These older papers appear to be of interest to geoengineers as they
consider post-volcanic particulate response.  By my understanding of
the abstracts below, the climate response is less than expected.

Timmreck C et al. (2009) Geophys. Res. Lett. 36, doi:10.1029/2009GL040083
http://www.agu.org/pubs/crossref/2009/2009GL040083.shtml

Timmreck C et al. (2010) Geophys. Res. Lett. 37, doi:10.1029/2010GL045464
http://www.agu.org/pubs/crossref/2010/2010GL045464.shtml


A

http://www.agu.org/pubs/crossref/2009/2009GL040083.shtml

Limited temperature response to the very large AD 1258 volcanic eruption
The large AD 1258 eruption had a stratospheric sulfate load
approximately ten times greater than the 1991 Pinatubo eruption. Yet
surface cooling was not substantially larger than for Pinatubo (∼0.4
K). We apply a comprehensive Earth System Model to demonstrate that
the size of the aerosol particles needs to be included in simulations,
especially to explain the climate response to large eruptions. The
temperature response weakens because increased density of particles
increases collision rate and therefore aerosol growth. Only aerosol
particle sizes substantially larger than observed after the Pinatubo
eruption yield temperature changes consistent with terrestrial
Northern Hemisphere summer temperature reconstructions. These results
challenge an oft-held assumption of volcanic impacts not only with
respect to the immediate or longer-term temperature response, but also
any ecosystem response, including extinctions.


http://www.agu.org/pubs/crossref/2010/2010GL045464.shtml

Aerosol size confines climate response to volcanic super-eruptions
Extremely large volcanic eruptions have been linked to global climate
change, biotic turnover, and, for the Younger Toba Tuff (YTT) eruption
74,000 years ago, near-extinction of modern humans. One of the largest
uncertainties of the climate effects involves evolution and growth of
aerosol particles. A huge atmospheric concentration of sulfate causes
higher collision rates, larger particle sizes, and rapid fall out,
which in turn greatly affects radiative feedbacks. We address this key
process by incorporating the effects of aerosol microphysical
processes into an Earth System Model. The temperature response is
shorter (9–10 years) and three times weaker (−3.5 K at maximum
globally) than estimated before, although cooling could still have
reached −12 K in some midlatitude continental regions after one year.
The smaller response, plus its geographic patchiness, suggests that
most biota may have escaped threshold extinction pressures from the
eruption.

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