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    <title>DSpace Collection:</title>
    <link>http://hdl.handle.net/2117/1088</link>
    <description />
    <pubDate>Tue, 21 May 2013 06:31:53 GMT</pubDate>
    <dc:date>2013-05-21T06:31:53Z</dc:date>
    <itunes:owner>
      <itunes:email>webmaster.bupc@upc.edu</itunes:email>
      <itunes:name>Universitat Politècnica de Catalunya. Servei de Biblioteques i Documentació</itunes:name>
    </itunes:owner>
    <itunes:explicit>no</itunes:explicit>
    <itunes:keywords />
    <item>
      <title>Modelling shoreline sand waves: application to the coast of Namibia</title>
      <link>http://hdl.handle.net/2117/14928</link>
      <description>Title: Modelling shoreline sand waves: application to the coast of Namibia
Authors: Falqués Serra, Albert; Van den Berg, Niels; Ribas Prats, Francesca; Caballeria Suriñach, Miquel
Abstract: The SW coast of Africa (Namibia and part of Angola) features very long sandy beaches and a wave climate dominated by energetic swells from the SSW, therefore approaching the coast with a very high obliquity. Satellite images reveal that along that coast there are many shoreline sand waves with wavelengths ranging from 2 to 8 km. A more detailed study, including a Fourier analysis of the shoreline position, confirms a high spectral density concentration at these lengths scales. Also, it becomes apparent that at least some of the sand waves are dynamically active rather than being controlled by the geological setting. A morphodynamic model is used to test the hypothesis that these sand waves could emerge as free morphodynamic instabilities of the coastline due to the obliquity in wave incidence. It is found that the wave period, Tp, is crucial to establish the tendency to stability or instability, instability increasing for decreasing period, whilst there is some discrepancy in the observed periods. Model results for Tp = 7 s clearly show the tendency for the coast to develop free sand waves at 2 km wavelength within a few years, which migrate to the north at rates of 0.6-0.7 km/yr. For Tp = 8 s, instability is weaker and rather sensitive to other factors as the underlying bathymetry. In this case, the coast seems to be nearly at neutral stability so that sand waves originated from other mechanisms can propagate downdrift with little decay.</description>
      <guid isPermaLink="false">http://hdl.handle.net/2117/14928</guid>
      <itunes:author>Falqués Serra, Albert; Van den Berg, Niels; Ribas Prats, Francesca; Caballeria Suriñach, Miquel</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>The SW coast of Africa (Namibia and part of Angola) features very long sandy beaches and a wave climate dominated by energetic swells from the SSW, therefore approaching the coast with a very high obliquity. Satellite images reveal that along that coast there are many shoreline sand waves with wavelengths ranging from 2 to 8 km. A more detailed study, including a Fourier analysis of the shoreline position, confirms a high spectral density concentration at these lengths scales. Also, it becomes apparent that at least some of the sand waves are dynamically active rather than being controlled by the geological setting. A morphodynamic model is used to test the hypothesis that these sand waves could emerge as free morphodynamic instabilities of the coastline due to the obliquity in wave incidence. It is found that the wave period, Tp, is crucial to establish the tendency to stability or instability, instability increasing for decreasing period, whilst there is some discrepancy in the observed periods. Model results for Tp = 7 s clearly show the tendency for the coast to develop free sand waves at 2 km wavelength within a few years, which migrate to the north at rates of 0.6-0.7 km/yr. For Tp = 8 s, instability is weaker and rather sensitive to other factors as the underlying bathymetry. In this case, the coast seems to be nearly at neutral stability so that sand waves originated from other mechanisms can propagate downdrift with little decay.</itunes:summary>
    </item>
    <item>
      <title>Percolation experiments in complex fractal media</title>
      <link>http://hdl.handle.net/2117/19318</link>
      <description>Title: Percolation experiments in complex fractal media
Authors: Redondo Apraiz, José Manuel; Tarquis, Ana Maria; Cherubini, Claudia; Lopez Gonzalez-Nieto, Pilar; Vila, Teresa</description>
