(Top left) Global
annual mean radiative influences (W m — 2) of LGM climate change agents, generally feedbacks in glacial - interglacial cycles, but also specified in most Atmosphere - Ocean General Circulation Model (AOGCM) simulations for the LGM.
Not exact matches
Tsushima, Y., A. Abe - Ouchi, and S. Manabe, 2005:
Radiative damping of
annual variation in global
mean surface temperature: Comparison between observed and simulated feedback.
To contribute to an understanding of the underlying causes of these changes we compile various environmental records (and model - based interpretations of some of them) in order to calculate the direct effect of various processes on Earth's
radiative budget and, thus, on global
annual mean surface temperature over the last 800,000 years.
The importance of orbital variations, of the greenhouse gases CO2, CH4 and N2O, of the albedo of land ice sheets,
annual mean snow cover, sea ice area and vegetation, and of the
radiative perturbation of mineral dust in the atmosphere are investigated.
Abstract:» The sensitivity of global climate with respect to forcing is generally described in terms of the global climate feedback — the global
radiative response per degree of global
annual mean surface temperature change.
Therefore, the total
annual and global
mean radiative forcing during the LGM is likely to have been approximately — 8 W m — 2 relative to 1750, with large seasonal and geographical variations and significant uncertainties (see Section 6.4.1).
Abstract:» The sensitivity of global climate with respect to forcing is generally described in terms of the global climate feedback — the global
radiative response per degree of global
annual mean surface temperature change.
The term «climate sensitivity» refers to the steady - state increase in the global
annual mean surface air temperature associated with a given global
mean radiative forcing.
Figure 7.18
Annual mean top of the atmosphere
radiative forcing due to aerosol — radiation interactions (RFari, in W m — 2) due to different anthropogenic aerosol types, for the 1750 — 2010 period.
«A multiple linear regression analysis of global
annual mean near - surface air temperature (1900 — 2012) using the known
radiative forcing and the El Niño — Southern Oscillation index as explanatory variables account for 89 % of the observed temperature variance.
The global
annual mean top of the atmosphere DMS aerosol all sky
radiative forcing is − 2.03 W / m2, whereas, over the southern oceans during SH summer, the
mean DMS aerosol
radiative forcing reaches − 9.32 W / m2.»
The climate sensitivity parameter (units: °C (W m - 2)-1) refers to the equilibrium change in the
annual mean global surface temperature following a unit change in
radiative forcing.
However, it should be noted that all of these studies suggest the majority of the global
annual mean direct
radiative forcing due to sulphate occurs in cloud - free regions.
ECS is the increase in the global
annual mean surface temperature caused by an instantaneous doubling of the atmospheric concentration of CO2 relative to the pre-industrial level after the model relaxes to
radiative equilibrium, while the TCR is the temperature increase averaged over 20 years centered on the time of doubling at a 1 % per year compounded increase.
The spatial distribution of the forcings is similar in the studies showing strongest
radiative forcings over industrial regions of the Northern Hemisphere although the ratio of the
annual mean Northern Hemisphere / Southern Hemisphere
radiative forcing varies from 2.0 (Graf et al., 1997) to 6.9 (Myhre et al., 1998c)(see Section 6.14.2 for further details).
Global -
annual mean adjusted
radiative forcing at the top of the atmosphere is, in general, a reliable metric relating the effects of various climate perturbations to global
mean surface temperature change as computed in general circulation models (GCMs).
Therefore, the total
annual and global
mean radiative forcing during the LGM is likely to have been approximately — 8 W m — 2 relative to 1750, with large seasonal and geographical variations and significant uncertainties (see Section 6.4.1).
The
annual mean forcing from these cloud systems is in the range of — 45 to — 55 W m — 2 and effectively these cloud systems are shielding both the northern and the southern polar regions from intense
radiative heating.