The Entropy of Climate Swings ✛

Original: "Statistics of stochastic entropy for recorded transitions between ENSO states"
· Sílvio M. Duarte Queirós
arXiv:2507.10516 · 2025-07-14 · CC BY 4.0 · 3 min
Transitions between El Niño and La Niña turn out to be statistically ordinary events, not extreme entropy spikes.

You can sit on a seesaw and pump your legs, or you can just tip from one side to the other. The Pacific Ocean does both. Every few years, warm water off the coast of Peru gives way to cooler water, and rainfall patterns, winds, and entire ecosystems across half the planet reshuffle. These shifts are called El Niño and La Niña, together known as ENSO: Earth's climate seesaw.

For a long time, climatologists tracked the seesaw using a single number: the atmospheric pressure difference between Tahiti and Darwin, Australia. When pressure rises in Darwin and falls in Tahiti, the index goes negative, and El Niño sets in. When the opposite happens, it's La Niña. This index, the SOI, has been recorded daily from 1991 to 2023, yielding 11,744 data points. The author of the new study decided to ask not "when will the seesaw tip," but "how unusual is the very swing from one side to the other?"

Entropy here isn't about mess in a room; it's about irreversibility. If you film a system's motion and play it backward, the reverse version of an irreversible process looks impossible. The measure of that impossibility is the entropy change.

To calculate the entropy of a transition, the author first extracted a slow background from the daily SOI values: the annual cycle, the Madden–Julian oscillation, and five other rhythms. He described the remainder as a random walk in which the strength of random kicks depends on the current state, much as gusts of wind rock a swing harder once it's already moving. Then, for each of the 11 transitions between phases, he compared the probability of the forward path with that of the reverse path. If the forward path is much more likely than the reverse, entropy increases sharply, and the transition can be called extreme.

It turns out that nearly all transitions are ordinary. Only one, from the strong La Niña of 1999–2000 to the moderate El Niño of 2002–2003, deviated from the mean by four standard deviations. That's like the seesaw suddenly looping the loop, but even such a loop fits within the rules of the game: all transitions satisfied the probabilistic version of the second law of thermodynamics. In other words, the climate seesaw doesn't squeak.

Key takeaway: the informational entropy of the SOI index is only weakly related to the thermal entropy of the ocean. The indicator may miss details that matter for the phenomenon itself.

Previously, it was unclear whether fluctuation theorems could be applied to climate indices at all, and whether ENSO transitions are extreme events. Now it's clear that almost all of them are statistically ordinary, with only one approaching the threshold. The method can be extended to multivariate indicators: sea surface temperature, outgoing radiation, precipitation. Then entropy analysis would no longer depend on a single number and would reveal which components of the system truly carry information about the phase transition. For now, the seesaw swings without squeaking, and that in itself is news.

El Niño literally translates from Spanish as 'the boy,' and La Niña as 'the girl.' The names arose because the warm current off Peru often appeared around Christmas, associating it with the Christ child.

\Delta S(\vec{s}) = -\ln\frac{p(s_{t_f}; \{s_{t_i},\ldots,s_{t_{f-1}}\})}{p(s_{t_i}; \{s_{t_{i+1}},\ldots,s_{t_f}\})}
Logarithm of the ratio of probabilities of forward and backward SOI trajectories
p_t^*(s) = \frac{1}{Z_t^*}\exp\left[\frac{a\beta+2b\alpha^2}{\alpha^2\sqrt{4\alpha^2\gamma^2-\beta^2}}\arctan\left(\frac{\beta+2\alpha^2(s-\Phi(t))}{\sqrt{4\alpha^2\gamma^2-\beta^2}}\right)\right]\left(\gamma^2+\beta(s-\Phi(t))+\alpha^2(s-\Phi(t))^2\right)^{-(1+\frac{a}{2\alpha^2})}
Probability distribution of SOI values given the background protocol
ds = D_1(s,t)\,dt + \sqrt{2D_2(s,t)}\,dW_t
SOI dynamics with drift and multiplicative noise
Scientists
Ludwig BoltzmannRudolf ClausiusJacob BekensteinStephen HawkingJames Clerk MaxwellEdward Witten
Concepts
ENSO El Niño index El Niño-Southern Oscillation Multivariate ENSO Index ERSST spring predictability barrier Southern Oscillation La Niña Jin-Timmermann model recharge oscillator model NOAA CPC interannual variability TAO/TRITON moorings natural variability Warm water volume relative ONI stochastic dynamical system seasonal cycle mixed mode oscillations Westerly wind burst