<?xml version="1.0" encoding="utf-8"?><rss version="2.0"><channel><title>ESDD - Latest Articles</title><link>http://www.earth-syst-dynam-discuss.net/</link><description>Earth System Dynamics Discussions Latest Articles</description><language>en</language><item><title>On the determination of the global cloud feedback from satellite measurements</title><link>http://www.earth-syst-dynam-discuss.net/3/73/2012/</link><description>&lt;b&gt;On the determination of the global cloud feedback from satellite measurements&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 3, 73-90, 2012&lt;br /&gt;&lt;br /&gt;Author(s): T. Masters&lt;br /&gt;&lt;br /&gt;A detailed analysis is presented in order to determine the sensitivity of
the estimated short-term cloud feedback to choices of temperature datasets,
sources of top-of-atmosphere (TOA) radiative flux data, and temporal
averaging. It is shown that the results of a previous analysis, which
suggested a likely positive value for the short-term cloud feedback,
depended upon combining radiative fluxes from satellite and reanalysis data
when determining the cloud radiative forcing (CRF). These results are
contradicted when &amp;Delta;CRF is derived from NASA's Clouds and Earth's
Radiant Energy System (CERES) all-sky and clear-sky measurements over the
same period, resulting in a likely negative feedback. The differences
between the radiative flux data sources are thus explored, along with the
potential problems with each method. Overall, there is little correlation
between the changes in the CRF and surface temperatures on these timescales,
suggesting that the net effect of clouds varies during this time period
quite apart from global temperature changes. Attempts to diagnose long-term
cloud feedbacks in this manner are unlikely to be robust.</description><pubDate>Fri, 03 Feb 2012 00:00:00 +0100</pubDate></item><item><title>Can a reduction of solar irradiance counteract CO&lt;sub&gt;2&lt;/sub&gt;-induced climate change? – Results from four Earth system models</title><link>http://www.earth-syst-dynam-discuss.net/3/31/2012/</link><description>&lt;b&gt;Can a reduction of solar irradiance counteract CO&lt;sub&gt;2&lt;/sub&gt;-induced climate change? – Results from four Earth system models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 3, 31-72, 2012&lt;br /&gt;&lt;br /&gt;Author(s): H. Schmidt, K. Alterskjær, D. Bou Karam, O. Boucher, A. Jones, J. E. Kristjansson, U. Niemeier, M. Schulz, A. Aaheim, F. Benduhn, M. Lawrence, and C. Timmreck&lt;br /&gt;&lt;br /&gt;In this study we compare the response of four state-of-the-art Earth system
models to climate engineering under scenario G1 of the GeoMIP and IMPLICC
model intercomparison projects. In G1, the radiative forcing from an
instantaneous quadrupling of the CO&lt;sub&gt;2&lt;/sub&gt; concentration, starting from the
preindustrial level, is balanced by a reduction of the solar constant. Model
responses to the two counteracting forcings in G1 are compared to the
preindustrial climate in terms of global means and regional patterns and
their robustness. While the global mean surface air temperature in G1 remains
almost unchanged, the meridional temperature gradient is reduced in all
models compared to the control simulation. Another robust response is the
global reduction of precipitation with strong effects in particular over
North and South America and northern Eurasia. It is shown that this reduction
is only partly compensated by a reduction in evaporation so that large
continental regions are drier in the engineered climate. In comparison to the
climate response to a quadrupling of CO&lt;sub&gt;2&lt;/sub&gt; alone the temperature responses
are small in experiment G1. Precipitation responses are, however, of
comparable magnitude but in many regions of opposite sign.</description><pubDate>Wed, 25 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Comparison of physically- and economically-based CO&lt;sub&gt;2&lt;/sub&gt;-equivalences for methane</title><link>http://www.earth-syst-dynam-discuss.net/3/1/2012/</link><description>&lt;b&gt;Comparison of physically- and economically-based CO&lt;sub&gt;2&lt;/sub&gt;-equivalences for methane&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 3, 1-29, 2012&lt;br /&gt;&lt;br /&gt;Author(s): O. Boucher&lt;br /&gt;&lt;br /&gt;There is a controversy on the role methane (and other short-lived species)
should play in climate mitigation policies and no consensus on what an
optimal methane CO&lt;sub&gt;2&lt;/sub&gt;-equivalence should be. We revisit this question by
discussing the relative merits of physically-based (i.e. Global
Warming Potential or GWP and Global Temperature change Potential or GTP)
and socio-economically-based climate metrics. To this effect we use
a simplified Global Damage Potential (GDP) that was introduced by
earlier authors and investigate the uncertainties in the methane
CO&lt;sub&gt;2&lt;/sub&gt;-equivalence that arise from physical and socio-economic
factors. The median value of the methane GDP comes out very close to the
widely used methane 100-year GWP because of various compensating effects.
However there is a large spread in possible methane CO&lt;sub&gt;2&lt;/sub&gt;-equivalences
(1–99% interval: 10.0–42.5; 5–95% interval: 12.5–38.0) that is essentially
due to the choice in some socio-economic parameters (i.e. the damage cost
function and the discount rate). The methane 100-year GTP falls
outside these ranges. It is legitimate to increase the methane
CO&lt;sub&gt;2&lt;/sub&gt;-equivalence in the future as global warming unfolds.
