<?xml version="1.0" encoding="utf-8"?><!DOCTYPE rss PUBLIC "-//Netscape Communications//DTD RSS 0.91//EN" "http://my.netscape.com/publish/formats/rss-0.91.dtd"><rss version="0.91"><channel><title>ESD - Latest Articles</title><link>http://www.earth-syst-dynam.net/</link> <description>Earth System Dynamics Latest Articles</description><language>en</language><item><title>Vertical and horizontal processes in the global atmosphere and the maximum entropy production conjecture</title><link>http://www.earth-syst-dynam.net/3/19/2012/</link><description>&lt;b&gt;Vertical and horizontal processes in the global atmosphere and the maximum entropy production conjecture&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 3, 19-32, 2012&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;The objective of this paper is to reconsider the Maximum Entropy Production
conjecture (MEP) in the context of a very simple two-dimensional
zonal-vertical climate model able to represent the total material entropy
production due at the same time to both horizontal and vertical heat fluxes.
MEP is applied first to a simple 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 resolution, and compare it with GCM output. A MEP solution is
found which is fairly realistic as far as the horizontal large scale
organisation of the climate is concerned whereas the vertical structure looks
to be unrealistic and presents seriously unstable features. This study
suggest that the thermal meridional structure of the atmosphere is predicted
fairly well by MEP once the insolation is given but the vertical structure of
the atmosphere cannot be predicted satisfactorily by MEP unless constraints
are imposed to represent the determination of longwave absorption by
water vapour and clouds as a function of the state of the climate.
Furthermore an order-of-magnitude estimate of contributions to the material
entropy production due to horizontal and vertical processes within the
climate system is provided by using two different methods. In both cases we
found that approximately 40 mW m&lt;sup&gt;−2&lt;/sup&gt; K&lt;sup&gt;−1&lt;/sup&gt; of material entropy
production is 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.</description><pubDate>Thu, 19 Jan 2012 00:00:00 +0100</pubDate></item><item><title>No way out? The double-bind in seeking global prosperity alongside mitigated climate change</title><link>http://www.earth-syst-dynam.net/3/1/2012/</link><description>&lt;b&gt;No way out? The double-bind in seeking global prosperity alongside mitigated climate change&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 3, 1-17, 2012&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 economic growth model designed to be consistent
with general thermodynamic laws. Unlike traditional
economic models, civilization is viewed only as a
well-mixed global whole with no distinction made between individual nations,
economic sectors, labor, or capital investments. At the model core is a
hypothesis that the global economy's current rate of primary energy
consumption is tied through a constant to a very general representation of
its historically accumulated wealth. Observations support this hypothesis,
and indicate that the constant's value is λ = 9.7 ± 0.3
milliwatts per 1990 US dollar. It is this link that allows for treatment of
seemingly complex economic systems as simple physical systems. Here, this
growth model is coupled to a linear formulation for the evolution of globally
well-mixed atmospheric CO&lt;sub&gt;2&lt;/sub&gt; concentrations. While very simple, the
coupled model provides faithful multi-decadal hindcasts of trajectories in
gross world product (GWP) and CO&lt;sub&gt;2&lt;/sub&gt;. Extending the model to the future,
the model suggests 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. For one, global CO&lt;sub&gt;2&lt;/sub&gt; emission rates cannot be
decoupled from wealth through efficiency gains. For another, like a long-term
natural disaster, future greenhouse warming can be expected to act as an
inflationary drag on the real growth of global wealth. For atmospheric
CO&lt;sub&gt;2&lt;/sub&gt; concentrations to remain below a &quot;dangerous&quot; level of 450 ppmv
(Hansen et al., 2007), model forecasts suggest that there will have to
be some combination of an unrealistically rapid rate of energy
decarbonization and nearly immediate reductions in global civilization
wealth. Effectively, it appears that civilization may be 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 risk is that civilization will gradually tend towards
collapse.</description><pubDate>Thu, 05 Jan 2012 00:00:00 +0100</pubDate></item><item><title>The magnitudes and timescales of global mean surface temperature feedbacks in climate models</title><link>http://www.earth-syst-dynam.net/2/213/2011/</link><description>&lt;b&gt;The magnitudes and timescales of global mean surface temperature feedbacks in climate models&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 213-221, 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 response
of surface temperature to perturbations in radiative forcing, it is
important we understand the dynamic characteristics of these feedbacks.
