The Tropical Lower Stratospheric Response to 11Year Solar Forcing: Dynamical Feedbacks From the Troposphere-Ocean Response Lon Hood Lunar and Planetary Laboratory University of Arizona Tucson, Arizona USA Acknowledgments: Boris Soukharev SORCE Science Meeting Sedona, Arizona September 14, 2011 The Mean Meridional Circulation Inferred from the Observed Distributions of Trace Species (Ozone, Water Vapor, Methane, etc.): The ``Brewer-Dobson’’ Circulation E. Cordero et al., Stratospheric Ozone Electronic Textbook, NASA/GSFC C Solar versus Volcanic Origin: P After Hood et al., JGR, 2010 Timing agrees better with solar origin than with volcanic origin Ground-based ozone data prior to 1979 also show a solar cycle variation (WMO, 2006) Comparison of tropical column ozone record with 50 hPa temperature record from NCEP/NCAR Reanalysis data. 35oS to 35oN: Deseasonalized MULTIPLE REGRESSION STATISTICAL MODEL: Y’(t) = ctrendt + ctrendt’+ cQBO1u30mb(t-lagQBO1)+ cQBO2u10mb(t-lagQBO2) + cvolcanicAerosol(t) + csolar MgII(t) + dENSON3.4(t-lagENSO)+ (t) where: Y’(t) = deviation of atmospheric quantity from the seasonal mean t = time measured in 3-month seasonal increments t , = 0 for t < T0 ; t , = (t - T0) for t ≥ T0 ; T0 = DJF of 1996 U30(10)mb(t- lagQBO) = NCEP 30(10) mb equatorial wind speed (lagged) Aerosol(t) = Volcanic aerosol index (10 hPa and below only) MgII(t) = Solar MgII UV index N3.4(t-lagENSO) = Mean SST, 5oS - 5oN, 120oW - 170oW (lagged) (t) = residual error term ``Observed’’ Solar Cycle Variation of Stratospheric Ozone: (Estimated from a Multiple Regression Statistical Analysis of SAGE II Data, 1985-2003) Positive up to at least 54 km. Updated from Soukharev and Hood, JGR, 2006 Shaded areas are statistically significant at 95% confidence. SAGE II WACCM3 coupled to CCSM3: 2.5 1.0 1.5 Observations Model SAGE II WACCM3 coupled to CCSM3: 2.5 1.0 1.5 Observations Model What is producing the unexpectedly large lower stratospheric response to the solar cycle? SAGE II WACCM3 coupled to CCSM3: 2.5 1.0 1.5 Observations Model The observed lower stratospheric response to the solar cycle may imply a solar-induced weakening of the mean meridional (Brewer-Dobson) circulation near solar maxima that is not fully simulated by current models. The observed decadal variation of extratropical wave forcing has peaks near or approaching solar minima and has troughs near or approaching solar maxima: ``Top-Down’’ Solar UV Forcing Mechanism: Solar UV-induced enhancements of the lower mesospheric subtropical jet (LMSJ) near the time of winter solstice lead to changes in planetary wave propagation and the strength of the Brewer-Dobson circulation. The net result for the tropical stratosphere is relative downwelling under solar maximum conditions. A number of observational and model studies have supported this mechanism: Gray et al., 2001a,b; 2003; 2004; 2007; Matthes et al., 2004; 2006. However, the model response in the lower stratosphere is generally much weaker than is seen in the observations. Transportinduced O3 and T increase; + radiative T increase Kodera and Kuroda, JGR, 2002: On the other hand, changes in surface climate can also influence the BDC. Icelandic Low Siberian High Aleutian Low The sea level pressure distribution in the northern winter extratropics forces planetary-scale Rossby waves (``planetary waves’’) that propagate up into the stratosphere and drive the mean meridional (Brewer-Dobson) circulation. ``Bottom-Up’’ Solar Forcing Mechanism: Hypothesis: A significant troposphere-ocean response to solar total solar irradiance (TSI) forcing exists (van Loon et al., 2007; Meehl et al., 2009). If so, then the troposphere-ocean response will modify planetary wave forcing at the lower boundary, modify the BDC, and may produce part or all of the observed lower stratospheric response. Composite averages for DJF during 11 peak solar years (van Loon et al., [2007]: The derived response resembles that during a La Niña (cold ENSO) event. After Meehl et al., Science, 2009, and van Loon et al., JGR, 2007. ENSO Regression Coefficients: Sea