The hydrological cycle will change substantially in response to global warming. For the most part, wet regions will get wetter and dry regions will get drier as the amount of water the atmosphere can carry increases with warming. But regional patterns of precipitation minus evaporation are influenced by planetary-scale stationary waves, which are subject to substantial shifts and changes in strength as the planet warms. These stationary-wave changes lead to large regional changes in the hydrological cycle and modify the sensitivity of the hydrological cycle to global warming.
One of the most substantial climate changes in response to global warming is the increase in atmospheric water vapor content. Because of the increase in moisture content, existing wind patterns carry more moisture and strengthen the atmospheric branch of the hydrological cycle: storms bring more rainfall, wet regions get wetter, and dry regions get drier (Held and Soden 2006, O’Gorman and Schneider 2009).
Changes in the winds lead to further changes in the hydrological cycle with global warming. For example, there is an expansion of the subtropical dry zones associated with the poleward expansion of the Hadley circulation with global warming (Lu et al. 2009). Even bigger changes can result from shifts or changes in strength of tropical and subtropical convergence zones. These circulation changes lead to regional departures from the “wet gets wetter, dry gets drier” idea (Chou and Neelin 2004, Seager et al. 2010).
Wills et al. (2016) present an analysis of how circulation changes influence the global pattern of change in net precipitation (precipitation minus evaporation, P – E). The focus is on the east-west (or zonal) variations of P – E, and how they change with global warming. Here, we overview some of the findings from this paper.
Zonally anomalous net precipitation, P* – E*, is the difference between the full net precipitation and the zonal mean (denoted by [ ]), where ( )* = ( ) – [ ]. Large positive values of P* – E* indicate anomalously wet regions such as the Asian monsoon regions, the Pacific ITCZ, and the Northern Hemisphere storm tracks; large negative values of P* – E* indicate anomalously dry regions such as the subtropical lows, the Mediterranean, and the Boreal forests (Fig. 1). The change in P* – E* over the next century, as modeled by 23 state-of-the-art climate models forced with continued greenhouse gas emissions throughout the century, is substantial in many regions.
We can estimate the P* – E* changes that would result solely from the increase in atmospheric moisture content, from the fractional increase of zonal-mean surface specific humidity [qs],
A comparison of this “wet gets wetter” or simple thermodynamic scaling to the actual change (Fig. 1) reveals many regions where the sign of change is opposite of the thermodynamic prediction (1/3 of the globe in total). Especially in the tropical oceans, there are large regions where zonally anomalous wet regions get drier and zonally anomalous dry regions get wetter. This lies in contrast to changes in zonal-mean P – E, where the “wet gets wetter” idea explains the modeled drying of the subtropics and wetting of the tropics and midlatitudes with global warming.
The lack of zonal correlation between the P* – E* change and the simple thermodynamic scaling (dashed blue line in Fig. 2) further emphasizes that the “wet gets wetter” mechanism breaks down for anomalies from the zonal mean. To analyze the other mechanisms making up regional P* – E* changes, we can split the moisture budget change into thermodynamic and dynamic components based on changes in specific humidity, q, and changes in winds, u, respectively:
Dynamic changes, that is, changes in stationary-eddy circulations, are strongly correlated with the full P* – E* change (Fig. 2). Transient-eddy changes are also important in the midlatitudes (beyond 30 degrees latitude).
We propose a simplification of the dynamic term, based on the change in stationary-eddy vertical motion at 850 hPa:
This simple approximation captures most of the modeled P* – E* change. The importance of stationary-eddy vertical motions at 850 hPa arises as vertical motions bring moisture from the boundary layer to a mean condensation height of about 850 hPa (Wills and Schneider 2015).
The zonal variance of P – E is unaffected by circulation shifts, and may still increase with the increase in atmospheric moisture content. Indeed, we find that the zonal variance increases at all latitudes over the next century (Fig. 3). However, this increase is less than would be expected from a simple thermodynamic estimate (blue dashed line), obtained by computing the variance of the simple thermodynamic scaling.
Just as for the change in P* – E*, we can split the change in zonal P – E variance into thermodynamic, dynamic, and transient-eddy components. The thermodynamic term based on the moisture budget decomposition dramatically overestimates the change in zonal variance in the tropics and subtropics, but gets the change approximately right at higher latitudes (Fig 3). The total implied dynamic change, which results from stationary-eddy circulation changes and transient-eddy moisture flux changes, is negative at most latitudes. Our paper goes on to show that this is primarily a result of the reduced strength of stationary-eddy overturning circulations, such as the Walker circulation. The reduction of stationary-eddy vertical velocities limits the increase in strength of the zonally anomalous hydrological cycle that would otherwise result from the increased atmospheric moisture content with warming.
The increase in zonal variance of P – E means that regions that are wetter than the zonal mean will get wetter on average and that regions that are drier than the zonal mean will get drier on average. However, the decreasing strength of stationary-eddy circulations means that these changes are smaller on average than would be expected from the “wet gets wetter, dry gets drier” mechanism.
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