Rather than attribute the aggregate surface temperature feedback to
particular physical processes, this paper adopts a linear systems approach
to investigate the partitioning with respect to the timescale of the
feedbacks regulating global mean surface temperature in climate models. The
analysis reveals that there is a dominant net negative feedback realised on
an annual timescale and that this is partially attenuated by a spectrum of
positive feedbacks with characteristic timescales in the range 10 to 1000 yr. This attenuation was composed of two discrete phases which are
attributed to the equilibration of &quot;diffusive &amp;ndash; mixed layer&quot; and
&quot;circulatory &amp;ndash; deep ocean&quot; ocean heat uptake. The diffusive equilibration
was associated with time constants on the decadal timescale and accounted
for approximately 75 to 80 percent of the overall ocean heat feedback,
whilst the circulatory equilibration operated on a centennial timescale and
accounted for the remaining 20 to 25 percent of the response. This suggests
that the dynamics of the transient ocean heat uptake feedback first
discussed by Baker and Roe (2009) tends to be dominated by loss of diffusive
heat uptake in climate models, rather than circulatory deep ocean heat
equilibration.</description><pubDate>Thu, 15 Dec 2011 00:00:00 +0100</pubDate></item><item><title>Jet stream wind power as a renewable energy resource: little power, big impacts</title><link>http://www.earth-syst-dynam.net/2/201/2011/</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, 2, 201-212, 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 &lt;span style=&quot;border-bottom: 1px solid #000; vertical-align: 50%;
font-size: .7em; color: #000;&quot;&gt;1&lt;/span&gt;&lt;span style=&quot;margin-left: -0.5em;
margin-right: .5em; vertical-align: -15%; font-size: .7em; color:
#000;&quot;&gt;2&lt;/span&gt; &lt;i&gt;&amp;rho;&lt;/i&gt;&lt;i&gt;v&lt;/i&gt;&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 &amp;deg;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>Tue, 29 Nov 2011 00:00:00 +0100</pubDate></item><item><title>Emulating Atlantic overturning strength for low emission scenarios: consequences for sea-level rise along the North American east coast</title><link>http://www.earth-syst-dynam.net/2/191/2011/</link><description>&lt;b&gt;Emulating Atlantic overturning strength for low emission scenarios: consequences for sea-level rise along the North American east coast&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 191-200, 2011&lt;br /&gt;&lt;br /&gt;Author(s): C. F. Schleussner, K. Frieler, M. Meinshausen, J. Yin, and A. Levermann&lt;br /&gt;&lt;br /&gt;In order to provide probabilistic projections of the future evolution of the
Atlantic Meridional Overturning Circulation (AMOC), we calibrated a simple
Stommel-type box model to emulate the output of fully coupled
three-dimensional atmosphere-ocean general circulation models (AOGCMs) of the
Coupled Model Intercomparison Project (CMIP). Based on this calibration to
idealised global warming scenarios with and without interactive
atmosphere-ocean fluxes and freshwater perturbation simulations, we project
the future evolution of the AMOC mean strength within the covered calibration range for the
lower two Representative Concentration Pathways (RCPs) until 2100 obtained
from the reduced complexity carbon cycle-climate
model MAGICC 6. For RCP3-PD with a global mean temperature median below 1.0 °C
warming relative to the year 2000, we project an ensemble median weakening of up to
11% compared to 22% under RCP4.5 with a warming median up to 1.9 °C over
the 21st century. Additional Greenland meltwater of 10 and 20 cm of global
sea-level rise equivalent further weakens the AMOC by about 4.5 and 10%,
