293 research outputs found
Distroglicanopatías: análisis en pacientes, generación del knockout condicional de Pomt1 en fotorreceptores, y estudios genéticos y funcionales de FKTN y de FKRP en células en cultivo
Tesis doctoral inédita leída en la Universidad Autónoma de Madrid, Facultad de Medicina, Departamento de Bioquímica. Fecha de lectura: 25 -11-2016Esta tesis tiene embargado el acceso al texto completo hasta el 25-05-2018Las
distroglicanopatías
son
un
grupo
heterogéneo
de
distrofias
musculares
de
herencia
recesiva
que
también
pueden
presentar
en
diferentes
grados
afectación
nerviosa
y
ocular.
A
nivel
molecular
se
caracterizan
por
la
pérdida
de
la
glicosilación
del
alfa-‐
distroglicano
(α-‐DG).
El
DG
es
una
proteína
de
la
matriz
extracelular
(MEC)
formada
por
dos
subunidades
(α-‐DG
y
β-‐DG)
que
conecta
proteínas
de
la
MEC
(p.
ej.
laminina,
perlecano
o
pikachurina)
con
el
citoesqueleto
de
actina,
a
través
de
su
unión
citoplasmática
a
la
distrofina.
La
conexión
con
las
proteínas
de
la
MEC
se
realiza
a
través
de
los
residuos
glicosílicos,
principalmente
O-‐manosilglicanos,
presentes
en
la
región
mucina
del
α-‐DG.
Hasta
la
fecha,
18
genes
se
han
relacionado
con
el
proceso
de
O-‐manosilación
del
α-‐
DG.
Entre
ellos
encontramos
genes
que
codifican
tanto
glicosiltransferasas
como
proteínas
que
intervienen
en
la
generación
de
compuestos
intermedios
de
la
glicosilación.
La
proteína
O-‐manosiltransferasa
1
(POMT1)
es
la
primera
enzima,
que
conjuntamente
con
su
homóloga
POMT2,
introduce
la
manosa
inicial.
Este
monosacárido
es
esencial
para
la
generación
de
las
diferentes
estructuras
glicosiladas
del
α-‐DG.
Por
otra
parte,
las
proteínas
FKTN
y
FKRP
son
enzimas
que
actúan
en
pasos
posteriores
del
proceso
de
glicosilación.
Recientemente
se
ha
descrito
que
ambas
introducen
residuos
de
ribitol
5-‐fosfato
en
uno
de
los
residuos
del
α-‐DG.
Mutaciones
en
POMT1,
FKTN
y
FKRP
generan
desde
distroglicanopatías
muy
graves,
como
pueden
ser
el
síndrome
de
Walker-‐Warburg
(WWS)
o
la
distrofia
muscular
congénita
tipo
Fukuyama
(FCMD),
a
presentaciones
clínicas
más
leves
como
las
distrofias
musculares
de
cintura
tipo
2
(LGMD2).
En
este
trabajo
hemos
analizado
dos
pacientes
con
sospecha
de
distroglicanopatía,
los
cuales
finalmente
han
mostrado
un
déficit
en
la
vía
de
autofagia
con
una
alteración
en
la
glicosilación
del
α-‐DG.
Este
hecho
plantea
una
posible
relación
entre
la
glicosilación
del
α-‐
DG
y
esta
ruta
de
degradación.
Por
otra
parte,
hemos
generado
un
modelo
knockout
condicional
de
ratón
para
el
gen
Pomt1
en
los
fotorreceptores
de
la
retina.
Hemos
demostrado
cómo
la
mutación
del
gen
Pomt1
está
asociada
a
la
pérdida
de
glicosilación
del
α-‐DG,
la
cual
genera
una
malformación
de
la
sinapsis
entre
los
fotorreceptores
y
la
células
bipolares
(sinapsis
ribbon)
y
una
disfunción
visual.