While changes in biogeochemical cycles and radiative efficiencies
cause some small changes to physically-based metrics, a
systematic increase in the methane CO&lt;sub&gt;2&lt;/sub&gt;-equivalence can only
be achieved by some ad-hoc shortening of the time horizon. In contrast
using a convex damage cost function provides a natural increase in the
methane CO&lt;sub&gt;2&lt;/sub&gt;-equivalence for the socio-economically-based metrics.
We also show that a methane CO&lt;sub&gt;2&lt;/sub&gt;-equivalence based on a pulse emission
is sufficient to inform multi-year climate policies and emissions reductions
as long as there is some degree of visibility on CO&lt;sub&gt;2&lt;/sub&gt; prices and
CO&lt;sub&gt;2&lt;/sub&gt;-equivalences.</description><pubDate>Fri, 13 Jan 2012 00:00:00 +0100</pubDate></item><item><title>Rolling stones; fast weathering of olivine in shallow seas for cost-effective CO&lt;sub&gt;2&lt;/sub&gt; capture and mitigation of global warming and ocean acidification</title><link>http://www.earth-syst-dynam-discuss.net/2/551/2011/</link><description>&lt;b&gt;Rolling stones; fast weathering of olivine in shallow seas for cost-effective CO&lt;sub&gt;2&lt;/sub&gt; capture and mitigation of global warming and ocean acidification&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 551-568, 2011&lt;br /&gt;&lt;br /&gt;Author(s): R. D. Schuiling and P. L. de Boer&lt;br /&gt;&lt;br /&gt;Human CO&lt;sub&gt;2&lt;/sub&gt; emissions may drive the Earth into a next
greenhouse state. They can be mitigated by accelerating weathering of
natural rock under the uptake of CO&lt;sub&gt;2&lt;/sub&gt;. We disprove the paradigm that
olivine weathering in nature would be a slow process, and show that it is
not needed to mill olivine to very fine, 10 μm-size grains in order to
arrive at a complete dissolution within 1–2 year. In high-energy shallow
marine environments olivine grains and reaction products on the grain
surfaces, that otherwise would greatly retard the reaction, are abraded so
that the chemical reaction is much accelerated. When kept in motion even
large olivine grains rubbing and bumping against each other quickly produce
fine clay- and silt-sized olivine particles that show a fast chemical
reaction. Spreading of olivine in the world's 2% most energetic shelf
seas can compensate a year's global CO&lt;sub&gt;2&lt;/sub&gt; emissions and counteract ocean
acidification against a price well below that of carbon credits.</description><pubDate>Tue, 06 Dec 2011 00:00:00 +0100</pubDate></item><item><title>Climate sensitivity in the Anthropocene</title><link>http://www.earth-syst-dynam-discuss.net/2/531/2011/</link><description>&lt;b&gt;Climate sensitivity in the Anthropocene&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 531-550, 2011&lt;br /&gt;&lt;br /&gt;Author(s): M. Previdi, B. G. Liepert, D. T Peteet, J. Hansen, D. J Beerling, A. J. Broccoli, S. Frolking, J. N Galloway, M. Heimann, C. Le Quéré, S. Levitus, and V. Ramaswamy&lt;br /&gt;&lt;br /&gt;Understanding the sensitivity of Earth's climate to an imposed
external forcing is one of the great challenges in science and a critical
component of efforts to avoid dangerous anthropogenic interference with the
climate system. Climate sensitivity (or equilibrium global surface warming)
to a doubling of atmospheric CO&lt;sub&gt;2&lt;/sub&gt; has long been estimated to be
about 3 °C, considering only fast climate feedbacks associated with
increases in water vapor, decreases in sea ice, and changes in clouds.
However, evidence from Earth's history suggests that slower surface albedo
feedbacks due to vegetation change and melting of Greenland and Antarctica
can come into play on the timescales of interest to humans, which could
increase the sensitivity to significantly higher values, as much as 6 °C.
Even higher sensitivity may result as present-day land and ocean carbon
sinks begin to lose their ability to sequester anthropogenic
CO&lt;sub&gt;2&lt;/sub&gt; in the coming decades. The evolving view of climate
sensitivity in the Anthropocene is therefore one in which a wider array of
Earth system feedbacks are recognized as important. Since these feedbacks
are overwhelmingly positive, the sensitivity is likely to be higher than has
traditionally been assumed.</description><pubDate>Thu, 15 Sep 2011 00:00:00 +0200</pubDate></item><item><title>Downscaling climate change scenarios for apple pest and disease modeling in Switzerland</title><link>http://www.earth-syst-dynam-discuss.net/2/493/2011/</link><description>&lt;b&gt;Downscaling climate change scenarios for apple pest and disease modeling in Switzerland&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 493-529, 2011&lt;br /&gt;&lt;br /&gt;Author(s): M. Hirschi, S. Stoeckli, M. Dubrovsky, C. Spirig, P. Calanca, M. W. Rotach, A. M. Fischer, B. Duffy, and J. Samietz&lt;br /&gt;&lt;br /&gt;As a consequence of current and projected climate change in temperate regions
of Europe, agricultural pests and diseases are expected to occur more
frequently and possibly to extend to previously not affected regions. Given
their economic and ecological relevance, detailed forecasting tools for
various pests and diseases have been developed, which model their phenology
depending on actual weather conditions and suggest management decisions on
that basis. Assessing the future risk of pest-related damages requires future
weather data at high temporal and spatial resolution. Here, we use a combined
stochastic weather generator and re-sampling procedure for producing
site-specific hourly weather series representing present and future
(1980–2009 and 2045–2074 time periods) climate conditions in Switzerland.
