountains often represent a wall such that lr is typically greater than lm, where Ro > 1, and the flow is not expected to be geostrophic (i.e., the flow will not remain perpendicular to the pressure gradient). The offshore influence of mountain coasts is given by the Rossby radius of deformation, which typically varies from 10 to 100 km.
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When uniform onshore flow, characterized by a low Froude number, encounters a coastal barrier the steady-state response is a pressure ridge, a phenomenon referred to as damming. The topographically induced pressure fields produce along-ridge pressure gradients that can result in barrier jets. The best examples of the phenomenon are found associated with cold air damming between a coastal front and mountain ridges. A similar structure can occur when the incident flow is not uniform, such as in the vicinity of a storm.
  
 
==Interactions with large scale meteorological systems==  
 
==Interactions with large scale meteorological systems==  

Revision as of 09:43, 21 December 2007

Category:Stub
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This article is still incomplete, since the author is still working on it. The section 'See also' already provides some interesting links. The section 'References' provides on overview of interesting literature on this topic.

Introduction

The coastal zone often experiences a unique weather which results into a very special climate. Coastal meteorology is the study of meteorological phenomena within about 100 km inland or offshore of a coastline. Improved understanding of the processes in the meteorology of the coastal zone is based on detailed knowledge of marine and terrestrial boundary layers and air-sea-interaction but has also to consider large-scale atmospheric dynamics and circulation of the coastal ocean. In addition to the importance of coastal meteorology to coastal weather forecast the subject helps in understanding the physical, chemical and biological aspects of the coastal ocean. Furthermore, the application of the knowledge is vital for the prediction of sea state and pollutant dispersal, and it is also important for public safety, ship routing and naval operations. The phenomena in coastal meteorology are caused, or significantly affected, by sharp changes in heat, moisture, and momentum transfer and changes in elevation, often a complex orography, that occur between land and water. Thermally driven effects like the land-sea breeze and orographically induced flows are the most prominent features in coastal meteorology, but also coastal cloud systems and fog, low level jets, coastal fronts and land-falling hurricanes, whose low-level flows are often modified as to favour the formation of tornadoes, are aspects of coastal weather phenomena. Complex terrain or coastlines and marine boundary layer stratus complicate the subject of coastal meteorology.

Structured coastline

Boundary Layer Processes, Air-Sea Interaction aspects

The Atmospheric boundary layer (ABL) is the lowest layer of the atmosphere which most directly is influenced (on time scales of an hour or less) by the presence of the ground. Turbulent motions dominate the flow in this region. Strong momentum, heat, water vapour, trace gas and particle transfer occurs at the air-land and air sea interface which is mainly driven by turbulent motions Garratt, 1995). The ABL is the region where life and human activities predominantly take place (Pal Arya 2001).

Chapter references:

Garratt, J.R., 1995: The Atmospheric Boundary Layer. Cambridge University Press, 334pp. Pal Arya, S., 2001: Introduction to Micrometeorology. Second Edition, Academic Press, San Diego, 415pp.

Thermally driven effects, the land-sea breeze

There is generally a large thermal contrast between the ocean and the land that drives the well-known sea-breeze circulation, which results in the confluence of air originating over the ocean with air originating over the land. The sea-breeze is associated with many processes that contribute to the recirculation and trapping of pollution, the evolution of precipitating convective storms, the creation of strong nearshore thermal, moisture and aerosol gradients, and the formation and transport of fog and low cloud in the coastal zone.

Mechanically induced flows

Orographic Influences

Coastal mountains form a barrier to the wind field that may affect both the downstream and upstream evolution of the flow. The problem is characterized by two free parameters, the Froude number Fr, defined by U/(Nhm) and the Rossby number Ro, defined by U/(flm), where U is the speed of the air stream, hm is the height of the barrier, f is the Coriolis parameter, lm is the half width of the barrier, N is the Brunt-Vaisala frequency and is equal to (g/q0 dq/dz)0.5, g is gravity, and q0 is the mean potential temperature (the temperature of a parcel of air moved dry adiabatically to a pressure of 1000 mb). Generally blocking of the air flow occurs when Fr is < 1, which for a typical value of N of 10-1 s-1 can occur with elevations as low as 100 m. The influence of the earth's rotation on the deceleration of the upstream flow is considered through Ro. Deceleration is insignificant when Ro < 1. In steep topography it has been shown that the deceleration zone will grow upstream to a width defined by the Rossby radius of deformation lr, which is equal to Nhm/f. Steep topography is defined by the non-dimensional slope (hm/lm)(N/f), being greater than 1. This may also be written as Ro/Fr. In the coastal region the mountains often represent a wall such that lr is typically greater than lm, where Ro > 1, and the flow is not expected to be geostrophic (i.e., the flow will not remain perpendicular to the pressure gradient). The offshore influence of mountain coasts is given by the Rossby radius of deformation, which typically varies from 10 to 100 km. When uniform onshore flow, characterized by a low Froude number, encounters a coastal barrier the steady-state response is a pressure ridge, a phenomenon referred to as damming. The topographically induced pressure fields produce along-ridge pressure gradients that can result in barrier jets. The best examples of the phenomenon are found associated with cold air damming between a coastal front and mountain ridges. A similar structure can occur when the incident flow is not uniform, such as in the vicinity of a storm.

Interactions with large scale meteorological systems

Meteorological measurements in the coastal environment

See also

Internal links

Other articles about weather and climate:

External links

References

Geernaert, G.L. (ed.), 1999: Air-Sea Exchange: Physics, Chemistry and Dynamics. Kluwer Academic Publishers, Dordrecht, 578pp.

Hsu, S.A., 1988: Coastal meteorology. Academic Press Inc., San Diego, 260pp. Kraus, E.B. and J. A. Businger, 1994: Atmosphere-Ocean Interaction. Oxford University Press, 362 pp.

Nuss, W.A., J.M. Bane, W.T. Thompson, T. Holt, C.E. Dorman, F.M. Ralph, R. Rotunno, J.B. Klemp, W.C. Skamarock, R.M. Samelson, A.M. Rodgerson, C. Reason, and P. Jackson, 2000: Coastally trapped wind reversals: Progress toward understanding. Bull. Amer. Meteoro. Soc., 81, 719-743.

Nuss, W., 2002: Coastal Meteorology. In M. Shankar (ed.) Enzyclopedia of Atmospheric Science, Elsevier, in Press.

Rogers, D.P., 1995: Coastal meteorology. U.S. National Report to IUGG 1991-1994, American Geophysical Union Rev. Geophys. Vol. 33 Suppl.

Rogers, D., C. Dorman, K. Edwards, I. Brooks, S. Burk, W. Thompson, T. Holt, L. Strom, M. Tjernström, B. Grisogono, J. Bane, W. Nuss, B. Morely and A. Schanot, 1998.: Highlights of Coastal Waves 1996. Bull. Amer. Meteoro. Soc., 79, 1307-1326.

Rotunno, R., J. A. Curry, C. W. Fairall, C. A. Friehe, W. A. Lyons, J. E. Overland, R. A. Pielke, D. P. Rogers, S. A. Stage, 1992: Coastal Meteorology, A review of the state of the science, National Academy Press, Washington, D. C., 99 pp.

Simpson, J.E., 1994: Sea Breeze and Local Winds. Cambridge University Press.

The main author of this article is Markus Quante
Please note that others may also have edited the contents of this article.

Citation: Markus Quante (2007): Coastal meteorology. Available from http://www.coastalwiki.org/wiki/Coastal_meteorology [accessed on 24-11-2024]