Numéro |
J. Phys. IV France
Volume 121, December 2004
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Page(s) | 1 - 35 | |
DOI | https://doi.org/10.1051/jp4:2004121001 |
J. Phys. IV France 121 (2004) 1-35
DOI: 10.1051/jp4:2004121001
Astronomical theory of climate change
A. Berger and M.F. LoutreUniversité catholique de Louvain, Institut d'Astronomie et de Géophysique Georges Lemaître, Chemin du Cyclotron, 2, 1348 Louvain-la-Neuve, Belgique
Abstract
The astronomical theory of paleoclimates aims to
explain the climatic variations occurring with quasi-periodicities lying
between tens and hundreds of thousands of years. Such variations are
recorded in deep-sea sediments, in ice sheets and in continental archives.
The origin of these quasi-cycles lies in the astronomically driven changes
in the latitudinal and seasonal distributions of the energy that the Earth
receives from the Sun. These changes are then amplified by the feedback
mechanisms which characterize the natural behaviour of the climate system
like those involving the albedo-, the water vapor-, and the vegetation-
temperature relationships. Climate models of different complexities are used
to explain the chain of processes which finally link the long-term
variations of three astronomical parameters to the long-term climatic
variations at time scale of tens to hundreds of thousands of years. In
particular, sensitivity analysis to the astronomically driven insolation
changes and to the CO2 atmospheric concentrations have been performed
with the 2-dimension climate model of Louvain-la-Neuve. It could be shown
that this model simulates more or less correctly the entrance into
glaciation around 2.75 Myr BP, the late Pliocene-early Pleistocene 41-kyr
cycle, the emergence of the 100-kyr cycle around 850 kyr BP and the
glacial-interglacial cycles of the last 600 kyr. During the Late Pliocene
(in an ice-free - warm world) ice sheets can only develop during times of
sufficiently low summer insolation. This occurs during large eccentricity
times when climatic precession and obliquity combine to obtain such low
values, leading to the 41-kyr period between 3 and 1 Myr BP. On the contrary
in a glacial world, ice sheets persist most of the time except when
insolation is very high in polar latitudes, requiring large eccentricity
again, but leading this time to interglacial and finally to the 100-kyr
period of the last 1 Myr. Using CO2 scenarios, it has been shown that
stage 11 and stage 1 request a high CO2 to reach the interglacial
level. Moreover, the insolation pattern at both stages and modeling results
lead to conclude that stage 11 is a better analogue for our future climate
than the Eem. Although the insolation changes alone act as a pacemaker for
the glacial-interglacial cycles, CO2 changes help to better reproduce
past climatic changes and, in particular, the air temperature and the
southern extend of the Northern Hemisphere ice sheets. Insolation and
CO2 scenarios for the next 130 kyr lead to an interglacial which will
most probably last particularly long (50 kyr). This conclusion is reinforced
by the possible intensification of the greenhouse effect which might result
from man's activities over the next centuries.
© EDP Sciences 2004