Articles | Volume 32, issue 2
https://doi.org/10.5194/npg-32-201-2025
© Author(s) 2025. This work is distributed under the Creative Commons Attribution 4.0 License.
Explaining the high skill of reservoir computing methods in El Niño prediction
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- Final revised paper (published on 01 Jul 2025)
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CC1: 'Comment on npg-2024-24', Paul Pukite, 23 Nov 2024
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RC1: 'Comment on npg-2024-24', Anonymous Referee #1, 18 Dec 2024
- AC1: 'Reply on RC1', Francesco Guardamagna, 09 Feb 2025
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RC2: 'Comment on npg-2024-24', Anonymous Referee #2, 04 Jan 2025
- AC2: 'Reply on RC2', Francesco Guardamagna, 09 Feb 2025
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RC4: 'Comment on npg-2024-24', Anonymous Referee #3, 06 Jan 2025
- AC3: 'Reply on RC4', Francesco Guardamagna, 09 Feb 2025
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AR by Francesco Guardamagna on behalf of the Authors (12 Mar 2025)
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ED: Referee Nomination & Report Request started (13 Mar 2025) by Wansuo Duan
RR by Anonymous Referee #1 (24 Mar 2025)
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ED: Publish subject to minor revisions (review by editor) (02 Apr 2025) by Wansuo Duan
AR by Francesco Guardamagna on behalf of the Authors (04 Apr 2025)
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ED: Publish as is (06 Apr 2025) by Wansuo Duan
AR by Francesco Guardamagna on behalf of the Authors (09 Apr 2025)
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Because of the importance of the thermocline in ENSO behavior, the impact of long-period tides in a reduced effective gravity environment has to be included in any predictive analysis. This is particularly appropriate for machine learning, where known tidal data can be straightforwardly included as with any other input. It's obvious from the paper that the concentration focuses on natural responses (see the reproduced Fig.A2(a ) below) which clearly shows the damping characteristic of the perhaps stochastically-selected (via noise) eigenvalue solution to a differential equation.
" This distinction hinges on whether ENSO variability occurs as a sustained oscillation or limit cycle (supercritical) or is a damped oscillation excited by stochastic forcing (subcritical)."
Yet, it's more than likely that ENSO is the result of a forced response to tidal forces, with the annual nonlinear interaction creating an erratic cycling about the approximate 4 year mean period estimated from an index such as NINO3. For the main long-period tidal factors of Mf and Mm, the annually sidebanded periods are calculated at 3.8 and 3.9 years. The complete nonlinear solution of the shallow-water Laplace's tidal equations used to model oceanic fluid dynamics is described in [1]. A similar training/validation/test procedure is used for finding an optimal predictive fit as that used in machine learning. The main point in this type of modeling is that predictive analysis can conceivably be made years in advance. The continually forcing of the mixed lunar and annual cycles will create the requisite temporal boundary/guiding conditions to maintain coherence over a long range, much like conventional tides do for sea-level height (SLH) analysis.
[1] Pukite, P., Coyne, D., & Challou, D. (2019). Mathematical Geoenergy: Discovery, Depletion, and Renewal (Vol. 241). John Wiley & Sons. https://agupubs.onlinelibrary.wiley.com/doi/10.1002/9781119434351.ch12. Also see the following site for recent information: https://geoenergymath.com/2024/11/10/lunar-torque-controls-all