The Invisible Thread Between Ocean and Rain Is Getting Stronger ✎

Original: "Nonlinear forced change and nonergodicity: The case of ENSO-Indian monsoon and global precipitation teleconnections"
arXiv:2009.02155 · 2020-09-04 · arXiv non-exclusive · independent analysis · 1 min
The link between a warm Pacific current and Indian rainfall is strengthening, but unevenly, like a rope braided in fits and starts.

Every few years, the water in the Pacific Ocean off the coast of South America becomes warmer than usual. This phenomenon is called El Niño. It affects weather around the world, and especially rainfall in India. When El Niño arrives, monsoon rains often weaken, leading to droughts.

El Niño is a warm current in the Pacific Ocean that changes weather across the entire planet.

Scientists wanted to know whether this connection changes over time. They ran the same climate model 63 times with slight differences in initial conditions, producing 63 possible futures. In every one, the link between El Niño and Indian rainfall strengthened. But it did so unevenly: faster in some years, slower in others. Like a rope braided in fits and starts, it becomes stronger, but not smoothly.

This finding matters for forecasts. If the connection shifts unevenly, historical data can mislead. Models need constant updates to better predict droughts and floods in India, since these rains determine the harvest and the lives of hundreds of millions of people.

The non-ergodicity test showed that even if the correlation changes linearly over time, biases can arise if mean values or standard deviations change. In this case, these trivial contributions turned out to be insignificant, confirming the true nonlinearity of the forced response.

r = \frac{1}{\sqrt{1 + (\sigma_\xi / a \sigma_\Phi)^2}}
This formula shows that an increase in correlation can be caused by an increase in ENSO variability, an increase in the regression coefficient, or a decrease in noise.
a = r \frac{\sigma_\Psi}{\sigma_\Phi}
Allows estimation of the regression coefficient given the correlation and standard deviations of the variables.
v = \sum_{t=1}^{T} \sum_{n=1}^{N} (\hat{z}_{\tau,t,n} - \hat{z}_t)^2
Sum of squared differences between temporal and ensemble z-transformations of correlations; large values indicate non-ergodicity.
Concepts
ENSO interannual variability Teleconnection spring predictability barrier Multivariate ENSO Index Jin-Timmermann model El Niño-Southern Oscillation El Niño index TAO/TRITON moorings monsoon onset monsoon natural variability seasonal forcing Southern Oscillation La Niña recharge oscillator model ocean-atmosphere coupling relative ONI Indian Ocean Dipole ensemble forecast