respectively. By combining our outcome with a multi-model sea-level rise
study we project a dynamic sea-level rise along the New York City coastline
of 4 cm for the RCP3-PD and of 8 cm for the RCP4.5 scenario over the 21st
century. We estimate the total steric and dynamic sea-level rise for New York
City to be about 24 cm until 2100 for the RCP3-PD scenario, which can hold as
a lower bound for sea-level rise projections in this region,  as it does not
include ice sheet and mountain glacier contributions.</description><pubDate>Wed, 28 Sep 2011 00:00:00 +0200</pubDate></item><item><title>Entropy production of soil hydrological processes and its maximisation</title><link>http://www.earth-syst-dynam.net/2/179/2011/</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, 2, 179-190, 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, 02 Sep 2011 00:00:00 +0200</pubDate></item><item><title>A multi-model ensemble method that combines imperfect models through learning</title><link>http://www.earth-syst-dynam.net/2/161/2011/</link><description>&lt;b&gt;A multi-model ensemble method that combines imperfect models through learning&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 161-177, 2011&lt;br /&gt;&lt;br /&gt;Author(s): L. A. van den Berge, F. M. Selten, W. Wiegerinck, and G. S. Duane&lt;br /&gt;&lt;br /&gt;In the current multi-model ensemble approach climate model simulations are
combined a posteriori. In the method of this study the models in the ensemble
exchange information during simulations and learn from historical
observations to combine their strengths into a best representation of the
observed climate. The method is developed and tested in the context of small
chaotic dynamical systems, like the Lorenz 63 system. Imperfect models are
created by perturbing the standard parameter values. Three imperfect models
are combined into one super-model, through the introduction of connections
between the model equations. The connection coefficients are learned from
data from the unperturbed model, that is regarded as the truth.
&lt;br&gt;&lt;br&gt;
The main result of this study is that after learning the super-model is a
very good approximation to the truth, much better than each imperfect model
separately. These illustrative examples suggest that the super-modeling
approach is a promising strategy to improve weather and climate simulations.</description><pubDate>Thu, 30 Jun 2011 00:00:00 +0200</pubDate></item><item><title>Towards understanding how surface life can affect interior geological processes: a non-equilibrium thermodynamics approach</title><link>http://www.earth-syst-dynam.net/2/139/2011/</link><description>&lt;b&gt;Towards understanding how surface life can affect interior geological processes: a non-equilibrium thermodynamics approach&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 139-160, 2011&lt;br /&gt;&lt;br /&gt;Author(s): J. G. Dyke, F. Gans, and A. Kleidon&lt;br /&gt;&lt;br /&gt;Life has significantly altered the Earth's atmosphere, oceans and crust. To
what extent has it also affected interior geological processes? To address
this question, three models of geological processes are formulated: mantle
convection, continental crust uplift and erosion and oceanic crust recycling.
These processes are characterised as non-equilibrium thermodynamic systems.
Their states of disequilibrium are maintained by the power generated from the
dissipation of energy from the interior of the Earth. Altering the thickness
of continental crust via weathering and erosion affects the upper mantle
temperature which leads to changes in rates of oceanic crust recycling and
consequently rates of outgassing of carbon dioxide into the atmosphere.