The climate change scenarios originate from the ENSEMBLES multi-model
projections and provide probabilistic information on future regional changes
in temperature and precipitation. Hourly weather series are produced by first
generating daily weather data for these climate scenarios and then using a
nearest neighbor re-sampling approach for creating realistic diurnal cycles.
These hourly weather series are then used for modeling the impact of climate
change on important life phases of the codling moth and on the number of
predicted infection days of fire blight. Codling moth (&lt;i&gt;Cydia pomonella&lt;/i&gt;)
 and fire blight (&lt;i&gt;Erwinia amylovora&lt;/i&gt;) are two major pest
and disease threats to apple, one of the most important commercial and rural
crops across Europe. Results for the codling moth indicate a shift in the
occurrence and duration of life phases relevant for pest control. In southern
Switzerland, a 3rd generation per season occurs only very rarely under
today's climate conditions but is projected to become normal in the
2045–2074 time period. While the potential risk for a 3rd generation is also
significantly increasing in northern Switzerland (for most stations from
roughly 1 % on average today to over 60 % in the future for the median
climate change signal of the multi-model projections), the actual risk will
critically depend on the pace of the adaptation of the codling moth with
respect to the critical photoperiod. To control this additional generation,
an intensification and prolongation of control measures (e.g., insecticides)
will be required, implying an increasing risk of pesticide resistances. For
fire blight, the projected changes in infection days are less certain due to
uncertainties in the leaf wetness approximation and the simulation of the
blooming period. Two compensating effects are projected, warmer temperatures
favoring infections are balanced by a temperature-induced advancement of the
blooming period, leading to no significant change in the number of infection
days under future climate conditions for most stations.</description><pubDate>Thu, 25 Aug 2011 00:00:00 +0200</pubDate></item><item><title>The magnitude-timescale relationship of surface temperature feedbacks in climate models</title><link>http://www.earth-syst-dynam-discuss.net/2/467/2011/</link><description>&lt;b&gt;The magnitude-timescale relationship of surface temperature feedbacks in climate models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 467-491, 2011&lt;br /&gt;&lt;br /&gt;Author(s): A. Jarvis&lt;br /&gt;&lt;br /&gt;Because of the fundamental role feedbacks play in determining the
characteristics of climate it is important we are able to specify both the
magnitude and response timescale of the feedbacks we are interested in. This
paper employs three different climate models driven to equilibrium with a
4 ×  CO&lt;sub&gt;2&lt;/sub&gt; forcing to analyze the magnitude and timescales of
surface temperature feedbacks. These models
are a global energy balance model, an intermediate complexity climate model
and a general circulation model. Rather than split surface temperature
feedback into characteristic physical processes, this paper adopts a linear
systems approach to split feedback according to their time constants and
corresponding feedback amplitudes. The analysis reveals that there is a
dominant net negative feedback realised during the first year. However, this
is partially attenuated by a spectrum of positive feedbacks for time
constants in the range 10 to 1000 years. This attenuation was composed of
two discrete phases which are attributed to the effects of ''diffusive –
mixed layer'' and ''circulatory – deep ocean'' ocean heat equilibration
processes. The diffusive equilibration was associated with time constants on
the decadal timescale and accounted for approximately 75 to 80 % of
the overall ocean heat equilibration feedback, whilst the circulatory
feedback operated on a centennial timescale and accounted for the remaining
20 to 25 % of the response. It is important to quantify these decadal
and centennial feedback processes to understand the range of climate model
projections on these longer timescales.</description><pubDate>Fri, 01 Jul 2011 00:00:00 +0200</pubDate></item><item><title>Jet stream wind power as a renewable energy resource: little power, big impacts</title><link>http://www.earth-syst-dynam-discuss.net/2/435/2011/</link><description>&lt;b&gt;Jet stream wind power as a renewable energy resource: little power, big impacts&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 435-465, 2011&lt;br /&gt;&lt;br /&gt;Author(s): L. M. Miller, F. Gans, and A. Kleidon&lt;br /&gt;&lt;br /&gt;Jet streams are regions of sustained high wind speeds in the upper atmosphere
and are seen by some as a substantial renewable energy resource. However, jet
streams are nearly geostrophic flow, that is, they result from the balance
between the pressure gradient and Coriolis force in the near absence of
friction. Therefore, jet stream motion is associated with very small
generation rates of kinetic energy to maintain the high wind velocities, and
it is this generation rate that will ultimately limit the potential use of
jet streams as a renewable energy resource. Here we estimate the maximum
limit of jet stream wind power by considering extraction of kinetic energy as
