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Volumn 75, Issue 1, 2007, Pages 15-24

El Niño and the delayed action oscillator

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EID: 33846407247     PISSN: 00029505     EISSN: None     Source Type: Journal    
DOI: 10.1119/1.2358155     Document Type: Article
Times cited : (63)

References (28)
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    • A delayed action oscillator shared by biennial, interannual, and decadal signals in the Pacific Basin
    • Warren B. White, Yves M. Tourre, Mathew Barlow, and Mike Dettinger, "A delayed action oscillator shared by biennial, interannual, and decadal signals in the Pacific Basin," J. Geophys. Res. 108, 3070-3088 (2003).
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    • The measured sea-surface temperature is obtained as a monthly average of accumulated buoy data from the El Niño 3.4 region. The annual cycle (average) sea-surface temperature data represent the long term monthly average over all observed years. The sea-surface temperature anomaly is therefore the difference between average and measured sea-surface temperature
    • The measured sea-surface temperature is obtained as a monthly average of accumulated buoy data from the El Niño 3.4 region. The annual cycle (average) sea-surface temperature data represent the long term monthly average over all observed years. The sea-surface temperature anomaly is therefore the difference between average and measured sea-surface temperature.
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    • See EPAPS Document No. E-AJPIAS-74-002612 for the simulation software, accompanying notebook, and example runs. This document can be reached via a direct link in the online article's HTML reference section or via the EPAPS homepage (http://www.aip.org/pubservs/epaps.html).
    • See EPAPS Document No. E-AJPIAS-74-002612 for the simulation software, accompanying notebook, and example runs. This document can be reached via a direct link in the online article's HTML reference section or via the EPAPS homepage (http://www.aip.org/pubservs/epaps.html).
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    • We remark that a simple sinusoidal term will also suffice for most purposes
    • We remark that a simple sinusoidal term will also suffice for most purposes.
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  • 28
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    • If a single-fluid model of the ocean with depth H=4000 m had been assumed throughout, then c=√gH≈ 200 m/s. This Tsunami-like speed is clearly absurd for the purposes of this project, and hence the need for the more sophisticated two-fluid model.
    • If a single-fluid model of the ocean with depth H=4000 m had been assumed throughout, then c=√gH≈ 200 m/s. This Tsunami-like speed is clearly absurd for the purposes of this project, and hence the need for the more sophisticated two-fluid model.


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