surface temperature (SST) and sea level pressure (SLP) response to a moderate La Niña event (change in the Niña 3.4 index of -1 unit) during NH winter. oC 3.5 hPa hPa Sea surface temperature (SST) and sea level pressure (SLP) response to the 11-year solar cycle (solar max - min) based on Hadley Centre data over the 1908-2009 period. hPa HADLEY 3.3 hPa SLP results are consistent with previous studies: Christoforou and Hameed, 1997; van Loon et al., 2007; Roy and Haigh, 2010. oC 3.3 hPa The sea level pressure response to the solar cycle has similarities to the SLP response to a moderate La Niña event (change in the Niña 3.4 index of -1 unit) during NH winter. oC 3.5 hPa hPa Solar Regression Coefficient ENSO Regression Coefficient Transportinduced NOX decrease; photochemic al O3 increase Transport-induced ozone decrease Reproducibility Test for ENSO Aliasing: Solar regression coefficients at zero lag for Hadley Centre Sea Level Pressure (SLP) and Sea Surface Temperature (SST) over the 1880-1945 period: SLP Response is centered on a lag of about -1 year. Areas enclosed by dark lines are formally significant at 95% confidence. Reproducibility Test for ENSO Aliasing: Solar regression coefficients at zero lag for Hadley Centre Sea Level Pressure (SLP) and Sea Surface Temperature (SST) over the 1946-2009 period: SLP Response is centered on a lag of about -1 year. Areas enclosed by dark lines are formally significant at 95% confidence. Conclusions: 1. There is observational evidence for solar cycle responses of lower stratospheric ozone and temperature at tropical and subtropical latitudes. 2. There is observational evidence for solar cycle responses of sea level pressure and (to a much lesser extent) sea surface temperature in the North Pacific region over the 1880-2009 period. The SLP response consists of a weakening and westward shift of the Aleutian low near and approaching solar maxima. This is similar to the SLP response to a moderate La Niña event. 3. The weakened Aleutian low near solar maxima reduces the planetary wave one amplitude near the surface, which results in a reduced planetary wave flux in the extratropical lower stratosphere. This reduced wave flux implies a deceleration of the Brewer-Dobson circulation, which reduces the tropical upwelling rate, leading to increased tropical ozone column amounts. 4. This ``bottom-up’’ mechanism probably contributes significantly to producing the tropical lower stratospheric response, including the solar cycle variation of total ozone. Extra Slides Extratropical Wave Forcing of the Brewer-Dobson Circulation: F 0 u/t < 0 w* > 0 dT/dt < 0 dO3/dt < 0 w* > 0 dT/dt > 0 dO3/dt > 0 Tropopause Vertically Propagating, Planetary-Scale Rossby Waves Equator Pole Surface Winter Hemisphere Extreme wave forcing events can lead to polar stratospheric sudden warmings (SSWs). Model Simulation of the Solar Cycle Variation of Stratospheric Ozone: WACCM3 coupled to CCSM3 with imposed QBO: Multiple regression analysis of WACCM3 model data done by Christian Blume and Katja Matthes, FUB. We also know that solar variability can affect planetary wave propagation, polar vortex strength, and the Brewer-Dobson circulation. From Gray et al., Reviews of Geophysics, 2010 During the west phase of the QBO near solar maxima, planetary wave propagation is altered such that more stratospheric warmings occur than during solar minima. UARS MLS Water Vapor Mixing Ratio Deviations, ppmV Alan Brewer, QJRMS, 1949; Gordon Dobson, PRSL, 1956: Mote et al., JGR, 1996 The water content of air at northern midlatitudes just above the tropopause is very low. This is best explained by a circulation in which air enters the stratosphere where it is dried by condensation during passage through the cold tropical tropopause, travels to higher latitudes, and sinks into the troposphere. The same circulation would simultaneously explain why ozone values are highest at high latitudes even though it is produced mainly at low latitudes. Hence, the ``Brewer-Dobson’’ circulation. E. Cordero et al., Chapter 6, Stratospheric Ozone, NASA/GSFC