a term in the free energy balance of kinetic energy that describes the
generation, depletion, and extraction of kinetic energy. We use this balance
as the basis to quantify the maximum limit of how much kinetic energy can be
extracted sustainably from the jet streams of the global atmosphere as well
as the potential climatic impacts of its use. We first use a simple thought
experiment of geostrophic flow to demonstrate why the high wind velocities of
the jet streams are not associated with a high potential for renewable energy
generation. We then use an atmospheric general circulation model to estimate
that the maximum sustainable extraction from jet streams of the global
atmosphere is about 7.5 TW. This estimate is about 200-times less than
previous estimates and is due to the fact that the common expression for
instantaneous wind power &amp;frac12 &amp;rho; v&lt;sup&gt;3&lt;/sup&gt; merely characterizes the
transport of kinetic energy by the flow, but not the generation rate of
kinetic energy. We also find that when maximum wind power is extracted from
the jet streams, it results in significant climatic impacts due to a
substantial increase of heat transport across the jet streams in the upper
atmosphere. This results in upper atmospheric temperature differences of
&gt;20 °C, greater atmospheric stability, substantial reduction in
synoptic activity, and substantial differences in surface climate. We
conclude that jet stream wind power does not have the potential to become a
significant source of renewable energy.</description><pubDate>Fri, 17 Jun 2011 00:00:00 +0200</pubDate></item><item><title>MEP solution for a minimal climate model: success and limitation of a variational problem</title><link>http://www.earth-syst-dynam-discuss.net/2/393/2011/</link><description>&lt;b&gt;MEP solution for a minimal climate model: success and limitation of a variational problem&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 393-434, 2011&lt;br /&gt;&lt;br /&gt;Author(s): S. Pascale, J. M. Gregory, M. H. P. Ambaum, R. Tailleux, and V. Lucarini&lt;br /&gt;&lt;br /&gt;Maximum Entropy Production conjecture (MEP) is applied to a &lt;i&gt;minimal&lt;/i&gt;
four-box model of climate which accounts for both horizontal and vertical
material heat fluxes. It is shown that, under condition of fixed insolation,
a MEP solution is found with reasonably realistic temperature and heat
fluxes, thus generalising results from independent two-box horizontal or
vertical models. It is also shown that the meridional and the vertical
entropy production terms are independently involved in the maximisation and
thus MEP can be applied to each subsystem with fixed boundary conditions. We
then extend the four-box model by increasing its number of degrees of
freedom, and test its realism by comparing it with a GCM output. An
order-of-magnitude evaluation of contributions to the material entropy
production (&amp;asymp;50 mW m&lt;sup&gt;−2&lt;/sup&gt; K&lt;sup&gt;−1&lt;/sup&gt;) due to horizontal and
vertical processes within the climate system is carried out by using &lt;i&gt;ad
hoc&lt;/i&gt; temperature fields. It turns out that approximately 40 mW m&lt;sup&gt;−2&lt;/sup&gt; K&lt;sup&gt;−1&lt;/sup&gt;
is the entropy production due to vertical heat transport and 5–7 mW m&lt;sup&gt;−2&lt;/sup&gt; K&lt;sup&gt;−1&lt;/sup&gt;
to horizontal heat transport. A MEP solution is
found which is fairly realistic as far as the horizontal large scale
organisation of the surface climate is concerned whereas the vertical
structure looks to be unrealistic and presents seriously unstable features.
Finally a more general problem is investigated in which the longwave
transmissivity is varied simultaneously with the temperature. This leads to a
MEP solution characterised by a much warmer climate, with very vigorous
vertical heat fluxes, in which the atmosphere is opaque to longwave
radiation. A critical discussion about how to interpret MEP and how to apply
it in a physically correct way concludes the paper.</description><pubDate>Mon, 23 May 2011 00:00:00 +0200</pubDate></item><item><title>The energetics response to a warmer climate: relative contributions from the transient and stationary eddies</title><link>http://www.earth-syst-dynam-discuss.net/2/355/2011/</link><description>&lt;b&gt;The energetics response to a warmer climate: relative contributions from the transient and stationary eddies&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 355-391, 2011&lt;br /&gt;&lt;br /&gt;Author(s): D. Hernández-Deckers and J.-S. von Storch&lt;br /&gt;&lt;br /&gt;We use the Lorenz Energy Cycle (LEC) to evaluate changes in global
energetic activity due to CO&lt;sub&gt;2&lt;/sub&gt;-doubling in the coupled
atmosphere-ocean ECHAM5/MPI-OM model. Globally, the energetic
activity – measured as the total conversion rate of available
potential energy into kinetic energy – decreases by about 4%. This
weakening results from a dual response that consists of a
strengthening of the LEC in the upper-troposphere and a weakening in
the lower and middle troposphere. This is fully consistent with
results from a coarser resolution version of the same coupled model.
We further use our experiments to investigate the individual
contributions of the transient and stationary eddy components to the
main energetics response.