      <pubDate>Thu, 16 May 2013 16:20:33 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/19318</guid>
      <dc:date>2013-05-16T16:20:33Z</dc:date>
      <itunes:author>Redondo Apraiz, José Manuel; Tarquis, Ana Maria; Cherubini, Claudia; Lopez Gonzalez-Nieto, Pilar; Vila, Teresa</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords>Percolation, Fractal, Karstic</itunes:keywords>
    </item>
    <item>
      <title>SAR measurements of coastal features in the NW Mediterranean</title>
      <link>http://hdl.handle.net/2117/19317</link>
      <description>Title: SAR measurements of coastal features in the NW Mediterranean
Authors: Redondo Apraiz, José Manuel; Martínez Benjamín, Juan José; Díez Rilova, Margarita; Lopez Gonzalez-Nieto, Pilar</description>
      <pubDate>Thu, 16 May 2013 16:15:04 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/19317</guid>
      <dc:date>2013-05-16T16:15:04Z</dc:date>
      <itunes:author>Redondo Apraiz, José Manuel; Martínez Benjamín, Juan José; Díez Rilova, Margarita; Lopez Gonzalez-Nieto, Pilar</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords>SAR, Coastal Features, Vortex</itunes:keywords>
    </item>
    <item>
      <title>The evolution and C, N and O yields of intermediate-mass Z = 10-5 stars in isolation and in close binary systems</title>
      <link>http://hdl.handle.net/2117/18967</link>
      <description>Title: The evolution and C, N and O yields of intermediate-mass Z = 10-5 stars in isolation and in close binary systems
Authors: Gil Pons, Pilar; Doherty, Carolyn L.; Suda, T.; Campbell, Simon; Lau, H.; Mansouri Guilani, Shervin; Lattanzio, John
Abstract: We have computed the evolution of Z = 10−5 stars of masses between 4 and 9 M , from their&#xD;
main sequence till the late TP-(S)AGB phase.We use a recent version of the Mount Stromlo Stellar&#xD;
Evolution code, in which molecular opacities include the effects of variable C/O abundances ratio,&#xD;
[1]. By computing hundreds (or thousands) of thermal pulses, we have been able either to remove&#xD;
the bulk of the stellar envelopes or to obtain stellar cores very close to MCh. Using [2] prescription&#xD;
for the mass loss rates the computed stars lose their envelopes before their cores reach MCh. This&#xD;
would forbid the occurrence of SN 1.5 for Z = 10−5 stars. Nevertheless the results by [3] suggest&#xD;
that the former prescription might overestimate the mass-loss rates. Therefore we have decreased&#xD;
the rates by [2]. For all the cases we present, even a decrease of one order of magnitude let the&#xD;
stellar cores reach MCh before the envelope is lost. Therefore the occurrence of SN1.5 at Z = 10 −5&#xD;
and their potential contribution to the chemical evolution of the Universe should not be discarded.&#xD;
We consider the combined effects of the deep/corrosive 2 nd dredge-up and Roche Lobe Overflow&#xD;
(RLOF) during the E-AGB to help to constrain the contribution of massive Z = 10 −5 AGB stars to&#xD;
the CEMPs problem. Our results have implications for the chemical evolution of the Universe and&#xD;
might provide another piece for the puzzle of the CEMPs problem.</description>
      <pubDate>Tue, 23 Apr 2013 14:39:01 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18967</guid>
      <dc:date>2013-04-23T14:39:01Z</dc:date>
      <itunes:author>Gil Pons, Pilar; Doherty, Carolyn L.; Suda, T.; Campbell, Simon; Lau, H.; Mansouri Guilani, Shervin; Lattanzio, John</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>We have computed the evolution of Z = 10−5 stars of masses between 4 and 9 M , from their&#xD;
main sequence till the late TP-(S)AGB phase.We use a recent version of the Mount Stromlo Stellar&#xD;
Evolution code, in which molecular opacities include the effects of variable C/O abundances ratio,&#xD;
[1]. By computing hundreds (or thousands) of thermal pulses, we have been able either to remove&#xD;
the bulk of the stellar envelopes or to obtain stellar cores very close to MCh. Using [2] prescription&#xD;
for the mass loss rates the computed stars lose their envelopes before their cores reach MCh. This&#xD;
would forbid the occurrence of SN 1.5 for Z = 10−5 stars. Nevertheless the results by [3] suggest&#xD;
that the former prescription might overestimate the mass-loss rates. Therefore we have decreased&#xD;
the rates by [2]. For all the cases we present, even a decrease of one order of magnitude let the&#xD;
stellar cores reach MCh before the envelope is lost. Therefore the occurrence of SN1.5 at Z = 10 −5&#xD;