Por
último,
hemos
generado
líneas
celulares
de
mioblastos
de
ratón
knockout
para
los
genes
Fktn
y
Fkrp.
En
estas
células
hemos
realizado
estudios
comparativos
de
glicoproteómica
y
del
perfil
de
expresión
con
el
objetivo
de
aproximarnos
a
la
función
de
estos
genes
de
una
manera
indirecta.
También
hemos
llevado
a
cabo
estudios
de
la
señal
de
retención
en
el
aparato
de
Golgi
de
estas
proteínas
en
las
líneas
silvestres
y
knockout.Dystroglycanopathies
are
a
heterogenous
group
of
recessive
muscular
dystrophies
which
can
also
present
different
grades
of
nervous
and
ocular
affectation.
At
a
molecular
level,
the
absence
of
α-‐dystroglycan
(α-‐DG)
glycosylation
is
the
main
characteristic
of
these
diseases.
Dystroglycan
is
a
matrix
extracelular
(ECM)
protein
conformed
by
two
subunits
(α-‐DG
and
β-‐DG),
that
conects
other
ECM
proteins
(such
as
laminin,
perlecan
or
pikachurin)
with
the
actin
cytoskeleton
through
its
cytoplasmatic
connection
with
dystrophin.
The
interaction
with
ECM
proteins
is
mediated
by
its
glycan
residues,
mainly
O-‐
mannosylglycans,
located
in
the
mucine
región
of
α-‐DG.
To
date,
18
genes
have
been
related
with
α-‐DG
O-‐mannosylation
process.
These
genes
codified
for
glycosyltransferases
or
proteins
that
generate
glycosylation
intermediates.
Protein
O-‐mannosyltransferase
1
(POMT1)
is
the
first
enzyme,
together
with
its
homologous
POMT2,
which
introduces
the
inital
mannose.
This
monosacharide
is
essential
for
the
generation
of
different
mannosylated
cores.
On
the
other
hand,
FKTN
and
FKRP
are
enzymes
that
act
in
posterior
steps
of
the
glycosylation
process.
It
has
recently
been
described
that
both
of
them
introduces
ribitol
5-‐phosphate
in
a
specific
α-‐DG
core.
Mutationzs
in
POMT1,
FKTN
and
FKRP
are
able
to
cause
from
severe
dystroglycanopathies,
such
as
Walker-‐Warburg
syndrome
(WWS)
or
Fukuyama
congenital
muscular
dystrophy
(FCMD),
to
less
severe
dystroglycanopathies
like
limb-‐girdle
muscular
dystrophies
type
2
(LGMD2).
In
this
work,
we
have
analyzed
two
patients
with
dystroglycanopathy
suspicion.
The
genetic-‐molecular
characterization
has
finally
revealed
an
imparment
in
the
autophagy
pathway
but
we
have
also
detected
α-‐DG
glyscosylation
anomalies.
The
data
seem
to
highlight
a
posible
relation
between
autophagy
and
α-‐DG.
On
the
other
hand,
we
have
generated
a
conditional
knockout
mouse
model
for
Pomt1
gene
in
the
retinal
photoreceptors.
We
have
demonstrated
how
the
mutation
of
POMT1
is
associated
with
the
loss
of
α-‐DG
glycosylation,
which
causes
a
destructing
in
the
synapsis
between
both
photoreceptor
and
bipolar
cells
(ribbon
synapsis)
and
an
associated
visual
imparment.
Finally,
we
have
generated
mouse
myoblast
cell
lines
knockout
for
Fktn
and
Fkrp.
In
these
cell
lines
we
have
performed
comparative
glycoproteomic
and
transcriptional
profile
analysis
with
the
aim
to
approach,
indirectly,
to
the
function
of
these
proteins.