&lt;br&gt;&lt;br&gt;
The transient eddy terms have a larger contribution to the total
energetic activity than the stationary ones. We find that this is also
true in terms of their 2 × CO&lt;sub&gt;2&lt;/sub&gt;-response. Changes in the transient
eddy components determine the main energetics response, whereas the
stationary eddy components have very small contributions. Hence, the
dual response – strengthening in the upper troposphere and weakening
below – concerns mainly the transient eddy terms. We can relate
qualitatively this response to the two main features of the 2 × CO&lt;sub&gt;2&lt;/sub&gt;
warming pattern: (a) the tropical upper-tropospheric warming increases
the pole-to-equator temperature gradient – strengthening the energetic
activity above – and enhances static stability – weakening the
energetic activity below; and (b) the high-latitude surface warming
decreases the pole-to-equator temperature gradient in the lower
troposphere – weakening the energetic activity below. Despite the
small contribution from the stationary eddies to the main energetics
response, changes in stationary eddy available potential energy
(&lt;i&gt;P&lt;/i&gt;&lt;sub&gt;se&lt;/sub&gt;) reflect some features of the warming pattern: stronger
land-sea contrasts at the subtropics and weaker land-sea contrasts at
the high northern latitudes affect &lt;i&gt;P&lt;/i&gt;&lt;sub&gt;se&lt;/sub&gt; regionally, but do not
affect the global energetics response.</description><pubDate>Fri, 08 Apr 2011 00:00:00 +0200</pubDate></item><item><title>No way out? The double-bind in seeking global prosperity along with mitigated climate change</title><link>http://www.earth-syst-dynam-discuss.net/2/315/2011/</link><description>&lt;b&gt;No way out? The double-bind in seeking global prosperity along with mitigated climate change&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 315-354, 2011&lt;br /&gt;&lt;br /&gt;Author(s): T. J. Garrett&lt;br /&gt;&lt;br /&gt;In a prior study (Garrett, 2011), I introduced a simple
thermodynamics-based economic growth model. By treating civilization as a
whole, it was found that the global economy's current rate of energy
consumption can be tied through a constant to its current accumulation of
wealth. The value of the constant is λ = 9.7 ± 0.3 milliwatts per
1990 US dollar. Here, this model is coupled to a linear formulation for the
evolution of atmospheric CO&lt;sub&gt;2&lt;/sub&gt; concentrations. Despite the model's extreme
simplicity, multi-decadal hindcasts of trajectories in gross world product
(GWP) and CO&lt;sub&gt;2&lt;/sub&gt; agree closely with recent observations. Extending the model
to the future, the model implies that the well-known IPCC SRES scenarios
substantially underestimate how much CO&lt;sub&gt;2&lt;/sub&gt; levels will rise for a given
level of future economic prosperity. Instead, what is shown is that, like a
long-term natural disaster, future greenhouse warming should be expected to
retard the real growth of wealth through inflationary pressures. Because
wealth is tied to rates of energy consumption through the constant λ,
it follows that dangerous climate change should be a negative feedback on
CO&lt;sub&gt;2&lt;/sub&gt; emission rates, and therefore the ultimate extent of greenhouse
warming. Nonetheless, if atmospheric CO&lt;sub&gt;2&lt;/sub&gt; concentrations are to remain
below a &quot;dangerous&quot; level of 450 ppmv (Hansen et al., 2007), there
will have to be some combination of an unrealistically rapid rate of energy
decarbonization and a near immediate collapse of civilization wealth.
Effectively, civilization is in a double-bind. If civilization does not
collapse quickly this century, then CO&lt;sub&gt;2&lt;/sub&gt; levels will likely end up
exceeding 1000 ppmv; but, if CO&lt;sub&gt;2&lt;/sub&gt; levels rise by this much, then the
danger is that civilization will gradually tend towards collapse.</description><pubDate>Wed, 06 Apr 2011 00:00:00 +0200</pubDate></item><item><title>A simple metabolic model of glacial-interglacial energy supply to the upper ocean</title><link>http://www.earth-syst-dynam-discuss.net/2/271/2011/</link><description>&lt;b&gt;A simple metabolic model of glacial-interglacial energy supply to the upper ocean&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 271-313, 2011&lt;br /&gt;&lt;br /&gt;Author(s): J. L. Pelegrí, R. Olivella, and A. García-Olivares&lt;br /&gt;&lt;br /&gt;We use a simple two-state two-box ocean to simulate the CO&lt;sub&gt;2&lt;/sub&gt; signal
during the last four glacial-interglacial transitions in the earth system.
The model is inspired by the similarity in spatial organization and temporal
transition patterns between the earth and other complex systems, such as
mammals. The comparison identifies the earth's metabolic rate with net
autotrophic primary production in the upper ocean, sustained through new
inorganic carbon and nutrients advected from the deep ocean and organic
matter remineralized within the upper ocean. We view the
glacial-interglacial transition as a switch of the upper ocean from a basal
to an enhanced metabolic state, with energy supply initially relying on the
remineralization of the local organic sources and the eventual steady state
resulting from the increased advective supply of inorganic deep sources.