and their potential contribution to the chemical evolution of the Universe should not be discarded.&#xD;
We consider the combined effects of the deep/corrosive 2 nd dredge-up and Roche Lobe Overflow&#xD;
(RLOF) during the E-AGB to help to constrain the contribution of massive Z = 10 −5 AGB stars to&#xD;
the CEMPs problem. Our results have implications for the chemical evolution of the Universe and&#xD;
might provide another piece for the puzzle of the CEMPs problem.</itunes:summary>
    </item>
    <item>
      <title>Frontogenesis in the meso-a and meso-ß scales in the Mediterranean basin: From cloud arch to cloud cells.</title>
      <link>http://hdl.handle.net/2117/18917</link>
      <description>Title: Frontogenesis in the meso-a and meso-ß scales in the Mediterranean basin: From cloud arch to cloud cells.
Authors: Mazón Bueso, Jordi; Pino González, David</description>
      <pubDate>Mon, 22 Apr 2013 12:01:45 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18917</guid>
      <dc:date>2013-04-22T12:01:45Z</dc:date>
      <itunes:author>Mazón Bueso, Jordi; Pino González, David</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>Nocturnal offshore precipitation near the coastline in the Mediterranean basin</title>
      <link>http://hdl.handle.net/2117/18916</link>
      <description>Title: Nocturnal offshore precipitation near the coastline in the Mediterranean basin
Authors: Mazón Bueso, Jordi; Pino González, David</description>
      <pubDate>Mon, 22 Apr 2013 11:48:29 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18916</guid>
      <dc:date>2013-04-22T11:48:29Z</dc:date>
      <itunes:author>Mazón Bueso, Jordi; Pino González, David</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>The role of large sea-land temperature, the coastline shape and the SST in</title>
      <link>http://hdl.handle.net/2117/18790</link>
      <description>Title: The role of large sea-land temperature, the coastline shape and the SST in
Authors: Mazón Bueso, Jordi; Pino González, David</description>
      <pubDate>Mon, 15 Apr 2013 11:35:30 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18790</guid>
      <dc:date>2013-04-15T11:35:30Z</dc:date>
      <itunes:author>Mazón Bueso, Jordi; Pino González, David</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>Flash heat events: the case of 27th August 2010 in northeast of Iberian</title>
      <link>http://hdl.handle.net/2117/18554</link>
      <description>Title: Flash heat events: the case of 27th August 2010 in northeast of Iberian
Authors: Mazón Bueso, Jordi; Pino González, David</description>
      <pubDate>Wed, 03 Apr 2013 09:34:09 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18554</guid>
      <dc:date>2013-04-03T09:34:09Z</dc:date>
      <itunes:author>Mazón Bueso, Jordi; Pino González, David</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>Uncertainties in the CO2 budget associated to the diurnal variability of the boundary layer dynamics</title>
      <link>http://hdl.handle.net/2117/18552</link>
      <description>Title: Uncertainties in the CO2 budget associated to the diurnal variability of the boundary layer dynamics
Authors: Pino González, David; Kaikkonen, Jukka-Pekka; Vilà-Guerau de Arellano, Jordi</description>
      <pubDate>Wed, 03 Apr 2013 09:05:04 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18552</guid>
      <dc:date>2013-04-03T09:05:04Z</dc:date>
      <itunes:author>Pino González, David; Kaikkonen, Jukka-Pekka; Vilà-Guerau de Arellano, Jordi</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>Production of short-lived radioactive nuclei in Super Asymptotic Giant Branch stars</title>
      <link>http://hdl.handle.net/2117/18437</link>
      <description>Title: Production of short-lived radioactive nuclei in Super Asymptotic Giant Branch stars
Authors: Doherty, Carolyn L.; Lugaro, M.; Lau, H. H. B.; Siess, Lionel; Lattanzio, John; Gil Pons, Pilar</description>
      <pubDate>Wed, 20 Mar 2013 12:17:20 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18437</guid>
      <dc:date>2013-03-20T12:17:20Z</dc:date>
      <itunes:author>Doherty, Carolyn L.; Lugaro, M.; Lau, H. H. B.; Siess, Lionel; Lattanzio, John; Gil Pons, Pilar</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>What determines the wavelength of self-organized shoreline sand waves?</title>
      <link>http://hdl.handle.net/2117/18428</link>
      <description>Title: What determines the wavelength of self-organized shoreline sand waves?
