Why El Niño First Strengthens and Then Weakens ✛

Original: "The Rise and Fall of ENSO in a Warming World: Insights from a Lag-Linear Model"
· PJ Tuckman, Da Yang
arXiv:2603.03458 · 2026-03-03 · CC BY 4.0 · 2 min
A simple delay model explains why El Niño first intensifies and then fades under warming, and allows predicting its strength without running climate models.

Every few years, the Pacific Ocean off the coast of Peru warms so abruptly that fish disappear and rains flood the desert. This phenomenon is called El Niño, and it acts like a pendulum that swings the planet's climate. But when the planet itself warms, the pendulum behaves strangely: first its swing widens, then it suddenly fades. Why does that happen?

The reason is that the ocean warms unevenly. The upper layer, which touches the air, warms quickly. Deeper layers, especially water at about a hundred meters depth, lag behind by decades. It's like heating an old house: the radiator by the window heats up right away, but the far wall only warms an hour later. While the top is warm and the bottom is cold, the boundary between them acts like a taut string: any disturbance travels along it more strongly. So in the first decades of warming, El Niño indeed intensifies.

El Niño is the warm phase of a natural oscillation in sea surface temperatures of the eastern Pacific. Its opposite, La Niña, brings unusually cold water.

But there is a second process. The winds that blow along the equator from east to west push warm water toward Indonesia. As the climate warms, these winds weaken. The conveyor slows, and the temperature difference between west and east diminishes. That means El Niño has less energy to draw from. The pendulum begins to fade.

Scientists built a model that accounts for this lag between surface warming and deep warming. It takes today's surface temperature and the surface temperature from thirty-six years ago, and from these two numbers predicts El Niño's strength. Across different climate models, this simple formula explains about ninety percent of the variability. The peak swing occurs roughly fifty years after warming begins, and by the end of the century El Niño strength could drop by forty percent relative to preindustrial levels. A pendulum that is swung and then damped is an apt description of how the climate system works.

Economic losses from the extreme El Niño events of 1997–1998 and 2015–2016 are estimated at 4.1 and 5.7 trillion dollars, respectively, while La Niña brings only modest economic benefits.

\Delta M_{\mathrm{ENSO}}(t) = \alpha \Delta \mathrm{GMST}(t) + \beta \Delta \mathrm{GMST}(t - t_{\mathrm{lag}})
The change in ENSO strength equals the sum of contributions from the current sea surface temperature and from the temperature with a lag corresponding to the subtropical cell time.
Scientists
Ludwig BoltzmannJohn von NeumannJosiah Willard GibbsHenri Poincaré
Concepts
ENSO El Niño-Southern Oscillation El Niño index Southern Oscillation spring predictability barrier La Niña Jin-Timmermann model Multivariate ENSO Index recharge oscillator model TAO/TRITON moorings natural variability ERSST Warm water volume equatorial wave propagation interannual variability relative ONI North Equatorial Countercurrent NOAA CPC NOAA PMEL / TAO ocean-atmosphere coupling