During the interglacial-glacial transition the opposite occurs, with an
initial excess of advective supply and primary production that allows the replenishment of the
upper-ocean organic storages. We set the relative change in energy supply
from the CO&lt;sub&gt;2&lt;/sub&gt; signal and use genetic algorithms to explore the
sensitivity of the model output to both the basal recirculation rate and the
intensity-timing of the maximum recirculation rate. The model is capable of
reproducing quite well the long-term oscillations, as shown by correlations
with observations typically about 0.8. The dominant time scale for each
cycle ranges between about 40 and 45 kyr, close to the 41 kyr average
obliquity astronomical period, and the deep-ocean recirculation rate
increases between one and two orders of magnitude from glacial to
interglacial periods.</description><pubDate>Tue, 22 Mar 2011 00:00:00 +0100</pubDate></item><item><title>Climate change, in the framework of the constructal law</title><link>http://www.earth-syst-dynam-discuss.net/2/241/2011/</link><description>&lt;b&gt;Climate change, in the framework of the constructal law&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 241-270, 2011&lt;br /&gt;&lt;br /&gt;Author(s): M. Clausse, F. Meunier, A. H. Reis, and A. Bejan&lt;br /&gt;&lt;br /&gt;Here we present a simple and transparent alternative to the complex models
of Earth thermal behavior under time-changing conditions. We show the
one-to-one relationship between changes in atmospheric properties and
time-dependent changes in temperature and its distribution on Earth. The
model accounts for convection and radiation, thermal inertia and changes in
albedo (&amp;rho;) and greenhouse factor (γ). The constructal law is
used as the principle that governs the evolution of flow configuration in
time, and provides closure for the equations that describe the model. In the
first part of the paper, the predictions are tested against the current
thermal state of Earth. Next, the model showed that for two time-dependent
scenarios, (&amp;delta;&amp;rho; = 0.002; &amp;delta;&amp;gamma; = 0.011) and
(&amp;delta;&amp;rho; = 0.002; &amp;delta;&amp;gamma; = 0.005) the predicted
equatorial and polar temperature increases and the time scales are
(&amp;Delta;&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;H&lt;/sub&gt; = 1.16 K; &amp;Delta;&lt;i&gt;T&lt;/i&gt;&lt;sub&gt;L&lt;/sub&gt; = 1.11 K; 104 years)
and (0.41 K; 0.41 K; 57 years), respectively. In the second part, a continuous model of
temperature variation was used to predict the thermal response of the
Earth's surface for changes bounded by &amp;delta;&amp;rho; = &amp;delta;&amp;gamma;
and &amp;delta;&amp;rho; = &amp;minus;&amp;delta;&amp;gamma;. The results
show that the global warming amplitudes and time scales are consistent with
those obtained for &amp;delta;&amp;rho; = 0.002 and &amp;delta;&amp;gamma; = 0.005.
The poleward heat current reaches its maximum in the vicinity of 35°
latitude, accounting for the position of the Ferrel cell between the Hadley
and Polar Cells.</description><pubDate>Mon, 07 Mar 2011 00:00:00 +0100</pubDate></item><item><title>Geologic constraints on earth system sensitivity to CO&lt;sub&gt;2&lt;/sub&gt; during the Cretaceous and early Paleogene</title><link>http://www.earth-syst-dynam-discuss.net/2/211/2011/</link><description>&lt;b&gt;Geologic constraints on earth system sensitivity to CO&lt;sub&gt;2&lt;/sub&gt; during the Cretaceous and early Paleogene&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 211-240, 2011&lt;br /&gt;&lt;br /&gt;Author(s): D. L. Royer, M. Pagani, and D. J. Beerling&lt;br /&gt;&lt;br /&gt;Earth system sensitivity (ESS) is the long-term (&gt;10&lt;sup&gt;3&lt;/sup&gt; yr) equilibrium temperature
response to doubled CO&lt;sub&gt;2&lt;/sub&gt;. ESS has climate policy implications because
global temperatures are not expected to decline appreciably for at least
10&lt;sup&gt;3&lt;/sup&gt; yr, even if anthropogenic greenhouse-gas emissions drop to zero. We
report quantitative ESS estimates of 3 °C or higher for much of the
Cretaceous and early Paleogene based on paleo-reconstructions of CO&lt;sub&gt;2&lt;/sub&gt;
and temperature. These estimates are generally higher than climate
sensitivities simulated from global climate models for the same ancient
periods (~3 °C). We conclude that climate models do not capture
the full suite of positive climate feedbacks during greenhouse worlds. These
absent feedbacks are probably related to clouds, trace greenhouse gases,
seasonal snow cover, and/or vegetation, especially in polar regions. Continued
warming in the coming decades as anthropogenic greenhouse gases accumulate
in the atmosphere ensures that characterizing and quantifying these positive
climate feedbacks will become a scientific challenge of increasing priority.</description><pubDate>Thu, 03 Mar 2011 00:00:00 +0100</pubDate></item><item><title>Soil temperature response to 21st century global warming: the role of and some implications for peat carbon in thawing permafrost soils in North America</title><link>http://www.earth-syst-dynam-discuss.net/2/161/2011/</link><description>&lt;b&gt;Soil temperature response to 21st century global warming: the role of and some implications for peat carbon in thawing permafrost soils in North America&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 161-210, 2011&lt;br /&gt;&lt;br /&gt;Author(s): D. Wisser, S. Marchenko, J. Talbot, C. Treat, and S. Frolking&lt;br /&gt;&lt;br /&gt;Northern peatlands contain a large terrestrial carbon pool that plays an
important role in the Earth's carbon cycle. A considerable fraction of this
carbon pool is currently in permafrost and is biogeochemically relatively
inert; this will change with increasing soil temperatures as a result of
climate warming in the 21st century. We use a geospatially explicit
representation of peat areas and peat depth from a recently-compiled
database and a geothermal model to estimate northern North America soil
temperature responses to predicted changes in air temperature. We find that,
despite a widespread decline in the areas classified as permafrost, soil
temperatures in peatlands respond more slowly to increases in air
temperature owing to the insulating properties of peat. We estimate that an
additional 670 km&lt;sup&gt;3&lt;/sup&gt; of peat soils in North America, containing
~33 Pg C, could be seasonally thawed by the end of the century, representing
