GFDL - Geophysical Fluid Dynamics Laboratory

Evaluation of cloud and water vapor simulations in CMIP5 climate models using NASA “A-Train” satellite observations

July 23rd, 2012

Jonathan H Jiang, Hui Su, Chengxing Zhai, Vincent Perun, Anthony D. Del Genio, Larissa S. Nazarenko, Leo J. Donner, Larry Wayne Horowitz, Charles J. Seman, Jason Cole, Andrew Gettelman, Mark Adam Ringer, Leon D. Rotstayn, Stephen J. Jeffrey, Tongwen Wu, Florent Brient, Jean-Louis Dufresne, Hideaki Kawai, Tsuyoshi Koshiro, Watanabe Masahiro, Tristan Simon LEcuyer, Evgeny M. Volodin, Trond Iversen, Helge Drange, Michel dos Santos Mesquita, William G. Read, Joe W. Waters, Baijun Tian, Joao Teixeira, Graeme L. Stephens. Journal: Journal of Geophysical Research. DOI: 10.1029/2011JD017237

Summary

Clouds and water vapor are among the difficult features of the atmosphere for global climate models to simulate because they are affected by physical processes that operate over very small areas compared to the weather patterns that the models explicitly calculate. The authors used satellite data to assess the representation of clouds and water vapor simulated by several climate models that will participate in the Intergovernmental Panel on Climate Change (IPCC) Fifth Assessment Report (AR5).

This paper compares the new generation of models, including GFDL’s CM3, to state-of-the-art satellite data sets produced by NASA’s Jet Propulsion Laboratory. Using these data sets, the authors were able to examine the models in greater detail than was previously possible, including the vertical distribution of cloud and water vapour.

The study finds measurable improvements in the more recent models relative to the previous generation of climate models, in simulating the amount and the vertical and geographical distribution of clouds and water vapor over the globe. For clouds and water vapour over the tropical ocean, the study concludes that both the largest spread among models and the largest differences between models and satellite observations are at high altitudes, where cirrus clouds and anvil clouds associated with thunderstorms form.

Multi-year mean liquid water path from IPCC AR4 and AR5 models, and three estimates from A-train observations. The liquid water path is the total mass of liquid (per unit area) throughout the depth of the atmosphere. The resolution is 2 deg latitude by 2.5 deg longitude.
Multi-year mean liquid water path from IPCC AR4 and AR5 models, and three estimates from A-train observations. The liquid water path is the total mass of liquid (per unit area) throughout the depth of the atmosphere. The resolution is 2 deg latitude by 2.5 deg longitude.