Estimates for the power generated by various elements in the Earth system are
shown. This includes, inter alia, surface life generation of 264 TW of
power, much greater than those of geological processes such as mantle
convection at 12 TW. This high power results from life's ability to harvest
energy directly from the sun. Life need only utilise a small fraction of the
generated free chemical energy for geochemical transformations at the
surface, such as affecting rates of weathering and erosion of continental
rocks, in order to affect interior, geological processes. Consequently when
assessing the effects of life on Earth, and potentially any planet with a
significant biosphere, dynamical models may be required that better capture
the coupled nature of biologically-mediated surface and interior processes.</description><pubDate>Tue, 28 Jun 2011 00:00:00 +0200</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.net/2/121/2011/</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, 2, 121-138, 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>Fri, 24 Jun 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.net/2/105/2011/</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, 2, 105-120, 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>Tue, 21 Jun 2011 00:00:00 +0200</pubDate></item><item><title>Quantifying the thermodynamic entropy budget of the land surface: is this useful?</title><link>http://www.earth-syst-dynam.net/2/87/2011/</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, 2, 87-103, 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,
however with a large variance. This implies that quantifying the
thermodynamic entropy budget and entropy production is a useful metric for
assessing biosphere-atmosphere-hydrosphere system interactions.</description><pubDate>Mon, 20 Jun 2011 00:00:00 +0200</pubDate></item><item><title>Differences and implications in biogeochemistry from maximizing entropy production locally versus globally</title><link>http://www.earth-syst-dynam.net/2/69/2011/</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, 2, 69-85, 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 over space, 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>Fri, 17 Jun 2011 00:00:00 +0200</pubDate></item><item><title>Role of volcanic forcing on future global carbon cycle</title><link>http://www.earth-syst-dynam.net/2/53/2011/</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, 2, 53-67, 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 a 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
eruptions similar to Pinatubo in amplitude, but set to occur frequently, 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 it returns 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. Our climate-carbon feedback analysis shows that future volcanic
eruptions induce positive feedbacks (i.e., more carbon sink) on both the
terrestrial and oceanic carbon cycle. The feedback signal on the ocean is
consistently smaller than the terrestrial counterpart and the feedback
strength is proportionally related to the frequency of the volcanic eruption
events. 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 a reduced CO&lt;sub&gt;2&lt;/sub&gt; partial pressure
gradient between the ocean and the 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 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.</description><pubDate>Thu, 16 Jun 2011 00:00:00 +0200</pubDate></item><item><title>Thermodynamic dissipation theory for the origin of life</title><link>http://www.earth-syst-dynam.net/2/37/2011/</link><description>&lt;b&gt;Thermodynamic dissipation theory for the origin of life&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 37-51, 2011&lt;br /&gt;&lt;br /&gt;Author(s): K. Michaelian&lt;br /&gt;&lt;br /&gt;Understanding the thermodynamic function of life may shed light on its
origin. Life, as are all irreversible processes, is contingent on entropy
production. Entropy production is a measure of the rate of the tendency of
Nature to explore available microstates. The most important irreversible
process generating entropy in the biosphere and, thus, facilitating this
exploration, is the absorption and transformation of sunlight into heat.
Here we hypothesize that life began, and persists today, as a catalyst for
the absorption and dissipation of sunlight on the surface of Archean seas.
The resulting heat could then be efficiently harvested by other irreversible
processes such as the water cycle, hurricanes, and ocean and wind currents.
