Benito Chen-Charpentier

Prof. Benito Chen-Charpentier

University of texas at Arlington
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Research Focus & Metrics

Academic Career Length

48Years (1979-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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29 August 2013 in Mathematical Methods in the Applied Sciences
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Gilberto Gonzalez-ParraGilberto Gonzalez-Parra
Gilberto Gonzalez-Parra
ABRAHAM JOSE ARENAS TAWILABRAHAM JOSE ARENAS TAWIL
ABRAHAM JOSE ARENAS TAWIL
Benito Chen-CharpentierBenito Chen-Charpentier
Benito Chen-Charpentier

1 March 2016 in Mathematics and Computers in Simulation
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Journal Article
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ABRAHAM JOSE ARENAS TAWILABRAHAM JOSE ARENAS TAWIL
ABRAHAM JOSE ARENAS TAWIL
Gilberto Gonzalez-ParraGilberto Gonzalez-Parra
Gilberto Gonzalez-Parra
Benito Chen-CharpentierBenito Chen-Charpentier
Benito Chen-Charpentier

1 June 1979 in Studies in Applied Mathematics
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Benito Chen-CharpentierBenito Chen-Charpentier
Benito Chen-Charpentier
PSP. G. Saffman
P. G. Saffman

1 February 1980 in Studies in Applied Mathematics
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Benito Chen-CharpentierBenito Chen-Charpentier
Benito Chen-Charpentier
PSP. G. Sallman
P. G. Sallman

12 January 2017 in Biogeosciences
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YLYiqi Luo
Yiqi Luo
ZSZheng Shi
Zheng Shi
XLXingjie Lu
Xingjie Lu
JXJianyang Xia
Jianyang Xia
JLJunyi Liang
Junyi Liang
YWYingping Wang
Yingping Wang
Terrestrial ecosystems have absorbed roughly 30 % of anthropogenic CO2 emissions over the past decades, but it is unclear whether this carbon (C) sink will endure into the future. Despite extensive modeling and experimental and observational studies, what fundamentally determines transient dynamics of terrestrial C storage under global change is still not very clear. Here we develop a new framework for understanding transient dynamics of terrestrial C storage through mathematical analysis and numerical experiments. Our analysis indicates that the ultimate force driving ecosystem C storage change is the C storage capacity, which is jointly determined by ecosystem C input (e.g., net primary production, NPP) and residence time. Since both C input and residence time vary with time, the C storage capacity is time-dependent and acts as a moving attractor that actual C storage chases. The rate of change in C storage is proportional to the C storage potential, which is the difference between the current storage and the storage capacity. The C storage capacity represents instantaneous responses of the land C cycle to external forcing, whereas the C storage potential represents the internal capability of the land C cycle to influence the C change trajectory in the next time step. The influence happens through redistribution of net C pool changes in a network of pools with different residence times. Moreover, this and our other studies have demonstrated that one matrix equation can replicate simulations of most land C cycle models (i.e., physical emulators). As a result, simulation outputs of those models can be placed into a three-dimensional (3-D) parameter space to measure their differences. The latter can be decomposed into traceable components to track the origins of model uncertainty. In addition, the physical emulators make data assimilation computationally feasible so that both C flux- and pool-related datasets can be used to better constrain model predictions of land C sequestration. Overall, this new mathematical framework offers new approaches to understanding, evaluating, diagnosing, and improving land C cycle models.

1 May 2013 in Mathematical and Computer Modelling
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Benito Chen-CharpentierBenito Chen-Charpentier
Benito Chen-Charpentier
Hristo V KojouharovHristo V Kojouharov
Hristo V Kojouharov