We
have
also
analyzed
the
signal
for
Golgi
retention
in
wild-‐type
and
knockout
cell
lines
Maneuver Optimization for Simultaneous Airspeed Calibration and Wind Estimation
[EN] The purpose of this work is to optimize systematically the maneuver required to identify the wind and calibrate the airspeed sensor of a subsonic aircraft using a GPS method. The optimization is based on sensitivity analyses that require a considerable number of flight simulations. To face this challenging computational effort, we adapted and parallelized a particle swarm optimization algorithm. We also introduced a new formulation of the sensor model in the Bernstein form. The results show stability using the selected formulation and bring out non-obvious aliasing and precision loss effects that depend on the maneuver configuration. The knowledge of these effects allowed us to fine-tune the maneuver in order to improve the estimation's precision. Finally, we validated the method using the JSBSim flight simulator under calm and light turbulence conditions.S
Large-eddy simulation analysis of the influence of the needle lift on the cavitation in diesel injector nozzles
The cavitation phenomenon has a strong influence on the internal flow and spray development in diesel injector nozzles.
Despite its importance, there are many aspects which still remain unclear, especially for partial needle lifts when the
injector is in the opening and closing phases. For that reason, the current paper is focused on the influence of the needle
lift on the internal flow in a diesel nozzle. This study was carried out with three-dimensional simulations at a high injection
pressure (160 MPa) using a homogeneous equilibrium model implemented in OpenFOAM to model the cavitation
phenomenon. The nozzle was simulated with large-eddy simulation methods at six different needle lifts (10 mm, 30 mm,
50 mm, 75 mm, 100 mm and 250 mm), providing relevant information about the evolution of the internal flow, the turbulence
development (the vorticity, the turbulence–cavitation interaction and the turbulent structures) and the flow characteristics
in the nozzle outlet (the mass flow, the momentum flux and the effective velocity) with the needle position.Desantes Fernández, JM.; Salvador Rubio, FJ.; Carreres Talens, M.; Martínez López, J. (2015). Large-eddy simulation analysis of the influence of the needle lift on the cavitation in diesel injector nozzles. Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering. 229(4):407-423. doi:10.1177/0954407014542627S4074232294Faeth, G. ., Hsiang, L.-P., & Wu, P.-K. (1995). Structure and breakup properties of sprays. International Journal of Multiphase Flow, 21, 99-127. doi:10.1016/0301-9322(95)00059-7Park, S. H., Suh, H. K., & Lee, C. S. (2009). Effect of Bioethanol−Biodiesel Blending Ratio on Fuel Spray Behavior and Atomization Characteristics. Energy & Fuels, 23(8), 4092-4098. doi:10.1021/ef900068aPAYRI, R., GARCIA, J., SALVADOR, F., & GIMENO, J. (2005). Using spray momentum flux measurements to understand the influence of diesel nozzle geometry on spray characteristics. Fuel, 84(5), 551-561. doi:10.1016/j.fuel.2004.10.009Suh, H. K., & Lee, C. S. (2008). Effect of cavitation in nozzle orifice on the diesel fuel atomization characteristics. International Journal of Heat and Fluid Flow, 29(4), 1001-1009. doi:10.1016/j.ijheatfluidflow.2008.03.014Payri, R., Salvador, F. J., Gimeno, J., & de la Morena, J. (2009). Effects of nozzle geometry on direct injection diesel engine combustion process. Applied Thermal Engineering, 29(10), 2051-2060. doi:10.1016/j.applthermaleng.2008.10.009Park, S. H., Kim, S. H., & Lee, C. S. (2009). Mixing Stability and Spray Behavior Characteristics of Diesel−Ethanol−Methyl Ester Blended Fuels in a Common-Rail Diesel Injection System. Energy & Fuels, 23(10), 5228-5235. doi:10.1021/ef9004847Desantes, J. M., Payri, R., Salvador, F. J., & Gil, A. (2006). Development