A Switchback Pendulum: How Seasons Drive El Niño ✛ ✎

Original: "Seasonal Forcing Dominated Dynamics of a piecewise smooth Ghil-Zaliapin-Thompson ENSO model"
arXiv:2510.27084 · 2025-10-31 · arXiv non-exclusive · independent analysis · 2 min
Mathematicians replaced a complex climate model with a simple switchback pendulum and showed that it faithfully reproduces the ocean's behavior.

Imagine a pendulum that is pushed in time with the seasons: harder in winter, softer in summer. But this pendulum has a quirk: a switch that operates with a delay. When the pendulum passes through zero, the switch clicks and changes the direction of the push. That is exactly how the simplified El Niño model built by mathematicians works.

El Niño is a climate cycle in the Pacific Ocean where warm water piles up either off the coast of South America or near Indonesia. This affects rains, droughts, and hurricanes worldwide.

In the original Gil–Zaliapin–Thompson (GZT) model, the feedback is described by a smooth function: the hyperbolic tangent. But solving such equations analytically is nearly impossible. The authors replaced the smooth function with a sign function: it takes only two values, plus or minus, like a switch. Meanwhile, the seasonal forcing remained smooth, in the form of a cosine. The result is a pendulum pushed periodically, with the switch acting after a delay.

For such a pendulum, explicit solutions were found. It turns out that it performs periodic oscillations, and one can precisely calculate for which parameters these oscillations are stable. If the amplitude of the seasonal forcing is large enough, the oscillations are stable; as the amplitude decreases, they lose stability through a torus bifurcation or a fold.

A torus bifurcation is when periodic motion becomes quasiperiodic: the oscillation slowly 'drifts' in frequency, like two pendulums with nearly equal periods.

Comparison with numerical calculations of the original GZT model showed excellent agreement. The bifurcation curves and rotation numbers almost coincide, especially for large values of the coupling and delay parameters. This means that the crude simplification does not distort the essence of the phenomenon, but rather makes it accessible to precise analysis.

The switchback pendulum, pushed in time with the seasons, turned out to be more than just a toy. It allows one to rigorously explain why El Niño sometimes behaves regularly and sometimes falls out of rhythm. And now this simple mechanism can be used as a benchmark for testing complex climate models.

The GZT model was proposed in 2008 and named after three scientists: Michael Ghil, Ilya Zaliapin, and Michael Thompson. It has become one of the most studied conceptual ENSO models due to its simplicity and ability to reproduce key features of the phenomenon.

h'(t) = -\operatorname{sign}(h(t-\tau)) + c \cos(2\pi t)
The rate of change of thermocline depth equals minus the sign function of the delayed depth plus seasonal forcing.
\Delta_{2k+1}(\lambda) = (\lambda-1)\lambda^{2k} + \frac{4}{h'(\alpha)}\lambda^k - \frac{4}{[h'(\alpha)]^2}
The polynomial whose roots determine the stability of the periodic orbit.
Scientists
Ludwig BoltzmannJohn von NeumannJosiah Willard GibbsHenri Poincaré
Concepts
Jin-Timmermann model seasonal forcing El Niño-Southern Oscillation ENSO spring predictability barrier recharge oscillator model TAO/TRITON moorings El Niño index seasonal cycle Multivariate ENSO Index tropospheric biennial oscillation La Niña periodic orbit mixed mode oscillations delayed oscillator theory natural variability annual cycle