RNA and DNA are the most efficient of all known molecules for absorbing the
intense ultraviolet light that penetrated the dense early atmosphere and are
remarkably rapid in transforming this light into heat in the presence of
liquid water. From this perspective, the origin and evolution of life,
inseparable from water and the water cycle, can be understood as resulting
from the natural thermodynamic imperative of increasing the entropy
production of the Earth in its interaction with its solar environment. A
mechanism is proposed for the reproduction of RNA and DNA without the need
for enzymes, promoted instead through UV light dissipation and diurnal temperature
cycling of the Archean sea-surface.</description><pubDate>Fri, 11 Mar 2011 00:00:00 +0100</pubDate></item><item><title>Climate change under a scenario near 1.5 °C of global warming: monsoon intensification, ocean warming and steric sea level rise</title><link>http://www.earth-syst-dynam.net/2/25/2011/</link><description>&lt;b&gt;Climate change under a scenario near 1.5 °C of global warming: monsoon intensification, ocean warming and steric sea level rise&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 25-35, 2011&lt;br /&gt;&lt;br /&gt;Author(s): J. Schewe, A. Levermann, and M. Meinshausen&lt;br /&gt;&lt;br /&gt;We present climatic consequences of the Representative Concentration Pathways
(RCPs) using the coupled climate model CLIM&lt;i&gt;BER&lt;/i&gt;-3α, which contains a
statistical-dynamical atmosphere and a three-dimensional ocean model. We
compare those with emulations of 19 state-of-the-art atmosphere-ocean general
circulation models (AOGCM) using MAGICC6. The RCPs are designed as standard
scenarios for the forthcoming IPCC Fifth Assessment Report to span the full
range of future greenhouse gas (GHG) concentrations pathways currently
discussed. The lowest of the RCP scenarios, RCP3-PD, is projected in
CLIM&lt;i&gt;BER&lt;/i&gt;-3α to imply a maximal warming by the middle of the 21st
century slightly above 1.5 °C and a slow decline of temperatures
thereafter, approaching today's level by 2500. We identify two mechanisms
that slow down global cooling after GHG concentrations peak: The known
inertia induced by mixing-related oceanic heat uptake; and a change in
oceanic convection that enhances ocean heat loss in high latitudes, reducing
the surface cooling rate by almost 50%. Steric sea level rise under the
RCP3-PD scenario continues for 200 years after the peak in surface air
temperatures, stabilizing around 2250 at 30 cm. This contrasts with around
1.3 m of steric sea level rise by 2250, and 2 m by 2500, under the highest
scenario, RCP8.5. Maximum oceanic warming at intermediate depth (300–800 m)
is found to exceed that of the sea surface by the second half of the
21st century under RCP3-PD. This intermediate-depth
warming persists for centuries even after surface temperatures have returned
to present-day values, with potential consequences for marine ecosystems,
oceanic methane hydrates, and ice-shelf stability. Due to an enhanced
land-ocean temperature contrast, all scenarios yield an intensification of
monsoon rainfall under global warming.</description><pubDate>Tue, 08 Mar 2011 00:00:00 +0100</pubDate></item><item><title>Entropy production and multiple equilibria: the case of the ice-albedo feedback</title><link>http://www.earth-syst-dynam.net/2/13/2011/</link><description>&lt;b&gt;Entropy production and multiple equilibria: the case of the ice-albedo feedback&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 13-23, 2011&lt;br /&gt;&lt;br /&gt;Author(s): C. Herbert, D. Paillard, and B. Dubrulle&lt;br /&gt;&lt;br /&gt;Nonlinear feedbacks in the Earth System provide mechanisms that can prove
very useful in understanding complex dynamics with relatively simple
concepts. For example, the temperature and the ice cover of the planet are
linked in a positive feedback which gives birth to multiple equilibria for
some values of the solar constant: fully ice-covered Earth, ice-free Earth
and an intermediate unstable solution. In this study, we show an analogy
between a classical dynamical system approach to this problem and a Maximum
Entropy Production (MEP) principle view, and we suggest a glimpse on how to
reconcile MEP with the time evolution of a variable. It enables us in
particular to resolve the question of the stability of the entropy production
maxima. We also compare the surface heat flux obtained with MEP and with the
bulk-aerodynamic formula.</description><pubDate>Wed, 23 Feb 2011 00:00:00 +0100</pubDate></item><item><title>Estimating maximum global land surface wind power extractability and associated climatic consequences</title><link>http://www.earth-syst-dynam.net/2/1/2011/</link><description>&lt;b&gt;Estimating maximum global land surface wind power extractability and associated climatic consequences&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 2, 1-12, 2011&lt;br /&gt;&lt;br /&gt;Author(s): L. M. Miller, F. Gans, and A. Kleidon&lt;br /&gt;&lt;br /&gt;The availability of wind power for renewable energy extraction is ultimately
limited by how much kinetic energy is generated by natural processes within
the Earth system and by fundamental limits of how much of the wind power can
be extracted. Here we use these considerations to provide a maximum estimate
of wind power availability over land. We use several different methods.