~20% of the total peat volume in Alaska and Canada. Warming
conditions result in a lengthening of the soil thaw period by ~40
days, averaged over the model domain. These changes have potentially
important implications for the carbon balance of peat soils.</description><pubDate>Thu, 17 Feb 2011 00:00:00 +0100</pubDate></item><item><title>Role of volcanic forcing on future global carbon cycle</title><link>http://www.earth-syst-dynam-discuss.net/2/133/2011/</link><description>&lt;b&gt;Role of volcanic forcing on future global carbon cycle&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 133-159, 2011&lt;br /&gt;&lt;br /&gt;Author(s): J. F. Tjiputra and O. H. Otterå&lt;br /&gt;&lt;br /&gt;Using a fully coupled global climate-carbon cycle model, we assess the
potential role of volcanic eruptions on future projection of climate change
and its associated carbon cycle feedback. The volcanic-like forcings are
applied together with business-as-usual IPCC-A2 carbon emissions scenario. We
show that very large volcanic eruptions similar to Tambora lead to short-term
substantial global cooling. However, over a long period, smaller but more
frequent eruptions, such as Pinatubo, would have a stronger impact on future
climate change. In a scenario where the volcanic external forcings are
prescribed with a five-year frequency, the induced cooling immediately lower
the global temperature by more than one degree before return to the warming
trend. Therefore, the climate change is approximately delayed by several
decades and by the end of the 21st century, the warming is still below two
degrees when compared to the present day period. The cooler climate reduces
the terrestrial heterotrophic respiration in the northern high latitude and
increases net primary production in the tropics, which contributes to more
than 45% increase in accumulated carbon uptake over land. The increased
solubility of CO&lt;sub&gt;2&lt;/sub&gt; gas in seawater associated with cooler SST is offset by
reduced CO&lt;sub&gt;2&lt;/sub&gt; partial pressure gradient between ocean and atmosphere, which
results in small changes in net ocean carbon uptake. Similarly, there is
nearly no change in the seawater buffer capacity simulated between the
different volcanic scenarios. Our study shows that even in the relatively
extreme scenario where large volcanic eruptions occur every five-years
period, the induced cooling only leads to a reduction of 46 ppmv atmospheric
CO&lt;sub&gt;2&lt;/sub&gt; concentration as compared to the reference projection of 878 ppmv, at
the end of the 21st century. With respect to sulphur injection geoengineering
method, our study suggest that small scale but frequent mitigation is more
efficient than the opposite. Moreover, the longer we delay, the more
difficult it would be to counteract climate change.</description><pubDate>Wed, 16 Feb 2011 00:00:00 +0100</pubDate></item><item><title>Entropy production of soil hydrological processes and its maximisation</title><link>http://www.earth-syst-dynam-discuss.net/2/105/2011/</link><description>&lt;b&gt;Entropy production of soil hydrological processes and its maximisation&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 105-132, 2011&lt;br /&gt;&lt;br /&gt;Author(s): P. Porada, A. Kleidon, and S. J. Schymanski&lt;br /&gt;&lt;br /&gt;Hydrological processes are irreversible and produce entropy. Hence, the
framework of non-equilibrium thermodynamics is used here to describe them
mathematically. This means flows of water are written as functions of
gradients in the gravitational and chemical potential of water between two
parts of the hydrological system. Such a framework facilitates a consistent
thermodynamic representation of the hydrological processes in the model.
Furthermore, it allows for the calculation of the entropy production
associated with a flow of water, which is proportional to the product of
gradient and flow. Thus, an entropy budget of the hydrological cycle at the
land surface is quantified, illustrating the contribution of different
processes to the overall entropy production. Moreover, the proposed Principle
of Maximum Entropy Production (MEP) can be applied to the model. This means,
unknown parameters can be determined by setting them to values which lead to
a maximisation of the entropy production in the model. The model used in this
study is parametrised according to MEP and evaluated by means of several
observational datasets describing terrestrial fluxes of water and carbon. The
model reproduces the data with good accuracy which is a promising result with
regard to the application of MEP to hydrological processes at the land
surface.</description><pubDate>Fri, 28 Jan 2011 00:00:00 +0100</pubDate></item><item><title>Quantifying the thermodynamic entropy budget of the land surface: is this useful?</title><link>http://www.earth-syst-dynam-discuss.net/2/71/2011/</link><description>&lt;b&gt;Quantifying the thermodynamic entropy budget of the land surface: is this useful?&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 71-103, 2011&lt;br /&gt;&lt;br /&gt;Author(s): N. A. Brunsell, S. J. Schymanski, and A. Kleidon&lt;br /&gt;&lt;br /&gt;As a system is moved away from a state of thermodynamic equilibrium, spatial and temporal heterogeneity
is induced. A possible methodology to assess these impacts is to examine the thermodynamic
entropy budget and assess the role of entropy production and transfer between the surface
and the atmosphere. Here, we adopted this thermodynamic framework to examine the implications of
changing vegetation fractional cover on land surface energy exchange processes using the NOAH land surface
model and eddy covariance observations. Simulations that varied the relative fraction of vegetation were used
to calculate the resultant entropy budget as a function of
fraction of vegetation. Results showed that increasing vegetation fraction increases entropy production by the
land surface while decreasing the overall entropy budget (the rate of change in entropy at the surface). This is
accomplished largely via simultaneous increase in the entropy production associated with the absorption of
solar radiation and a decline in the Bowen ratio (ratio of sensible to latent heat flux), which leads to increasing
the entropy export associated with the latent heat flux during the daylight hours and dominated by entropy
transfer associated with sensible heat and soil heat fluxes during the nighttime hours.