Authors: Falqués Serra, Albert; Van den Berg, Niels; Ribas Prats, Francesca; Caballeria, M
Abstract: Shoreline undulations extending into the bathymetric contours with a length scale larger than that of the rhythmic surf zone bars are referred to as shoreline sand waves. Many observed undulations along sandy coasts display a wavelength in the order 1-7 km. Several models that are based on the hypothesis that sand waves emerge from a morphodynamic instability in case of very oblique wave incidence predict this range of wavelengths. Here we investigate the physical reasons for the wavelength selection and the main parametric trends of the wavelength in case of sand waves arising from such instability. It is shown that the existence of a minimum wavelength depends on an interplay between three factors affecting littoral drift: (A) the angle of wave fronts relative to local shoreline, which tends to cause maximum transport at the downdrift flank of the sand wave, (B) the refractive energy spreading which tends to cause maximum transport at the updrift flank and (C) wave focusing (de-focusing) by the capes (bays), which tends to cause maximum transport at the crest or slightly downdrift of it. Processes A and C cause decay of the sand waves while process B causes their growth. For low incidence angles, B is very weak so that a rectilinear shoreline is stable. For large angles and long sand waves, B is dominant and causes the growth of sand waves. For large angles and short sand waves C is dominant and the sand waves decay. Thus, wavelength selection depends on process C, which essentially depends on shoreline curvature. The growth rate of very long sand waves is weak because the alongshore gradients in sediment transport decrease with the wavelength. This is why there is an optimum or dominant wavelength. It is found that sand wave wavelength scales with λ0/β where λ0 is the water wave wavelength in deep water and β is the mean bed slope from shore to the wave base.</description>
      <pubDate>Tue, 19 Mar 2013 19:22:41 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18428</guid>
      <dc:date>2013-03-19T19:22:41Z</dc:date>
      <itunes:author>Falqués Serra, Albert; Van den Berg, Niels; Ribas Prats, Francesca; Caballeria, M</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>Shoreline undulations extending into the bathymetric contours with a length scale larger than that of the rhythmic surf zone bars are referred to as shoreline sand waves. Many observed undulations along sandy coasts display a wavelength in the order 1-7 km. Several models that are based on the hypothesis that sand waves emerge from a morphodynamic instability in case of very oblique wave incidence predict this range of wavelengths. Here we investigate the physical reasons for the wavelength selection and the main parametric trends of the wavelength in case of sand waves arising from such instability. It is shown that the existence of a minimum wavelength depends on an interplay between three factors affecting littoral drift: (A) the angle of wave fronts relative to local shoreline, which tends to cause maximum transport at the downdrift flank of the sand wave, (B) the refractive energy spreading which tends to cause maximum transport at the updrift flank and (C) wave focusing (de-focusing) by the capes (bays), which tends to cause maximum transport at the crest or slightly downdrift of it. Processes A and C cause decay of the sand waves while process B causes their growth. For low incidence angles, B is very weak so that a rectilinear shoreline is stable. For large angles and long sand waves, B is dominant and causes the growth of sand waves. For large angles and short sand waves C is dominant and the sand waves decay. Thus, wavelength selection depends on process C, which essentially depends on shoreline curvature. The growth rate of very long sand waves is weak because the alongshore gradients in sediment transport decrease with the wavelength. This is why there is an optimum or dominant wavelength. It is found that sand wave wavelength scales with λ0/β where λ0 is the water wave wavelength in deep water and β is the mean bed slope from shore to the wave base.</itunes:summary>