and validation of a theoretical model for diesel spray penetration. Fuel, 85(7-8), 910-917. doi:10.1016/j.fuel.2005.10.023Desantes, J. M., Payri, R., Garcia, J. M., & Salvador, F. J. (2007). A contribution to the understanding of isothermal diesel spray dynamics. Fuel, 86(7-8), 1093-1101. doi:10.1016/j.fuel.2006.10.011Badock, C., Wirth, R., Fath, A., & Leipertz, A. (1999). Investigation of cavitation in real size diesel injection nozzles. International Journal of Heat and Fluid Flow, 20(5), 538-544. doi:10.1016/s0142-727x(99)00043-0Som, S., Aggarwal, S. K., El-Hannouny, E. M., & Longman, D. E. (2010). Investigation of Nozzle Flow and Cavitation Characteristics in a Diesel Injector. Journal of Engineering for Gas Turbines and Power, 132(4). doi:10.1115/1.3203146Macian, V., Payri, R., Margot, X., & Salvador, F. J. (2003). A CFD ANALYSIS OF THE INFLUENCE OF DIESEL NOZZLE GEOMETRY ON THE INCEPTION OF CAVITATION. Atomization and Sprays, 13(5-6), 579-604. doi:10.1615/atomizspr.v13.i56.80Alajbegovic, A., Meister, G., Greif, D., & Basara, B. (2002). Three phase cavitating flows in high-pressure swirl injectors. Experimental Thermal and Fluid Science, 26(6-7), 677-681. doi:10.1016/s0894-1777(02)00179-6Unverdi, S. O., & Tryggvason, G. (1992). A front-tracking method for viscous, incompressible, multi-fluid flows. Journal of Computational Physics, 100(1), 25-37. doi:10.1016/0021-9991(92)90307-kBrackbill, J. ., Kothe, D. ., & Zemach, C. (1992). A continuum method for modeling surface tension. Journal of Computational Physics, 100(2), 335-354. doi:10.1016/0021-9991(92)90240-yPlesset M, Devine R. Effect of exposure time on cavitation damage. Report (Office of Naval Research Contract Nonr-220(28)), California Institute of Technology, Pasadena, California, USA, 1965.Chen, Y., & Heister, S. D. (1996). MODELING CAVITATING FLOWS IN DIESEL INJECTORS. Atomization and Sprays, 6(6), 709-726. doi:10.1615/atomizspr.v6.i6.50Vortmann, C., Schnerr, G. H., & Seelecke, S. (2003). Thermodynamic modeling and simulation of cavitating nozzle flow. International Journal of Heat and Fluid Flow, 24(5), 774-783. doi:10.1016/s0142-727x(03)00003-1Echouchene, F., Belmabrouk, H., Le Penven, L., & Buffat, M. (2011). Numerical simulation of wall roughness effects in cavitating flow. International Journal of Heat and Fluid Flow, 32(5), 1068-1075. doi:10.1016/j.ijheatfluidflow.2011.05.010Salvador, F. J., Romero, J.-V., Roselló, M.-D., & Martínez-López, J. (2010). Validation of a code for modeling cavitation phenomena in Diesel injector nozzles. Mathematical and Computer Modelling, 52(7-8), 1123-1132. doi:10.1016/j.mcm.2010.02.027Salvador, F. J., Hoyas, S., Novella, R., & Martínez-López, J. (2011). Numerical simulation and extended validation of two-phase compressible flow in diesel injector nozzles. Proceedings of the Institution of Mechanical Engineers, Part D: Journal of Automobile Engineering, 225(4), 545-563. doi:10.1177/09544070jauto1569Payri, F., Payri, R., Salvador, F. J., & Martínez-López, J. (2012). A contribution to the understanding of cavitation effects in Diesel injector nozzles through a combined experimental and computational investigation. Computers & Fluids, 58, 88-101. doi:10.1016/j.compfluid.2012.01.005Salvador, F. J., Martínez-López, J., Caballer, M., & De Alfonso, C. (2013). Study of the influence of the needle lift on the internal flow and cavitation phenomenon in diesel injector nozzles by CFD using RANS methods. Energy Conversion and Management, 66, 246-256. doi:10.1016/j.enconman.2012.10.011Salvador, F. J., Martínez-López, J., Romero, J.-V., & Roselló, M.