Teleconnection

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Teleconnection in atmospheric science refers to climate anomalies being related to each other at large distances (typically thousands of kilometers). The most emblematic teleconnection is that linking sea-level pressure at Tahiti and Darwin, Australia, which defines the Southern Oscillation.

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[edit] History

Teleconnections were first noted by the British meteorologist Sir Gilbert Walker in the late nineteenth century, through computation of the correlation between time series of atmospheric pressure, temperature and rainfall. They served as a building block for the understanding of climate variability, by showing that the latter was not purely random.

Indeed, the term El Niño-Southern Oscillation (ENSO) is an implicit acknowledgment that the phenomenon underlies variability in several locations at once. It was later noticed that associated teleconnections occurred all over North America, as embodied by the Pacific-North American teleconnection pattern.

In the 1980's, improved observations allowed to detect teleconnections at larger distances throughout the troposphere.[1] Concomitantly, the theory emerged that such patterns could be understood through the dispersion of Rossby waves due to the spherical geometry of the Earth.[2] This is sometimes called the "proto-model"[3].

[edit] Theory

Teleconnections within the tropical Pacific began to be understood thanks to the idealized calculations of A.E. Gill[4] and later through more complex models.

Building upon the "proto-model", much of the early theory of teleconnections dealt with barotropic, linearized model of atmospheric flow about a constant mean state. However, the model was soon invalidated when it was discovered that actual teleconnection patterns were nearly insensitive to the location of the forcing, in direct contradiction with the predictions offered by this simple picture. Simmons and collaborators[5] showed that if a more realistic background state was prescribed, it would become unstable, leading to a similar pattern regardless of the location of the forcing, in accordance to observations. This "modal" property turned out to be an artifact of the barotropicity of the model, though it has appeared for more subtle reasons in more realistic models.

More recent work has shown that most teleconnections from the tropics to the extratropics can be understood to surprising accuracy by the propagation of linear, planetary waves upon a 3-dimensionall seasonally-varying basic state.[6]. Because the patterns are persistent over time and somewhat "locked" to geographical feature such as mountain ranges, these waves are called stationary.

There is another mechanism of teleconnection between tropical oceans and midlatitude regions, one that is symmetric along latitude circles (i.e. "zonal") and between hemispheres, contrary to the stationary wave mechanism. It relies on interactions between transient eddies and the mean atmospheric flow that are mutually reinforcing (i.e. non-linear). It has been shown to explain some aspects of ENSO teleconnections in temperature[7] and rainfall.[8]

[edit] Applications

Since tropical sea surface temperatures are predictable up to 2 years ahead of time,[9] knowledge of teleconnection patterns gives some amount of predictability in remote locations with an outlook sometimes as long as a few seasons.[10] For instance, predicting El Niño enables prediction of North American rainfall, snowfall, droughts or temperature patterns with a few weeks to months lead time. In Sir Gilbert Walker's time, A strong El Niño usually meant a weaker Indian monsoon, but this anticorrelation has weakened in the 1980's and 1990's, for controversial reasons.

[edit] Bibliography

- Teleconnections linking worldwide climate anomalies : scientific basis and societal impact, by Glantz, M.H , Richard W Katz; N Nicholls. Cambridge University Press, 1991. ISBN: 0521364752 9780521364751

- Progress during TOGA in understanding and modeling global teleconnections associated with tropical sea surface temperatures Trenberth, Kevin E; Branstator, Grant W; Karoly, David; Kumar, Arun; Ropelewski, Chester; Lau, Ngar-Cheung Journal of Geophysical Research. Vol. 103, no. C7, pp. 14, 291-14, 324. 29 June 1998

[edit] References

  1. ^ Wallace, J.M., and D.S. Gutzler, 1981: Teleconnections in the Geopotential Height Field during the Northern Hemisphere Winter. Mon. Wea. Rev., 109, 784–812.
  2. ^ Hoskins, B.J., and D.J. Karoly, 1981: The Steady Linear Response of a Spherical Atmosphere to Thermal and Orographic Forcing. J. Atmos. Sci., 38, 1179–1196.
  3. ^ Progress during TOGA in understanding and modeling global teleconnections associated with tropical sea surface temperatures Trenberth, Kevin E; Branstator, Grant W; Karoly, David; Kumar, Arun; Ropelewski, Chester; Lau, Ngar-Cheung Journal of Geophysical Research. Vol. 103, no. C7, pp. 14, 291-14, 324. 29 June 1998
  4. ^ Gill, A. E. : Some simple solutions for heat-induced tropical circulation, Quarterly Journal of the Royal Meteorological Society, . Vol. 106, pp. 447-462. July 1980
  5. ^ Simmons, A., J. Wallace, and G. Branstator, 1983: Barotropic Wave Propagation and Instability, and Atmospheric Teleconnection Patterns. J. Atmos. Sci., 40, 1363–1392.
  6. ^ Held, I.M., M. Ting, and H. Wang, 2002: Northern Winter Stationary Waves: Theory and Modeling. J. Climate, 15, 2125–2144.
  7. ^ Seager, R., N. Harnik, Y. Kushnir, W. Robinson, and J. Miller, 2003: Mechanisms of Hemispherically Symmetric Climate Variability. J. Climate, 16, 2960–2978.
  8. ^ Mechanisms of ENSO-forcing of hemispherically symmetric precipitation variability Seager, R; Harnik, N; Robinson, W A; Kushnir, Y; Ting, M; Huang, H P; Velez, J Quarterly Journal of the Royal Meteorological Society. Vol. 131, no. 608B, pp. 1501-1527. 2005
  9. ^ Chen D, Cane MA, Kaplan A, Zebiak SE, Huang D. : Predictability of El Niño over the past 148 years, Nature. 2004 Apr 15;428(6984):733-6
  10. ^ IRI Seasonal Climate Forecasts