Eddy covariance observations also show that the entropy
production has a consistent sensitivity to land cover, while the overall entropy budget appears most related to the
net radiation at the surface. This implies that quantifying the thermodynamic entropy budget and entropy
production is a useful metric for assessing biosphere-atmosphere-hydrosphere system interactions.</description><pubDate>Wed, 26 Jan 2011 00:00:00 +0100</pubDate></item><item><title>Spectral solar irradiance and its entropic effect on Earth's climate</title><link>http://www.earth-syst-dynam-discuss.net/2/45/2011/</link><description>&lt;b&gt;Spectral solar irradiance and its entropic effect on Earth's climate&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 45-70, 2011&lt;br /&gt;&lt;br /&gt;Author(s): W. Wu, Y. Liu, and G. Wen&lt;br /&gt;&lt;br /&gt;The high-resolution measurements of the spectral solar irradiance at the top
of the Earth's atmosphere by the Solar Radiation and Climate Experiment
(SORCE) satellite suggest significant deviation of solar radiation from the
commonly assumed blackbody radiation. Here, we use these spectral irradiance
measurements to estimate the Earth's incident solar radiation entropy flux,
and examine the importance of a proper estimation approach. The Earth's
incident solar radiation entropy flux estimated by directly applying the
observed spectral solar irradiance into the most accurate Planck expression
is compared with that estimated with a conventional approach that uses the
Sun's brightness temperature under the assumption of a blackbody Sun. The
globally averaged non-blackbody incident solar radiation entropy flux at the
top of the Earth's atmosphere equals 0.31 W m&lt;sup&gt;−2&lt;/sup&gt; K&lt;sup&gt;−1&lt;/sup&gt;. This value is
about 4 times larger than that estimated from the conventional blackbody
approach, with the difference comparable to the typical value of the entropy
production rate associated with atmospheric latent heat process. Further
analysis reveals that the decrease of spectral solar radiation entropy flux
with radiation traveling distance, unlike the decrease of spectral solar
radiation energy flux with radiation traveling distance, is wavelength
dependent, and that the difference between the two estimates can be
attributed to the fact that the conventional approach ignores the influence
of radiation traveling distance on the spectral solar radiation entropy
flux. Moreover, sensitivity study further shows that the distribution of
top-of-atmosphere spectral solar irradiance could significantly impact the
magnitude of the estimated Earth's incident solar radiation entropy flux.
These results together suggest that the spectral distribution of incident
solar radiation is critical for determining the Earth's incident solar
radiation entropy flux, and thus the Earth's climate.</description><pubDate>Tue, 25 Jan 2011 00:00:00 +0100</pubDate></item><item><title>Differences and implications in biogeochemistry from maximizing entropy production locally versus globally</title><link>http://www.earth-syst-dynam-discuss.net/2/1/2011/</link><description>&lt;b&gt;Differences and implications in biogeochemistry from maximizing entropy production locally versus globally&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics Discussions, 2, 1-44, 2011&lt;br /&gt;&lt;br /&gt;Author(s): J. J. Vallino&lt;br /&gt;&lt;br /&gt;In this manuscript we investigate the use of the maximum entropy production
(MEP) principle for modeling biogeochemical processes that are catalyzed by
living systems. Because of novelties introduced by the MEP approach, many
questions need to be answered and techniques developed in the application of
MEP to describe biological systems that are responsible for energy and mass
transformations on a planetary scale. In previous work we introduce the
importance of integrating entropy production over time to distinguish
abiotic from biotic processes under transient conditions. Here we
investigate the ramifications of modeling biological systems involving one
or more spatial dimensions. When modeling systems with spatial dimensions,
entropy production can be maximized either locally at each point in space
asynchronously or globally over the system domain synchronously. We use a
simple two-box model inspired by two-layer ocean models to illustrate the
differences in local versus global entropy maximization. Synthesis and
oxidation of biological structure is modeled using two autocatalytic
reactions that account for changes in community kinetics using a single
parameter each. Our results show that entropy production can be increased if
maximized over the system domain rather than locally, which has important
implications regarding how biological systems organize and supports the
hypothesis for multiple levels of selection and cooperation in biology for
the dissipation of free energy.</description><pubDate>Wed, 19 Jan 2011 00:00:00 +0100</pubDate></item></channel></rss>