-D. (2013). Computational study of the cavitation phenomenon and its interaction with the turbulence developed in diesel injector nozzles by Large Eddy Simulation (LES). Mathematical and Computer Modelling, 57(7-8), 1656-1662. doi:10.1016/j.mcm.2011.10.050Piomelli, U. (1999). Large-eddy simulation: achievements and challenges. Progress in Aerospace Sciences, 35(4), 335-362. doi:10.1016/s0376-0421(98)00014-1Launder, B. E., & Spalding, D. B. (1974). The numerical computation of turbulent flows. Computer Methods in Applied Mechanics and Engineering, 3(2), 269-289. doi:10.1016/0045-7825(74)90029-2Payri, F., Bermúdez, V., Payri, R., & Salvador, F. J. (2004). The influence of cavitation on the internal flow and the spray characteristics in diesel injection nozzles. Fuel, 83(4-5), 419-431. doi:10.1016/j.fuel.2003.09.010Payri, R., Salvador, F. J., Gimeno, J., & de la Morena, J. (2009). Study of cavitation phenomena based on a technique for visualizing bubbles in a liquid pressurized chamber. International Journal of Heat and Fluid Flow, 30(4), 768-777. doi:10.1016/j.ijheatfluidflow.2009.03.011Martínez López, J. (s. f.). Estudio computacional de la influencia del levantamiento de aguja sobre el flujo interno y el fenómeno de la cavitación en toberas de inyección diésel. doi:10.4995/thesis/10251/29291Tabor, G. R., & Baba-Ahmadi, M. H. (2010). Inlet conditions for large eddy simulation: A review. Computers & Fluids, 39(4), 553-567. doi:10.1016/j.compfluid.2009.10.007Payri, R., Gimeno, J., Marti-Aldaravi, P., & Bracho, G. (2013). Study of the influence of the inlet boundary conditions in a LES simulation of internal flow in a diesel injector. Mathematical and Computer Modelling, 57(7-8), 1709-1715. doi:10.1016/j.mcm.2011.11.019de Villiers E. The potential of large eddy simulation for the modeling of wall bounded flows. PhD Thesis, Imperial College of Science, Technology and Medicine, London, UK, 2006.Lee, J. W., Min, K. D., Kang, K. Y., Bae, C. S., Giannadakis, E., Gavaises, M., & Arcoumanis, C. (2006). Effect of piezo-driven and solenoid-driven needle opening of common-rail diesel injectors on internal nozzle flow and spray development. International Journal of Engine Research, 7(6), 489-502. doi:10.1243/14680874jer00806Desantes, J. M., Payri, R., Salvador, F. J., & De la Morena, J. (2010). Influence of cavitation phenomenon on primary break-up and spray behavior at stationary conditions. Fuel, 89(10), 3033-3041. doi:10.1016/j.fuel.2010.06.004Lesieur, M., Métais, O., & Comte, P. (2005). Large-Eddy Simulations of Turbulence. doi:10.1017/cbo9780511755507Sagaut, P. (2001). Large Eddy Simulation for Incompressible Flows. Scientific Computation. doi:10.1007/978-3-662-04416-
Experimental Characterization of the Thermodynamic Properties of Diesel Fuels Over a Wide Range of Pressures and Temperatures
The influence of pressure and temperature on some of the important thermodynamic properties of diesel fuels has been assessed for a set of fuels. The study focuses on the experimental determination of the speed of sound, density and compressibility (via the bulk modulus) of these fuels by means of a method that is thoroughly described in this paper. The setup makes use of a common-rail
injection system in order to transmit a pressure wave through a high-pressure line and measure the time it takes for the wave to travel a given distance. Measurements have been performed in a wide range of pressures (from atmospheric pressure up to 200 MPa) and temperatures (from 303 to 353 K), in order to generate a fuel properties database for modelers on the field of injection systems for
diesel engines to incorporate to their simulations.This work was partly sponsored by "Ministerio de Economia y Competitividad" (Spanish Ministry of Economy) in the frame of the project "Comprension de la influencia de combustibles no convencionales en el proceso de inyeccion y combustion tipo diesel", reference TRA2012-36932. The equipment used in this work hasDesantes Fernández, JM.; Salvador Rubio, FJ.; Carreres Talens, M.; Jaramillo-Císcar, D. (2015). Experimental Characterization of the Thermodynamic Properties of Diesel Fuels Over a Wide Range of Pressures and Temperatures. SAE International Journal of Fuel and Lubricants. 8(1):190-199. https://doi.org/10.4271/2015-01-0951S1901998