    </item>
    <item>
      <title>Intertidal finger bars at El Puntal spit, bay of Santander, Spain</title>
      <link>http://hdl.handle.net/2117/18427</link>
      <description>Title: Intertidal finger bars at El Puntal spit, bay of Santander, Spain
Authors: Garnier, Roland; Medina, Raúl; Pellón, Erica; Falqués Serra, Albert; Turki, Imen
Abstract: We indentify the presence of an intertidal finger bar system in the swell-protected beaches of El Puntal Spit (Bay of Santander, Spain). The Horus video monitoring system allows us to perform a 2 year survey (June 2008- June 2010). We found that the bar system persists during the survey period with a wavelength of about 25 m and an oblique orientation with respect to the shore. Moreover, the analysis of the position of a particular bar (Bar 10) shows a&#xD;
movement characterized by a net migration to the west and a faster oscillation to the east or the west. Preliminary climate data analysis and morphological model results show that tide seems to be a forcing in the motion of the bars but also wind and waves generated by the wind probably affects the bar dynamics.</description>
      <pubDate>Tue, 19 Mar 2013 18:54:44 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18427</guid>
      <dc:date>2013-03-19T18:54:44Z</dc:date>
      <itunes:author>Garnier, Roland; Medina, Raúl; Pellón, Erica; Falqués Serra, Albert; Turki, Imen</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>We indentify the presence of an intertidal finger bar system in the swell-protected beaches of El Puntal Spit (Bay of Santander, Spain). The Horus video monitoring system allows us to perform a 2 year survey (June 2008- June 2010). We found that the bar system persists during the survey period with a wavelength of about 25 m and an oblique orientation with respect to the shore. Moreover, the analysis of the position of a particular bar (Bar 10) shows a&#xD;
movement characterized by a net migration to the west and a faster oscillation to the east or the west. Preliminary climate data analysis and morphological model results show that tide seems to be a forcing in the motion of the bars but also wind and waves generated by the wind probably affects the bar dynamics.</itunes:summary>
    </item>
    <item>
      <title>The Boundary Layer Late Afternoon and Sunset Turbulence 2011 field experiment (BLT)</title>
      <link>http://hdl.handle.net/2117/18398</link>
      <description>Title: The Boundary Layer Late Afternoon and Sunset Turbulence 2011 field experiment (BLT)
Authors: Lothon, Marie; Lohou, Fabienne; Durand, Pierre; Couvreux, Fleur; Hartogensis, Oskar; Legain, Dominique; Pardyjak, Erick; Pino González, David; Reuder, Joaquim; Vilà-Guerau de Arellano, Jordi
Abstract: Growth of the CBL over land in the middle of the&#xD;
day has been extensively observed and relatively successfully&#xD;
modeled. However the late afternoon transition&#xD;
(LAT), like the morning transition, is difficult to&#xD;
observe and model due to turbulence intermittency&#xD;
and anisotropy, horizontal heterogeneity, and rapid time&#xD;
changes. There is a striking paucity of observations of&#xD;
the turbulence decay within the CBL, as well as a lack of&#xD;
realistic modeling studies.&#xD;
This motivated the Boundary Layer Late Afternoon&#xD;
and Sunset Turbulence (BLLAST) 2011 field experiment,&#xD;
which aimed at enhancing observations of the LAT, so as&#xD;
to better understand the physical processes that control&#xD;
it, and elucidate the role of the LAT on mesoscale and&#xD;
turbulence scale motions, and on species transport.</description>
      <pubDate>Tue, 19 Mar 2013 12:02:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18398</guid>
      <dc:date>2013-03-19T12:02:00Z</dc:date>
