Global warming, convective threshold and false thermostats

Geophysical Research Letters American Geophysical Union (AGU) 36:21 (2009)

Authors:

Ian N Williams, Raymond T Pierrehumbert, Matthew Huber

The atmospheric charged kaon/pion ratio using seasonal variation methods

ArXiv 0909.5382 (2009)

Authors:

EW Grashorn, JK de Jong, MC Goodman, A Habig, ML Marshak, S Mufson, S Osprey, P Schreiner

Abstract:

Observed since the 1950's, the seasonal effect on underground muons is a well studied phenomenon. The interaction height of incident cosmic rays changes as the temperature of the atmosphere changes, which affects the production height of mesons (mostly pions and kaons). The decay of these mesons produces muons that can be detected underground. The production of muons is dominated by pion decay, and previous work did not include the effect of kaons. In this work, the methods of Barrett and MACRO are extended to include the effect of kaons. These efforts give rise to a new method to measure the atmospheric K/$\pi$ ratio at energies beyond the reach of current fixed target experiments. These methods were applied to data from the MINOS far detector. A method is developed for making these measurements at other underground detectors, including OPERA, Super-K, IceCube, Baksan and the MINOS near detector.

The atmospheric charged kaon/pion ratio using seasonal variation methods

(2009)

Authors:

EW Grashorn, JK de Jong, MC Goodman, A Habig, ML Marshak, S Mufson, S Osprey, P Schreiner

Stratospheric temperature and radiative forcing response to 11-year solar cycle changes in irradiance and ozone

Journal of the Atmospheric Sciences 66:8 (2009) 2402-2417

Authors:

LJ Gray, ST Rumbold, KP Shine

Abstract:

The 11-yr solar cycle temperature response to spectrally resolved solar irradiance changes and associated ozone changes is calculated using a fixed dynamical heating (FDH) model. Imposed ozone changes are from satellite observations, in contrast to some earlier studies. A maximum of 1.6 K is found in the equatorial upper stratosphere and a secondary maximum of 0.4 K in the equatorial lower stratosphere, forming a double peak in the vertical. The upper maximum is primarily due to the irradiance changes while the lower maximum is due to the imposed ozone changes. The results compare well with analyses using the 40-yr ECMWF Re-Analysis (ERA-40) and NCEP/NCAR datasets. The equatorial lower stratospheric structure is reproduced even though, by definition, the FDH calculations exclude dynamically driven temperature changes, suggesting an important role for an indirect dynamical effect through ozone redistribution. The results also suggest that differences between the Stratospheric SoundingUnit (SSU)/Microwave Sounding Unit (MSU) and ERA-40 estimates of the solar cycle signal can be explained by the poor vertical resolution of the SSU/MSU measurements. The adjusted radiative forcing of climate change is also investigated. The forcing due to irradiance changes was 0.14 W m-2, which is only 78%of the value obtained by employing the standard method of simple scaling of the total solar irradiance (TSI) change. The difference arises because much of the change in TSI is at wavelengths where ozone absorbs strongly. The forcing due to the ozone change was only 0.004 W m-2 owing to strong compensation between negative shortwave and positive longwave forcings. © 2009 American Meteorological Society.

Can the frequency of blocking be described by a red noise process?

Journal of the Atmospheric Sciences 66:7 (2009) 2143-2149

Authors:

G Masato, BJ Hoskins, TJ Woollings

Abstract:

The frequency of persistent atmospheric blocking events in the 40-yr ECMWF Re-Analysis (ERA-40) is compared with the blocking frequency produced by a simple first-order Markov model designed to predict the time evolution of a blocking index [defined by the meridional contrast of potential temperature on the 2-PVU surface (1 PVU ≡ 1 × 10-6 K m2 kg-1 s-1)]. With the observed spatial coherence built into the model, it is able to reproduce the main regions of blocking occurrence and the frequencies of sector blocking very well. This underlines the importance of the climatological background flow in determining the locations of high blocking occurrence as being the regions where the mean midlatitude meridional potential vorticity (PV) gradient is weak. However, when only persistent blocking episodes are considered, the model is unable to simulate the observed frequencies. It is proposed that this persistence beyond that given by a red noise model is due to the self-sustaining nature of the blocking phenomenon. © 2009 American Meteorological Society.