Insights into the room temperature magnetism of ZnO/Co3O4 mixtures
The origin of room temperature (RT) ferromagneticlike behavior in ZnO-based
diluted magnetic semiconductors is still an unclear topic. The present work
concentrates on the appearance of RT magnetic moments in just mixed ZnO/Co3O4
mixtures without thermal treatment. In this study, it is shown that the
magnetism seems to be related to surface reduction of the Co3O4 nanoparticles,
in which, an antiferromagnetic Co3O4 nanoparticle (core) is surrounded by a
CoO-like shell. This singular superficial magnetism has also been found in
other mixtures with semiconductors such as TiO2 and insulators such as Al2O3
Molecular Recognition, Transient Chirality and Sulfur Hydrogen Bonding in the Benzyl Mercaptan Dimer
The homodimers of transiently chiral molecules offer physical insight into the process of molecular recognition, the preference for homo or heterochiral aggregation and the nature of the non-covalent interactions stabilizing the adducts. We report the observation of the benzyl mercaptan dimer in the isolation conditions of a supersonic jet expansion, using broadband (chirped-pulse) microwave spectroscopy. A single homochiral isomer was observed for the dimer, stabilized by a cooperative sequence of S-H···S and S-H···π hydrogen bonds. The structural data, stabilization energies and energy decomposition describe these non-covalent interactions as weak and dispersion-controlled. A comparison is also provided with the benzyl alcohol dimer.This research was funded by the Spanish Ministerio de Ciencia e Innovación MICINN-FEDER, grants numbers PGC2018-098561-B-C21 and PGC2018-098561-B-C22. The APC were funded by PGC2018-098561-B-C22
Light-driven motion of charged domain walls in isolated ferroelectrics
©2022 American Physical SocietyLight-induced ferroelectric domain wall motion turns out to be a promising phenomenon to de- velop new photo-controlled devices. However, the physical origin of this ligh-matter coupling when material is irradiated with visible light remains unclear. Here, a phenomenological model predicting the motion of charged domain walls (CDWs) is developed. The photo-induced electronic reconstruc- tion mechanism is proposed as the primary absorption mechanism, leading to a linear dependence for the polarization perturbation with the light intensity. Domain walls motion is then driven by the energetic difference between domains in a CDW array, such that the macroscopic polarization can be easily tuned.Postprint (author's final draft
Increased YKL-40 but Not C-Reactive Protein Levels in Patients with Alzheimer’s Disease
Neuroinflammation is a common feature in Alzheimer's (AD) and Parkinson's (PD) disease. In the last few decades, a testable hypothesis was proposed that protein-unfolding events might occur due to neuroinflammatory cascades involving alterations in the crosstalk between glial cells and neurons. Here, we tried to clarify the pattern of two of the most promising biomarkers of neuroinflammation in cerebrospinal fluid (CSF) in AD and PD. This study included cognitively unimpaired elderly patients, patients with mild cognitive impairment, patients with AD dementia, and patients with PD. CSF samples were analyzed for YKL-40 and C-reactive protein (CRP). We found that CSF YKL-40 levels were significantly increased only in dementia stages of AD. Additionally, increased YKL-40 levels were found in the cerebral orbitofrontal cortex from AD patients in agreement with augmented astrogliosis. Our study confirms that these biomarkers of neuroinflammation are differently detected in CSF from AD and PD patients
R-RAS2 overexpression in tumors of the human central nervous system