      <itunes:author>Lothon, Marie; Lohou, Fabienne; Durand, Pierre; Couvreux, Fleur; Hartogensis, Oskar; Legain, Dominique; Pardyjak, Erick; Pino González, David; Reuder, Joaquim; Vilà-Guerau de Arellano, Jordi</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>Growth of the CBL over land in the middle of the&#xD;
day has been extensively observed and relatively successfully&#xD;
modeled. However the late afternoon transition&#xD;
(LAT), like the morning transition, is difficult to&#xD;
observe and model due to turbulence intermittency&#xD;
and anisotropy, horizontal heterogeneity, and rapid time&#xD;
changes. There is a striking paucity of observations of&#xD;
the turbulence decay within the CBL, as well as a lack of&#xD;
realistic modeling studies.&#xD;
This motivated the Boundary Layer Late Afternoon&#xD;
and Sunset Turbulence (BLLAST) 2011 field experiment,&#xD;
which aimed at enhancing observations of the LAT, so as&#xD;
to better understand the physical processes that control&#xD;
it, and elucidate the role of the LAT on mesoscale and&#xD;
turbulence scale motions, and on species transport.</itunes:summary>
    </item>
    <item>
      <title>Boundary Layer Late Afternoon and Sunset Turbulence: the BLLAST 2011 experiment</title>
      <link>http://hdl.handle.net/2117/18364</link>
      <description>Title: Boundary Layer Late Afternoon and Sunset Turbulence: the BLLAST 2011 experiment
Authors: Pino González, David; Lothon, Marie; Lohou, Fabienne; Pardyjak, Erick; Reuder, Joaquim; Legain, Dominique; Durand, Pierre; Couvreux, Fleur; Vilà-Guerau de Arellano, Jordi</description>
      <pubDate>Mon, 18 Mar 2013 11:58:13 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/18364</guid>
      <dc:date>2013-03-18T11:58:13Z</dc:date>
      <itunes:author>Pino González, David; Lothon, Marie; Lohou, Fabienne; Pardyjak, Erick; Reuder, Joaquim; Legain, Dominique; Durand, Pierre; Couvreux, Fleur; Vilà-Guerau de Arellano, Jordi</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
    </item>
    <item>
      <title>Effect of surface rollers on the formation of crescentic bars: large angles of incidence</title>
      <link>http://hdl.handle.net/2117/17890</link>
      <description>Title: Effect of surface rollers on the formation of crescentic bars: large angles of incidence
Authors: Calvete Manrique, Daniel; Ribas Prats, Francesca; Swart, Huib E. de; Falqués Serra, Albert
Abstract: The formation of crescentic bars is examined using a morphodynamic model based in linear stability analysis. The effect of surface rollers for off-normal wave conditions is examined. The effect of the rollers is to increase the e-folding times with increasing the angle of incidence. For angles large enough the formation of crescentic bars is even inhibit. The main effect of the rollers it be through hydrodynamics. The longitudinal changes in current produced by&#xD;
the rollers cause the maximum of sediment concentration to be shifted towards the coast with the final effect of prevent the formation of crecscentic bars.</description>
      <pubDate>Tue, 19 Feb 2013 18:06:15 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2117/17890</guid>
      <dc:date>2013-02-19T18:06:15Z</dc:date>
      <itunes:author>Calvete Manrique, Daniel; Ribas Prats, Francesca; Swart, Huib E. de; Falqués Serra, Albert</itunes:author>
      <itunes:explicit>no</itunes:explicit>
      <itunes:keywords />
      <itunes:summary>The formation of crescentic bars is examined using a morphodynamic model based in linear stability analysis. The effect of surface rollers for off-normal wave conditions is examined. The effect of the rollers is to increase the e-folding times with increasing the angle of incidence. For angles large enough the formation of crescentic bars is even inhibit. The main effect of the rollers it be through hydrodynamics. The longitudinal changes in current produced by&#xD;
the rollers cause the maximum of sediment concentration to be shifted towards the coast with the final effect of prevent the formation of crecscentic bars.</itunes:summary>
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