First, we outline the processes associated with wind power generation and
extraction with a simple power transfer hierarchy based on the assumption
that available wind power will not geographically vary with increased
extraction for an estimate of 68 TW. Second, we set up a simple momentum balance model to estimate maximum
extractability which we then apply to reanalysis climate data, yielding an
estimate of 21 TW. Third, we perform general circulation model simulations in
which we extract different amounts of momentum from the atmospheric boundary
layer to obtain a maximum estimate of how much power can be extracted,
yielding 18–34 TW. These three methods consistently yield maximum estimates
in the range of 18–68 TW and are notably less than recent estimates that
claim abundant wind power availability. Furthermore, we show with the general
circulation model simulations that some climatic effects at maximum wind
power extraction are similar in magnitude to those associated with a doubling
of atmospheric CO&lt;sub&gt;2&lt;/sub&gt;. We conclude that in order to understand fundamental
limits to renewable energy resources, as well as the impacts of their
utilization, it is imperative to use a &quot;top-down&quot; thermodynamic Earth system
perspective, rather than the more common &quot;bottom-up&quot; engineering approach.</description><pubDate>Fri, 11 Feb 2011 00:00:00 +0100</pubDate></item><item><title>A new model of Holocene peatland net primary production, decomposition, water balance, and peat accumulation</title><link>http://www.earth-syst-dynam.net/1/1/2010/</link><description>&lt;b&gt;A new model of Holocene peatland net primary production, decomposition, water balance, and peat accumulation&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;Earth System Dynamics, 1, 1-21, 2010&lt;br /&gt;&lt;br /&gt;Author(s): S. Frolking, N. T. Roulet, E. Tuittila, J. L. Bubier, A. Quillet, J. Talbot, and P. J. H. Richard&lt;br /&gt;&lt;br /&gt;Peatland carbon and water cycling are tightly coupled, so dynamic modeling
of peat accumulation over decades to millennia should account for
carbon-water feedbacks. We present initial results from a new simulation
model of long-term peat accumulation, evaluated at a well-studied temperate
bog in Ontario, Canada. The Holocene Peat Model (HPM) determines vegetation
community composition dynamics and annual net primary productivity based on
peat depth (as a proxy for nutrients and acidity) and water table depth.
Annual peat (carbon) accumulation is the net balance above- and below-ground
productivity and litter/peat decomposition – a function of peat hydrology
(controlling depth to and degree of anoxia). Peat bulk density is simulated
as a function of degree of humification, and affects the water balance
through its influence on both the growth rate of the peat column and on peat
hydraulic conductivity and the capacity to shed water. HPM output includes
both time series of annual carbon and water fluxes, peat height, and water
table depth, as well as a final peat profile that can be &quot;cored&quot; and
compared to field observations of peat age and macrofossil composition. A
stochastic 8500-yr, annual precipitation time series was constrained by a
published Holocene climate reconstruction for southern Québec. HPM
simulated 5.4 m of peat accumulation (310 kg C m&lt;sup&gt;-2&lt;/sup&gt;) over 8500 years,
6.5% of total NPP over the period. Vascular plant functional types
accounted for 65% of total NPP over 8500 years but only 35% of the
final (contemporary) peat mass. Simulated age-depth and carbon accumulation
profiles were compared to a radiocarbon dated 5.8 m, c.9000-yr core. The
simulated core was younger than observations at most depths, but had a
similar overall trajectory; carbon accumulation rates were generally higher
in the simulation and were somewhat more variable than observations. HPM
results were sensitive to century-scale anomalies in precipitation, with
extended drier periods (precipitation reduced &amp;sim;10%) causing the
peat profile to lose carbon (and height), despite relatively small changes
in NPP.</description><pubDate>Mon, 04 Oct 2010 00:00:00 +0200</pubDate></item></channel></rss>