Malignant tumors of the central nervous system (CNS) are the 10th most frequent cause of cancer mortality. Despite
the strong malignancy of some such tumors, oncogenic mutations are rarely found in classic members of the RAS
family of small GTPases. This raises the question as to whether other RAS family members may be affected in CNS
tumors, excessively activating RAS pathways. The RAS-related subfamily of GTPases is that which is most closely
related to classical Ras and it currently contains 3 members: RRAS, RRAS2 and RRAS3. While R-RAS and R-RAS2 are
expressed ubiquitously, R-RAS3 expression is restricted to the CNS. Significantly, both wild type and mutated RRAS2
(also known as TC21) are overexpressed in human carcinomas of the oral cavity, esophagus, stomach, skin and
breast, as well as in lymphomas. Hence, we analyzed the expression of R-RAS2 mRNA and protein in a wide variety
of human CNS tumors and we found the R-RAS2 protein to be overexpressed in all of the 90 CNS cancer samples
studied, including glioblastomas, astrocytomas and oligodendrogliomas. However, R-Ras2 was more strongly
expressed in low grade (World Health Organization grades I-II) rather than high grade (grades III-IV) tumors,
suggesting that R-RAS2 is overexpressed in the early stages of malignancy. Indeed, R-RAS2 overexpression was
evident in pre-malignant hyperplasias, both at the mRNA and protein levels. Nevertheless, such dramatic changes in
expression were not evident for the other two subfamily members, which implies that RRAS2 is the main factor
triggering neural transformation.This work was supported by grants SAF2012-31279 from
the ‘Comisión Interministerial de Ciencia y Tecnología’ and the ‘Ramón y
Cajal’ program (RYC-2010-06251, to B.C.). We also thank the Fundación
Ramón Areces for its institutional support of the ‘Centro de Biología
Molecular Severo Ochoa’
Is a neutral expression also a neutral stimulus?: a study with functional magnetic resonance
Although neutral faces do not initially convey an explicit emotional message, it has been found that individuals tend to assign them an affective content. Moreover, previous research has shown that affective judgments are mediated by the task they have to perform. Using functional magnetic resonance imaging in 21 healthy participants, we
focus this study on the cerebral activity patterns triggered by neutral and emotional faces in two different tasks (social or gender judgments). Results obtained, using conjunction
analyses, indicated that viewing both emotional and neutral faces evokes activity in several similar brain areas indicating a common neural substrate. Moreover, neutral faces specifically elicit activation of cerebellum, frontal and temporal areas, while emotional faces involve the cuneus, anterior cingulated gyrus, medial orbitofrontal cortex, posterior superior temporal gyrus, precentral/postcentral gyrus and insula. The task selected was also found to influence brain activity, in that the social task recruited frontal areas while the gender task involved the posterior cingulated, inferior parietal lobule and middle temporal gyrus to a greater extent. Specifically, in the social task viewing neutral faces was associated with longer reaction times and increased activity of left dorsolateral frontal cortex compared with viewing facial expressions of emotions. In contrast, in the
same task emotional expressions distinctively activated the left amygdale. The results are discussed taking into consideration the fact that, like other facial expressions, neutral
expressions are usually assigned some emotional significance. However, neutral faces evoke a greater activation of circuits probably involved in more elaborate cognitive
processing.This research was supported by a grant from Ministerio de Ciencia y Tecnología, Spain (MICINN-PSI-2009-09067)
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